PRL - 2568

• (2025). Interdependent scaling exponents in the human brain. PRL, 135(19), 198401. (www)

  @article{ , abstract = {We apply the phenomenological renormalization group to resting-state fMRI time series of brain activity in a large population. By recursively coarse graining the data, we compute scaling exponents for the series variance, log probability of silence, and largest covariance eigenvalue. The scaling exponents clearly exhibit linear interdependencies in the form of scaling relations and inherent variability of values closely related to the structure of correlations of brain activity. The scaling relations between the exponents are derived analytically. We find a significant correlation of exponents with clinical (gray matter volume) and behavioral (cognitive performance) traits. Akin to scaling relations near critical points in thermodynamics, our results suggest that this interdependency is intrinsic to brain organization, and may also exist in other complex systems.}, archive = {J_PRL}, author = {Daniel M. Castro and Ernesto P. Raposo and Mauro Copelli and Fernando A. N. Santos}, doi = {10.1103/lvwj-hjr3}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {198401}, shortjournal = {Phys. Rev. Lett.}, title = {Interdependent scaling exponents in the human brain}, volume = {135}, year = {2025}, }
• (2025). Pure hydrodynamic instabilities in active jets of puller microalgae. PRL, 135(19), 198301. (www)

  @article{ , abstract = {Active fluids can develop spontaneous flow instabilities and complex patterns. However, spatiotemporal control of active particles has remained challenging, despite its relevance in biological and applied contexts. Here, we harnessed phototaxis to steer millions of swimming “puller” Chlamydomonas reinhardtii algae to create active jets and control both pearling and buckling instabilities through the preferential orientation of the cells. Our experiments, supported by a full analytical model and simulations, confirm long-standing predictions that self-generated flows can lead to jet destabilization. Our results further indicate that pullers can behave analogously to pushers when their orientation is properly tuned, and demonstrate how light enables the efficient control of active fluids.}, archive = {J_PRL}, author = {Isabelle Eisenmann and Marco Vona and Nicolas Desprat and Takuji Ishikawa and Eric Lauga and Raphaël Jeanneret}, doi = {10.1103/jjcv-ygvq}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {198301}, shortjournal = {Phys. Rev. Lett.}, title = {Pure hydrodynamic instabilities in active jets of puller microalgae}, volume = {135}, year = {2025}, }
• (2025). Finite-disorder critical point in the brittle-to-ductile transition of amorphous solids in the presence of particle pinning. PRL, 135(19), 198201. (www)

  @article{ , abstract = {Using particle based simulation of a model glass former, we demonstrate a transition from brittle yielding to ductile yielding in amorphous solids by introducing quenched disorder in the form of randomly pinned particles. The well-annealed samples, which exhibit brittle yielding, undergo a transition to increasingly ductile yielding with increasing pinning concentrations while exhibiting an enhanced stress overshoot. Extensive finite size analysis is performed to demonstrate the critical nature of the transition at a finite pinning concentration and the various scaling exponents obtained are found to be in good agreement with the reported values for the random field Ising model universality class. Finally, we establish a connection between inherent disorder strength of amorphous solids that controls the nature of the yielding and quenched disorder strength due to particle pinning.}, archive = {J_PRL}, author = {Anoop Mutneja and Bhanu Prasad Bhowmik and Smarajit Karmakar}, doi = {10.1103/nvkn-tmwq}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {198201}, shortjournal = {Phys. Rev. Lett.}, title = {Finite-disorder critical point in the brittle-to-ductile transition of amorphous solids in the presence of particle pinning}, volume = {135}, year = {2025}, }
• (2025). Clustering does not always imply latent geometry. PRL, 135(19), 197402. (www)

  @article{ , abstract = {The latent space approach to complex networks has revealed fundamental principles and symmetries, enabling geometric methods. However, the conditions under which network topology implies geometricity remain unclear. We provide a mathematical proof and empirical evidence showing that multiscale self-similarity in complex networks is a crucial factor of latent geometry. Using degree-thresholding renormalization, we prove that a general class of ensembles of random scale-free networks in Riemannian manifolds of constant curvature and of any dimension are self-similar when interactions are pairwise. Hence, both nonvanishing local clustering in the thermodynamic limit and self-similarity are required to imply geometricity. Our findings highlight that correlated links can lead to a finite clustering coefficient without self-similarity, and therefore without inherent latent geometry. The implications are significant for network mapping and ensemble equivalence between graphs and continuous spaces.}, archive = {J_PRL}, author = {Roya Aliakbarisani and Marián Boguñá and M. Ángeles Serrano}, doi = {10.1103/ycwq-92ms}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {197402}, shortjournal = {Phys. Rev. Lett.}, title = {Clustering does not always imply latent geometry}, volume = {135}, year = {2025}, }
• (2025). Interpretable disorder-promoted synchronization and coherence in coupled laser networks. PRL, 135(19), 197401. (www)

  @article{ , abstract = {Coupled lasers offer a promising approach to scaling the power output of photonic devices for applications demanding high frequency precision and beam coherence. However, maintaining coherence among lasers remains a fundamental challenge due to desynchronizing instabilities arising from time delay in the optical coupling. Here, we depart from the conventional notion that disorder is detrimental to synchronization and instead propose an interpretable mechanism through which heterogeneity in the laser parameters can be harnessed to promote synchronization. Our approach allows for stabilization of prespecified synchronous states that, while abundant, are often unstable in systems of identical lasers. The results show that stable synchronization enabling coherence can be frequently achieved by introducing intermediate levels of random mismatches in any of several laser constructive parameters. Our results establish a principled framework for enhancing coherence in large laser networks, offering a robust strategy for power scaling in photonic systems.}, archive = {J_PRL}, author = {Ana Elisa D. Barioni and Arthur N. Montanari and Adilson E. Motter}, doi = {10.1103/8qvk-hpwb}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {197401}, shortjournal = {Phys. Rev. Lett.}, title = {Interpretable disorder-promoted synchronization and coherence in coupled laser networks}, volume = {135}, year = {2025}, }
• (2025). Gapless single-spin qubit. PRL, 135(19), 197001. (www)

  @article{ , abstract = {All-electrical baseband control of qubits facilitates scaling up quantum processors by removing issues of crosstalk and heat generation. In semiconductor quantum dots, this is enabled by multispin qubit encodings, such as the exchange-only qubit. However, their performance is limited by unavoidable leakage states that are energetically close to the computational subspace. In this Letter, we introduce an alternative, scalable spin qubit architecture that leverages strong spin-orbit interactions of hole nanostructures for baseband qubit operations while completely eliminating leakage channels and reducing the overall gate overhead. This encoding is intrinsically robust to local variability in hole spin properties and operates with two degenerate states, removing the need for precise calibration and mitigating heat generation from fast signal sources. Finally, our architecture is fully compatible with current technology, utilizing the same initialization, readout, and multiqubit protocols of state-of-the-art spin- systems. By addressing critical scalability challenges, our design offers a robust and scalable pathway for semiconductor spin qubit technologies.}, archive = {J_PRL}, author = {Maximilian Rimbach-Russ and Valentin John and Barnaby van Straaten and Stefano Bosco}, doi = {10.1103/mvtj-zhrl}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {197001}, shortjournal = {Phys. Rev. Lett.}, title = {Gapless single-spin qubit}, volume = {135}, year = {2025}, }
• (2025). Zero-point motion of polar optical phonons revealed by up-converted photoluminescence from a single perovskite nanocrystal at cryogenic temperatures. PRL, 135(19), 196901. (www)

  @article{ , abstract = {Quantum mechanics suggests a persistent lattice vibration even at zero temperature; however, this elusive zero-point motion is difficult to measure for further analyses and exploitations. Here, we have performed near-resonant excitations on single perovskite CsPbI 3 nanocrystals (NCs) at cryogenic temperatures, showing that pronounced up-converted photoluminescence (UC-PL) still takes place even at ∼ 4 K despite the vanishing phonon-assisted absorption. This surprising result can be explained in terms of a dynamic electric field caused by the zero-point motion of polar optical phonons, which gives rise to an absorption tail as in the Franz-Keldysh electroabsorption process. Furthermore, laser cooling is demonstrated in the ∼ 4 K UC-PL process of a single CsPbI 3 NC, which opens a novel research avenue for the realization of even lower temperatures beyond the limit set forth by the helium-based cryostat.}, archive = {J_PRL}, author = {Rentong Duan and Fengrui Hu and Chunyang Yin and Yan Lv and Chunfeng Zhang and Min Xiao and Zhi-Gang Yu and Xiaoyong Wang}, doi = {10.1103/gp1z-fbl6}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196901}, shortjournal = {Phys. Rev. Lett.}, title = {Zero-point motion of polar optical phonons revealed by up-converted photoluminescence from a single perovskite nanocrystal at cryogenic temperatures}, volume = {135}, year = {2025}, }
• (2025). Spin-disorder-induced angular anisotropy in polarized magnetic neutron scattering. PRL, 135(19), 196706. (www)

  @article{ , abstract = {We experimentally report a hitherto unseen angular anisotropy in the polarized small-angle neutron scattering (SANS) cross section of a magnetically strongly inhomogeneous material. Based on an analytical prediction using micromagnetic theory, the difference between the spin-up and spin-down SANS cross sections is expected to show a spin-disorder-induced anisotropy. The effect is particularly pronounced in inhomogeneous magnetic materials, such as nanoporous ferromagnets, magnetic nanocomposites, or steels, which exhibit large nanoscale jumps in the saturation magnetization at internal pore-matrix or particle-matrix interfaces. Analysis of the experimental neutron data constitutes a method for determining the exchange-stiffness constant. Our results for the nuclear-magnetic interference terms contained in the polarized magnetic neutron scattering cross section might also be of relevance to other neutron techniques.}, archive = {J_PRL}, author = {Ivan Titov and Mathias Bersweiler and Michael P. Adams and Evelyn Pratami Sinaga and Venus Rai and Štefan Liščák and Max Lahr and Thomas L. Schmidt and Vladyslav M. Kuchkin and Andreas Haller and Kiyonori Suzuki and Nina-Juliane Steinke and Diego Alba Venero and Dirk Honecker and Joachim Kohlbrecher and Luis Fernández Barquín and Andreas Michels}, doi = {10.1103/5yc2-pv4y}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196706}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-disorder-induced angular anisotropy in polarized magnetic neutron scattering}, volume = {135}, year = {2025}, }
• (2025). Predictive indicator of critical point in equilibrium and nonequilibrium magnetic systems. PRL, 135(19), 196705. (www)

  @article{ , abstract = {Determining critical points of phase transitions from partial data is essential to avoid abrupt system collapses and to reduce experimental or computational costs. However, the complex physical systems and phase transition phenomena have long hindered the development of unified approaches applicable to both equilibrium and nonequilibrium phase transitions. In this Letter, we propose predictive indicators to determine critical points in equilibrium and nonequilibrium magnetic systems based on the frequency-dependent response function. For equilibrium phase transitions, such as magnetization switching under a magnetic field, the static magnetization response function to a perturbing magnetic field diverges at the critical field, serving as a noise-resilient predictive indicator that also reflects the transition order and critical exponents. In contrast, for nonequilibrium phase transitions such as magnetization switching driven by transfer torque, static response fails to signal criticality. Instead, the dynamic response at ferromagnetic resonance frequency diverges at the critical point, which is also robust against thermal noise. We further demonstrate that these static and dynamic indicators can be unified in the frame of first-order linear differential systems, offering a generalizable strategy for predicting criticality in both equilibrium and nonequilibrium transitions.}, archive = {J_PRL}, author = {Tianyi Zhang and Caihua Wan and Xiufeng Han}, doi = {10.1103/81nz-k6tb}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196705}, shortjournal = {Phys. Rev. Lett.}, title = {Predictive indicator of critical point in equilibrium and nonequilibrium magnetic systems}, volume = {135}, year = {2025}, }
• (2025). Spin-torque-driven subterahertz antiferromagnetic resonance dynamics. PRL, 135(19), 196704. (www)

  @article{ , abstract = {Spin torque antiferromagnetic resonance (ST-AFMR) is fundamental to high-frequency spintronic devices, such as ultrafast magnetic storage and terahertz spin nano-oscillators. However, limited by generating terahertz spin torques, it has been confined to the gigahertz in-plane linearly polarized low-frequency mode of easy-plane antiferromagnets. Here we employ optical terahertz pulses as high-frequency excitation sources and time-resolved Faraday effect as detection to investigate ST-AFMR of the out-of-plane linearly polarized high-frequency mode in bilayers. We observe ST-AFMR at a sub-terahertz frequency of 280 GHz, with fieldlike spin-orbit torque as the dominant mechanism. The net magnetization revealed by Faraday detection exhibits only in-plane oscillation, consistent with the high-frequency mode of easy-plane antiferromagnets. Moreover, the film thickness-dependent frequency indicates an inherent origin of the high frequency rather than standing waves. The ST-AFMR frequency also demonstrates high stability against external magnetic fields, which can be attributed to the absence of precession in the mode. Our findings open new avenues for ultrafast applications of antiferromagnetic-based devices.}, archive = {J_PRL}, author = {Yichen Su and Chunyan Geng and Deyin Kong and Lei Han and Lin Huang and Feng Pan and Fei Dai and Xiaojun Wu and Cheng Song}, doi = {10.1103/l8d1-gpgr}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196704}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-torque-driven subterahertz antiferromagnetic resonance dynamics}, volume = {135}, year = {2025}, }
• (2025). Circular dichroism in resonant photoelectron diffraction as a direct probe of sublattice magnetization in altermagnets. PRL, 135(19), 196703. (www)

  @article{ , abstract = {Altermagnets are a new class of magnetic materials that are promising for spintronics technology. Here, it is shown that in altermagnets, the circular dichroism (CD) in resonant photoelectron diffraction (RPED) contains a time-reversal odd signal, which provides a direct probe of the sublattice magnetization. RPED calculations are performed for MnTe at the Mn L 2 , 3 -edge resonance, using a combination of atomic multiplet and multiple scattering theory. A large magnetic CD is found for light helicity parallel to the Néel vector. This signal has the same angular distribution as the difference between the structural RPED of the two magnetic sublattices and its amplitude is approximately proportional to the x-ray magnetic CD in absorption of a single sublattice, thus providing a direct probe of the local magnetic moments.}, archive = {J_PRL}, author = {Peter Krüger}, doi = {10.1103/pl1p-v5rs}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196703}, shortjournal = {Phys. Rev. Lett.}, title = {Circular dichroism in resonant photoelectron diffraction as a direct probe of sublattice magnetization in altermagnets}, volume = {135}, year = {2025}, }
• (2025). Topological magneto-optics in the noncoplanar antiferromagnet Co1/3NbS2: Imaging and writing chiral magnetic domains. PRL, 135(19), 196702. (www)

  @article{ , abstract = {Despite its tiny net magnetization, the antiferromagnetic (AFM) van der Waals material Co 1 / 3 NbS 2 exhibits a large transverse Hall conductivity σ x y even at zero applied magnetic field, which arises, as recently shown, from the topological nature of its noncoplanar “tetrahedral” AFM order. This triple- q magnetic order can be regarded as the short-length-scale limit of a magnetic skyrmion lattice and has an intrinsic spin chirality. Here, we show, using optical wavelengths spanning the ultraviolet to infrared (400–1000 nm), that magnetic circular dichroism provides an incisive optical probe of the topological AFM order in Co 1 / 3 NbS 2 . Measurements as a continuous function of photon energy are directly compared with first-principles calculations, revealing the influence of the underlying quantum geometry on optical conductivity. Leveraging the power and flexibility of optical methods, we use scanning magnetic circular dichroism microscopy to directly image chiral AFM domains and demonstrate writing of chiral AFM domains.}, archive = {J_PRL}, author = {E. Kirstein and H. Park and I. Martin and J. F. Mitchell and N. J. Ghimire and S. A. Crooker}, doi = {10.1103/wh5t-12fn}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196702}, shortjournal = {Phys. Rev. Lett.}, title = {Topological magneto-optics in the noncoplanar antiferromagnet Co1/3NbS2: Imaging and writing chiral magnetic domains}, volume = {135}, year = {2025}, }
• (2025). Moiré-induced magnetoelectricity in twisted bilayer NiI2. PRL, 135(19), 196701. (www)

  @article{ , abstract = {Twisted magnetic van der Waals materials offer a promising route for multiferroic engineering, yet modeling large-scale moiré superlattices remains challenging. Leveraging a newly developed SpinGNN++ framework that effectively handles spin-lattice coupled systems, we develop a comprehensive interatomic machine learning potential and apply it to twisted bilayer . Structural relaxation introduces moiré-periodic “bumps” that modulate the interlayer spacing by about 0.55 Å and in-plane ionic shifts up to 0.48 Å. Concurrently, our machine learning potential, which faithfully captures all key spin interactions, produces reliable magnetic configurations; combined with the more accurate generalized Katsura-Nagaosa-Balatsky mechanism, it delivers precise spin-driven polarization. For twist angles , both mechanisms become prominent, yielding rich polarization textures that combine ionic out-of-plane dipoles with purely electronic in-plane domains. In the rigid (unrelaxed) bilayer, skyrmions are absent; lattice relaxation is thus essential for generating polar-magnetic topologies. In contrast, near , stacking-dependent ferroelectric displacements dominate, giving rise to polar meron-antimeron networks. These results reveal cooperative ionic and spin-driven ferroelectricity in twisted bilayer , positioning twisted van der Waals magnets as adaptable platforms for tunable multiferroic devices.}, archive = {J_PRL}, author = {Haiyan Zhu and Hongyu Yu and Weiqin Zhu and Guoliang Yu and Changsong Xu and Hongjun Xiang}, doi = {10.1103/p6n8-n1rx}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196701}, shortjournal = {Phys. Rev. Lett.}, title = {Moiré-induced magnetoelectricity in twisted bilayer NiI2}, volume = {135}, year = {2025}, }
• (2025). Multiphoton spectroscopy of a dynamical axion insulator. PRL, 135(19), 196601. (www)

  @article{ , abstract = {The unusual magnetoelectric transport present in Weyl semimetals and 3D topological insula- tors can be compactly understood as manifestations of a background axion field, which itself is determined by the microscopic band structure. In the presence of correlations, an additional axion quasiparticle may emerge as the collective excitations on top of the mean background field. Such modes couple nonlinearly to electric and magnetic fields, giving rise to a dynamical magnetoelectric response. However, unambiguous identification of this collective axion mode is challenging due to its inherent nonlinear dynamics. Here, we propose an all-optical protocol that utilizes a pump-probe setup for verifying and characterizing the transient dynamics of axion fields in three-dimensional insulator systems. In particular, we show that nonlinear Raman processes induce dynamical oscillations of the axion field that depend on the geometry of the incident electromagnetic fields. These oscillations manifest in the polarization and magnetization of the material, hence, can be subsequently measured using time-resolved Kerr rotation spectroscopy. Our results open a pathway toward using multiphoton and quantum pair spectroscopies to identify new correlated phases of quantum matter.}, archive = {J_PRL}, author = {Olivia Liebman and Jonathan B. Curtis and Ioannis Petrides and Prineha Narang}, doi = {10.1103/3zkg-95b3}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196601}, shortjournal = {Phys. Rev. Lett.}, title = {Multiphoton spectroscopy of a dynamical axion insulator}, volume = {135}, year = {2025}, }
• (2025). Orbital magnetic field driven metal-insulator transition in strongly correlated electron systems. PRL, 135(19), 196503. (www)

  @article{ , abstract = {We study the effects of an orbital magnetic field on the Mott metal-insulator transition in the Hubbard-Hofstadter model. We demonstrate that sufficiently large magnetic fields induce a Mott insulator-to-metal phase transition supporting our claim with dynamical mean field theory (DMFT) numerical results. For both competing phases (metal and insulator) we observe a magnetic-field-induced metallization reflected in an enhancement of kinetic and potential energy. The kinetic energy of the Mott insulator increases due to the Aharonov-Bohm effect experienced by electrons virtually tunneling around an elementary plaquette which is, however, suppressed by strong correlations. The kinetic energy of the metallic phase, on the other hand, is more strongly affected by the magnetic field through a field-driven redistribution of spectral weight due to the formation of magnetic minibands. This leads to an increase of the kinetic energy which tends to stabilize the metallic state. Our theoretical results might be relevant for recent experimental studies on magnetic field driven insulator-to-metal transitions in strongly correlated materials such as , -type organic conductors, and moiré multilayers.}, archive = {J_PRL}, author = {Georg Rohringer and Anton Markov}, doi = {10.1103/bw7f-p8mp}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196503}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital magnetic field driven metal-insulator transition in strongly correlated electron systems}, volume = {135}, year = {2025}, }
• (2025). Circular dichroism in resonant inelastic X-ray scattering: Probing altermagnetic domains in MnTe. PRL, 135(19), 196502. (www)

  @article{ , abstract = {X-ray magnetic circular dichroism provides a means to identify ferromagnetic, chiral, and altermagnetic orders via their time-reversal-symmetry ( T ) breaking. However, the symmetry properties that govern circular dichroism (CD) in resonant inelastic x-ray scattering (RIXS) remain poorly understood. We show that, due to the inherent irreversibility of the RIXS process, RIXS-CD does not require T breaking to be present, but reflects the change in unitary symmetries associated with magnetic ordering. Using the altermagnetic MnTe as a model system, we observe an azimuthal-angle dependent RIXS-CD signal in the magnon excitations. Our findings highlight the sensitivity of RIXS-CD to the relativistic symmetry in magnetic systems and its potential application as a probe of magnetic domains.}, archive = {J_PRL}, author = {D. Takegami and T. Aoyama and T. Okauchi and T. Yamaguchi and S. Tippireddy and S. Agrestini and M. García-Fernández and T. Mizokawa and K. Ohgushi and Ke-Jin Zhou and J. Chaloupka and J. Kuneš and A. Hariki and H. Suzuki}, doi = {10.1103/512v-n5f9}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196502}, shortjournal = {Phys. Rev. Lett.}, title = {Circular dichroism in resonant inelastic X-ray scattering: Probing altermagnetic domains in MnTe}, volume = {135}, year = {2025}, }
• (2025). Chiral graviton modes on the lattice. PRL, 135(19), 196501. (www)

  @article{ , abstract = {Chiral graviton modes are elusive excitations arising from the hidden quantum geometry of fractional quantum Hall states. It remains unclear, however, whether this picture extends to lattice models, where continuum translations are broken and additional quasiparticle decay channels arise. We present a framework in which we explicitly derive a field theory incorporating lattice chiral graviton operators within the paradigmatic bosonic Harper-Hofstadter model. Extensive numerical evidence suggests that chiral graviton modes persist away from the continuum and are well captured by the proposed lattice operators. We identify geometric quenches as a viable experimental probe, paving the way for the exploration of chiral graviton modes in near-term quantum simulation experiments.}, archive = {J_PRL}, author = {Hernan B. Xavier and Zeno Bacciconi and Titas Chanda and Dam Thanh Son and Marcello Dalmonte}, doi = {10.1103/1636-kl65}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196501}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral graviton modes on the lattice}, volume = {135}, year = {2025}, }
• (2025). Anomalous nodal gap in a doped spin-1/2 antiferromagnetic mott insulator. PRL, 135(19), 196403. (www)

  @article{ , abstract = {Many emergent phenomena appear in doped Mott insulators near the insulator-to-metal transition. In high-temperature cuprate superconductors, superconductivity arises when antiferromagnetic (AFM) order is gradually suppressed by carrier doping, and a -wave superconducting gap forms when an enigmatic nodal gap evolves into a point node. Here, we examine electron-doped , the -electron counterpart of cuprates, using angle-resolved photoemission spectroscopy. At low doping levels, we observe the formation of electronic states near the Fermi level, accompanied by a gap at the AFM zone boundary, mimicking the AFM gap in electron-doped cuprates. With increasing doping, a distinct gap emerges along the nodal direction, paralleling that observed in hole-doped cuprates. This anomalous nodal gap persists after the collapse of the AFM gap and gradually decreases with further doping. It eventually vanishes into a point node of the reported -wave gap. These observations replicate the characteristic features in both electron- and hole-doped cuprates, indicating a unified route toward nodal metallicity in doped spin- AFM Mott insulators.}, archive = {J_PRL}, author = {Yong Hu and Christopher Lane and Xiang Chen and Shuting Peng and Zeliang Sun and Makoto Hashimoto and Donghui Lu and Tao Wu and Robert S. Markiewicz and Xianhui Chen and Arun Bansil and Stephen D. Wilson and Junfeng He}, doi = {10.1103/3rw4-mhz8}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196403}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous nodal gap in a doped spin-1/2 antiferromagnetic mott insulator}, volume = {135}, year = {2025}, }
• (2025). Moiré band theory for M-valley twisted transition metal dichalcogenides. PRL, 135(19), 196402. (www)

  @article{ , abstract = {We propose twisted bilayers of certain group IV and IVB trigonal transition metal dichalcogenides (TMDs) ( , Hf, Sn and , Se) as moiré materials. In monolayer form, these TMDs have conduction band minima near the three inequivalent Brillouin zone points and negligible spin-orbit coupling, implying six flavors of low-energy conduction band states. The flavor sectors decouple at the single-particle level and in twisted bilayers are accurately described by emergent moiré-periodic Hamiltonians that we derive from small-unit-cell density functional theory calculations. Because the valley-projected Hamiltonians have large valley-dependent mass anisotropies and are time-reversal invariant, spontaneous valley polarization is signaled in transport by anisotropy instead of by the anomalous Hall and magnetic circular dichroism signals commonly observed in graphene and -valley TMD-based moiré multilayers.}, archive = {J_PRL}, author = {Chao Lei and Perry T. Mahon and A. H. MacDonald}, doi = {10.1103/5zt2-scbg}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196402}, shortjournal = {Phys. Rev. Lett.}, title = {Moiré band theory for M-valley twisted transition metal dichalcogenides}, volume = {135}, year = {2025}, }
• (2025). General first-principles approach to crystals in finite magnetic fields. PRL, 135(19), 196401. (www)

  @article{ , abstract = {We introduce a general first-principles methodology for computing electronic structure in a finite uniform magnetic field that allows for an arbitrary rational magnetic flux and nonlocal pseudopotentials at a comparable time complexity to conventional plane-wave pseudopotential approaches in zero-field conditions. The versatility of this method is demonstrated through comprehensive applications to both molecular and crystalline systems, including calculations of magnetizabilities, magnetically induced currents, and magnetic energy bands. Furthermore, we provide rigorous proofs of two properties for crystals in uniform magnetic fields: the “strong translational symmetry” and “magnetic band shift” phenomena.}, archive = {J_PRL}, author = {Chengye Lü and Yingwei Chen and Yuzhi Wang and Zhihao Dai and Zhong Fang and Xin-Gao Gong and Quansheng Wu and Hongjun Xiang}, doi = {10.1103/74bb-qmp8}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196401}, shortjournal = {Phys. Rev. Lett.}, title = {General first-principles approach to crystals in finite magnetic fields}, volume = {135}, year = {2025}, }
• (2025). Discovery of universal phonon thermal hall effect in crystals. PRL, 135(19), 196302. (www)

  @article{ , abstract = {Thermal Hall effect (THE) in insulators is a remarkable phenomenon that arises from the motion of chargeless quasiparticles under a magnetic field. While magnons or various exotic excitations were considered as the origin of THE in some magnetic materials, there is more and more evidence suggesting that phonons play a significant role. However, the mechanism behind phonon THE is still unknown. Here we report the observation of THE, including planar THE, in a broad range of nonmagnetic insulators and semiconductors: , (quartz), MgO, Si, and Ge. While the presence of antiferrodistortive domains in and chiral structure in may complicate the interpretation of THE, the striking observations of THE in trivial insulators MgO and , as well as in high-purity intrinsic semiconductors Si and Ge, demonstrate that phonon THE is a universal property of crystals. Without other effects on phonons such as from magnons, this universal phonon THE is characterized by a scaling behavior of . Our results experimentally discover a fundamental physics of phonons in the magnetic field, which should come from the direct coupling between atom vibrations and the field. Starting from this universal phonon THE in crystals, previous interpretations of THE in magnetic or nonmagnetic materials need to be reconsidered.}, archive = {J_PRL}, author = {X. B. Jin and X. Zhang and W. B. Wan and H. R. Wang and Y. H. Jiao and S. Y. Li}, doi = {10.1103/r572-5dfm}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196302}, shortjournal = {Phys. Rev. Lett.}, title = {Discovery of universal phonon thermal hall effect in crystals}, volume = {135}, year = {2025}, }
• (2025). Orientation-dependent ionic-current rectification in colloidal crystals. PRL, 135(19), 196301. (www)

  @article{ , abstract = {Nonreciprocal transport (current rectification) in bulk materials is rarer and more complex than at interfaces. We theoretically demonstrate ion current rectification in binary superlattices of oppositely charged nanoparticles and show that this effect strongly depends on the direction of the applied electric field. We derive an equation that relates the symmetry elements of the superlattice to the directions where rectification is forbidden. This equation is used to analyze the conductivity of different superlattices obtained from the numerical solution of the Poisson-Nernst-Planck equations.}, archive = {J_PRL}, author = {Santiago F. Bonoli and Leandro L. Missoni and Yamila A. Perez Sirkin and Mario Tagliazucchi}, doi = {10.1103/rlp5-v889}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196301}, shortjournal = {Phys. Rev. Lett.}, title = {Orientation-dependent ionic-current rectification in colloidal crystals}, volume = {135}, year = {2025}, }
• (2025). Josephson junction tuning described by depinning physics. PRL, 135(19), 196202. (www)

  @article{ , abstract = {Superconducting quantum computers leverage superconducting qubits, systems with well-defined energy levels, the spacing of which is determined by the properties of embedded Josephson junctions. Indeterminacy of Josephson junction manufacturing limits large-scale superconducting circuits; however, junction-by-junction tuning affords the possibility of an order of magnitude improvement of determinacy—although the origin of this tuning effect is uncertain. Understanding how tuning techniques may physically modify the tunnel barrier of a Josephson junction is important and will enable these techniques to be optimized. We develop a model of junction tuning based on depinning theory to interpret a phase diagram of the tuning rate. We extract the dependence on temperature, time-varying voltages, and oscillation frequency. Comparing the effect of junction tuning on room-temperature I − V ’s, electrical breakdown, and frequency of higher-energy levels of transmon qubits indicates that the tuning process leaves the barrier thickness unchanged but modifies its composition.}, archive = {J_PRL}, author = {Oscar W. Kennedy and Jared H. Cole and Connor D. Shelly}, doi = {10.1103/xkqs-grnd}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196202}, shortjournal = {Phys. Rev. Lett.}, title = {Josephson junction tuning described by depinning physics}, volume = {135}, year = {2025}, }
• (2025). Ab initio electron-phonon-coupling theory of elastic helium-atom scattering. PRL, 135(19), 196201. (www)

  @article{ , abstract = {We propose a fully ab initio approach to predicting thermal attenuation in elastic helium atom scattering amplitudes, validated through strong agreement with experiments on Nb(100) and surfaces. Our results reveal the relative contributions from bulk, resonant, and surface phonon modes, as well as from different surface mode polarizations, providing insights into differences between smooth and corrugated surfaces. These findings advance understanding of surface dynamics and electron-phonon coupling, laying groundwork for future studies on surface superconductivity.}, archive = {J_PRL}, author = {Cristóbal Méndez and C. J. Thompson and M. F. Van Duinen and S. J. Sibener and Tomás A. Arias}, doi = {10.1103/mcgg-8hk8}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196201}, shortjournal = {Phys. Rev. Lett.}, title = {Ab initio electron-phonon-coupling theory of elastic helium-atom scattering}, volume = {135}, year = {2025}, }
• (2025). Gyromorphs: A new class of functional disordered materials. PRL, 135(19), 196101. (www)

  @article{ , abstract = {We introduce a new class of functional correlated disordered materials, termed gyromorphs, which uniquely combine liquidlike translational disorder with quasi-long-range rotational order, induced by a ring of delta peaks in their structure factor. We generate gyromorphs in 2D and 3D by spectral optimization methods, verifying that they display strong discrete rotational order but no long-range translational order, while maintaining rotational isotropy at short range for sufficiently large . Using a coupled dipoles approximation, we numerically show that these structures outperform quasicrystals, stealthy hyperuniformity, and Vogel spirals in the formation of low-index-contrast isotropic band gaps in 2D, for both scalar and vector waves, and open complete isotropic band gaps in 3D. This claim is further supported by analytical effective-medium theory and by numerical estimates of scattering mean-free paths. Finally, we introduce “polygyromorphs” with several rotational symmetries at different length scales (i.e., multiple rings of delta peaks), enabling the formation of multiple band gaps in a single structure, thereby paving the way for fine control over optical properties.}, archive = {J_PRL}, author = {Mathias Casiulis and Aaron Shih and Stefano Martiniani}, doi = {10.1103/gqrx-7mn2}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {196101}, shortjournal = {Phys. Rev. Lett.}, title = {Gyromorphs: A new class of functional disordered materials}, volume = {135}, year = {2025}, }
• (2025). Dynamics of fractal ice grains in cryogenic plasmas. PRL, 135(19), 195301. (www)

  @article{ , abstract = {Ice grains formed in a cryogenically cooled plasma exhibit fractal morphologies that drive distinct collective dynamics. By measuring and quantifying the dynamics of these grains in a plasma afterglow, we observe a new fundamental dynamical regime induced by fractal scalings of ice mass and collisional cross section. In this regime, grains become more coupled to flows of gas and ions as they get larger, while the influence of gravity remains comparatively small, even as the grains reach millimeter sizes. These dynamics are unattainable by compact spheres, and thus inaccessible to dusty plasma models that assume spherical grains, challenging models for systems ranging from laboratory nanoparticle synthesis to astrophysical dust transport.}, archive = {J_PRL}, author = {André Nicolov and Seth Pree and Paul M. Bellan}, doi = {10.1103/rx5l-k7f9}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {195301}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamics of fractal ice grains in cryogenic plasmas}, volume = {135}, year = {2025}, }
• (2025). Proposal to use laser-accelerated electrons to probe the axion-electron coupling. PRL, 135(19), 195003. (www)

  @article{ , abstract = {The axion is a hypothetical particle associated with a possible solution to the strong CP problem and is a leading candidate for dark matter. In this Letter we investigate the emission of axions by accelerated electrons. We find the emission probability and energy within the WKB approximation for an electron accelerated by an electromagnetic field. As an application, we estimate the number of axions produced by electrons accelerated using two counterpropagating high-intensity lasers and discuss how they would be converted to photons to be detected. We find that, under realistic experimental conditions, competitive model-independent bounds on the coupling between the axion and the electron could be achieved in such an experiment.}, archive = {J_PRL}, author = {Georgios Vacalis and Atsushi Higuchi and Robert Bingham and Gianluca Gregori}, doi = {10.1103/vgvg-hcbr}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {195003}, shortjournal = {Phys. Rev. Lett.}, title = {Proposal to use laser-accelerated electrons to probe the axion-electron coupling}, volume = {135}, year = {2025}, }
• (2025). Beam realignment with emittance preservation in a plasma wakefield-accelerator stage. PRL, 135(19), 195002. (www)

  @article{ , abstract = {Plasma-based acceleration linear collider designs consist of many plasma stages where a drive beam drives a wake that accelerates a witness beam. Misalignment between the drive and witness beams can lead to the hosing instability, large emittance growth, and difficulty colliding beams at the final focus. The extreme charge and small spot size of a linear collider class electron beam causes the plasma ions to collapse within their transit time, leading to nonlinear focusing forces. It is shown that drive-beam-induced ion motion can be used to eliminate witness beam hosing and realign it with the drive beam. Fully self-consistent qpad simulations of an initial plasma stage with quasiadiabatic plasma density ramps at the entrance and exit show it is possible to simultaneously match the witness beam in the presence of ion motion while eliminating its centroid offset, at the expense of ∼ 4 % emittance growth. The energy spread growth is limited to < 1 % and the energy transfer efficiency is 50%.}, archive = {J_PRL}, author = {Lance Hildebrand and Yujian Zhao and Weiming An and Fei Li and Qianqian Su and Xinlu Xu and Chan Joshi and Warren B. Mori}, doi = {10.1103/cy5x-b81v}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {195002}, shortjournal = {Phys. Rev. Lett.}, title = {Beam realignment with emittance preservation in a plasma wakefield-accelerator stage}, volume = {135}, year = {2025}, }
• (2025). Laser-modulation-driven X-ray pulse shaping in regenerative amplifier free-electron lasers. PRL, 135(19), 195001. (www)

  @article{ , abstract = {In this Letter, we present a robust method for generating custom-shaped, coherent hard x-ray pulses in regenerative amplifier free-electron lasers (RAFELs) using laser-induced energy modulation of the electron beam. A temporally shaped optical modulation imprints an optical-wavelength energy pattern on the beam, which interacts with the recirculated seed in the x-ray cavity to generate spectral sidebands. These sidebands lie outside the Bragg reflection bandwidth and are extracted as out-coupled radiation, while the seed is retained for continued amplification, enabling a novel mechanism for both output coupling and pulse shaping. This approach allows deterministic control over the spectral and temporal properties of the emitted x-rays, including multicolor generation, twin-pulse structures, pulse duration tuning, and complex temporal waveforms. Importantly, it does not require modification of the RAFEL cavity or optics and is fully compatible with high-repetition-rate operation, offering a practical pathway to deliver coherent, shaped, and on-demand x-ray pulses for advanced time-resolved and nonlinear x-ray science.}, archive = {J_PRL}, author = {Zhen Zhang and Jingyi Tang and Erik Hemsing and Zhirong Huang}, doi = {10.1103/8lml-cckn}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {195001}, shortjournal = {Phys. Rev. Lett.}, title = {Laser-modulation-driven X-ray pulse shaping in regenerative amplifier free-electron lasers}, volume = {135}, year = {2025}, }
• (2025). Why and when merging surface nanobubbles jump. PRL, 135(19), 194001. (www)

  @article{ , abstract = {Gas bubble accumulation on substrates reduces the efficiency of many physicochemical processes, such as water electrolysis. For microbubbles, where buoyancy is negligible, coalescence-induced jumping driven by the release of surface energy provides an efficient pathway for their early detachment. At the nanoscale, however, gas compressibility breaks volume conservation during coalescence, suppressing surface energy release and seemingly disabling this detachment route. Using molecular dynamics simulations, continuum numerical simulations, and theoretical analysis, we show that surface nanobubbles with sufficiently large contact angles can nevertheless detach after coalescence. In this regime, detachment is powered by the release of pressure energy associated with nanobubble volume expansion. This finding thus establishes a unified driving mechanism for coalescence-induced bubble detachment across all length scales.}, archive = {J_PRL}, author = {Yixin Zhang and Xiangyu Zhang and Detlef Lohse}, doi = {10.1103/s5pj-vmq8}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {194001}, shortjournal = {Phys. Rev. Lett.}, title = {Why and when merging surface nanobubbles jump}, volume = {135}, year = {2025}, }
• (2025). Phase-space nonseparability, partial coherence, and optical beam shifts. PRL, 135(19), 193801. (www)

  @article{ , abstract = {As a paraxial wave packet is reflected or refracted from a planar interface separating two material media, it experiences spatial and angular shifts of its center position with respect to predictions of the geometrical ray picture. These in-plane and out-of-plane beam shifts are known as Goos-Hänchen and Imbert-Fedorov shifts, respectively. We discover a universal link between the phase-space nonseparability of an incident wave packet of any degree of spatial coherence and the reflected beam shifts. We unveil coherence Goos-Hänchen and coherence Hall effects, absent in the fully coherent limit. While the former effect can trigger a pronounced enhancement of the spatial Goos-Hänchen shift, the latter enables control of the spatial Imbert-Fedorov shift, from complete cancellation at a certain incidence angle to dramatic enhancement of the shift to giant magnitudes for nearly incoherent incident wave packets. Our results are equally applicable to optical, x-ray, and neutron, as well as matter waves, and they showcase novel phenomena in wave-matter interactions.}, archive = {J_PRL}, author = {Yahong Chen and Sergey A. Ponomarenko}, doi = {10.1103/cnvj-6w6f}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {193801}, shortjournal = {Phys. Rev. Lett.}, title = {Phase-space nonseparability, partial coherence, and optical beam shifts}, volume = {135}, year = {2025}, }
• (2025). Breaking a superfluid harmonic dam: Observation and theory of riemann invariants and accelerating sonic horizons. PRL, 135(19), 193402. (www)

  @article{ , abstract = {An experimental and theoretical study of sonic horizons emerging from the dam-break problem in a Bose-Einstein condensate confined in an anisotropic harmonic trap is presented. Measurements, analysis, and numerics reveal the formation of a sonic horizon that undergoes acceleration due to harmonic confinement. The superfluid is characterized using a robust measurement technique to determine Riemann invariants. Experimental observations agree with an analytical solution of the Gross-Pitaevskii equation and computations. The collision and annihilation between two sonic horizons at long times is predicted.}, archive = {J_PRL}, author = {Shashwat Sharan and Judith Gonzalez Sorribes and Patrick Sprenger and Mark A. Hoefer and P. Engels and Boaz Ilan and M. E. Mossman}, doi = {10.1103/38f7-ym2v}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {193402}, shortjournal = {Phys. Rev. Lett.}, title = {Breaking a superfluid harmonic dam: Observation and theory of riemann invariants and accelerating sonic horizons}, volume = {135}, year = {2025}, }
• (2025). Mass-gap description of heavy impurities in fermi gases. PRL, 135(19), 193401. (www)

  @article{ , abstract = {We present a unified theory that connects the quasiparticle picture of Fermi polarons for mobile impurities to the Anderson orthogonality catastrophe for static impurities. By operator reordering of the underlying many-body Hamiltonian, we obtain a modified fermionic dispersion relation that features a recoil-induced energy gap, which we call the “mass gap.” We show that the resulting mean-field Hamiltonian exhibits an in-gap state for finite impurity mass, which takes a key role in Fermi polaron and molecule formation. We identify the mass gap as the microscopic origin of the quasiparticle weight of Fermi polarons and derive a power-law scaling of the weight with the impurity-to-fermion mass ratio. The associated in-gap state is shown to give rise to the emergence of the polaron-to-molecule transition away from the limiting case of the Anderson orthogonality catastrophe in which the transition is absent.}, archive = {J_PRL}, author = {Xin Chen and Eugen Dizer and Emilio Ramos Rodríguez and Richard Schmidt}, doi = {10.1103/h2f7-dhjh}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {193401}, shortjournal = {Phys. Rev. Lett.}, title = {Mass-gap description of heavy impurities in fermi gases}, volume = {135}, year = {2025}, }
• (2025). Clock precision beyond the standard quantum limit at 10−18 level. PRL, 135(19), 193202. (www)

  @article{ , abstract = {Optical atomic clocks with unrivaled precision and accuracy have advanced the frontier of precision measurement science and opened new avenues for exploring fundamental physics. A fundamental limitation on clock precision is the standard quantum limit (SQL), which stems from the uncorrelated projection noise of each atom. State-of-the-art optical lattice clocks interrogate large ensembles to minimize the SQL, but density-dependent frequency shifts pose challenges to scaling the atom number. The SQL can be surpassed, however, by leveraging entanglement, though it remains an open problem to achieve quantum advantage from spin squeezing at state-of-the-art stability levels. Here, we demonstrate clock performance beyond the SQL, achieving a fractional frequency precision of for a single spin-squeezed clock. With cavity-based quantum nondemolition measurements, we prepare two spin-squeezed ensembles of strontium atoms confined in a two-dimensional optical lattice. A synchronous clock comparison with an interrogation time of 61 ms achieves a metrological improvement of 2.0(2) dB beyond the SQL, after correcting for state preparation and measurement errors. These results establish the most precise entanglement-enhanced clock to date and offer a powerful platform for exploring the interplay of gravity and quantum entanglement.}, archive = {J_PRL}, author = {Y. A. Yang and Maya Miklos and Yee Ming Tso and Stella Kraus and Joonseok Hur and Jun Ye}, doi = {10.1103/6v93-whwq}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {193202}, shortjournal = {Phys. Rev. Lett.}, title = {Clock precision beyond the standard quantum limit at 10−18 level}, volume = {135}, year = {2025}, }
• (2025). Spin polarization in strong-field ionization as sensor of trapped electron orbits. PRL, 135(19), 193201. (www)

  @article{ , abstract = {We show how spin polarization of photoelectrons produced in strong-field ionization of noble-gas atoms can be used to detect highly unexpected electron orbits created in strong, circularly polarized near-infrared fields. In such fields, ionization is expected to generate photoelectrons rapidly moving away from the ionic core, freezing their initial spin due to the short-range nature of the spin-orbit interaction between the photoelectron and the core. However, we find clear evidence of spin flips in the photoelectron spectra at low photoelectron energies and confirm that they happen because a photoelectron has been trapped near the core. The presence of such highly unexpected orbits explains the marked deviations between the recent experimental measurements of spin polarization [ Nat. Photonics 10 , 526 (2016) ] and simulations with frozen spin.}, archive = {J_PRL}, author = {Linxuan Zhang and Stefanos Carlström and Olga Smirnova and Misha Ivanov and Difa Ye}, doi = {10.1103/9f8y-td77}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {193201}, shortjournal = {Phys. Rev. Lett.}, title = {Spin polarization in strong-field ionization as sensor of trapped electron orbits}, volume = {135}, year = {2025}, }
• (2025). Measurement of the g factor of ground-state sr87 at the parts-per-million level using co-trapped ultracold atoms. PRL, 135(19), 193001. (www)

  @article{ , abstract = {We demonstrate nuclear magnetic resonance of optically trapped ground-state ultracold atoms. Using a scheme in which a cloud of ultracold is co-trapped nearby, we improve the determination of the nuclear factor, of atomic by more than two orders of magnitude, reaching accuracy at the parts-per-million level. We achieve similar accuracy in the ratio of relevant factors between Rb and Sr. This establishes ultracold as an excellent linear in-vacuum magnetometer. More generally, our Letter demonstrates how ultracold neutral atoms can be used for the precise determination of highly relevant atomic and nuclear magnetic properties. These results are important for ongoing efforts toward quantum simulation, quantum computation and optical atomic clocks employing , and other neutral alkaline-earth and alkaline-earth-like atoms.}, archive = {J_PRL}, author = {Premjith Thekkeppatt and Digvijay and Alexander Urech and Florian Schreck and Klaasjan van Druten}, doi = {10.1103/cjks-9hlp}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {193001}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of the g factor of ground-state sr87 at the parts-per-million level using co-trapped ultracold atoms}, volume = {135}, year = {2025}, }
• (2025). Unraveling the structure of Λ hyperons with polarized ΛΛ¯ pairs. PRL, 135(19), 191902. (www)

  @article{ , abstract = {With data collected in a dedicated energy scan from 2.3864 up to 3.0800 GeV, the BESIII Collaboration provides the first complete energy-dependent measurements of the electromagnetic form factors in the timelike region. By combining double-tag and single-tag events from the reaction, we achieve a complete decomposition of the spin structure of the reaction at five energy points, with high statistical and systematic precision. Our data reveal that while the modulus of the ratio between the electric and magnetic form factor, remains fairly constant across the considered energy range, the relative phase changes by more than 90° between 2.396 and 2.6544 GeV. Using a fit to our data based on dispersion relations, the complex form factor ratio is determined as a function of , and the preferred solution has multiple zero-crossings in the complex plane. From the derivative of the ratio at , the root-mean-squared charge radius of the is obtained. The two most probable solutions yield a negative root-mean-squared charge radius, indicating an asymmetric charge distribution where the quark pair lies close to the center of the hyperon.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and J. Biernat and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Y. Y. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and F. M. Melendi and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and L. F. Tang and M. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and V. Thoren and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/9f1h-fl4k}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191902}, shortjournal = {Phys. Rev. Lett.}, title = {Unraveling the structure of Λ hyperons with polarized ΛΛ¯ pairs}, volume = {135}, year = {2025}, }
• (2025). Window observables for benchmarking parton distribution functions. PRL, 135(19), 191901. (www)

  @article{ , abstract = {Global analysis of collider and fixed-target experimental data and calculations from lattice quantum chromodynamics (QCD) are used to gain complementary information on the structure of hadrons. We propose novel “window observables” that allow for higher precision cross-validation between the different approaches, a critical step for studies that wish to combine the datasets. Global analyses are limited by the kinematic regions accessible to experiment, particularly in a range of Bjorken- x , and lattice QCD calculations also have limitations requiring extrapolations to obtain the parton distributions. We provide two different window observables that can be defined within a region of x where extrapolations and interpolations in global analyses remain reliable and where lattice QCD results retain sensitivity and precision.}, archive = {J_PRL}, author = {Joe Karpie and Christopher J. Monahan and Kostas Orginos and Savvas Zafeiropoulos}, doi = {10.1103/q6jl-816j}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191901}, shortjournal = {Phys. Rev. Lett.}, title = {Window observables for benchmarking parton distribution functions}, volume = {135}, year = {2025}, }
• (2025). Gravitational wave scattering via the born series: Scalar tidal matching to O(G7) and beyond. PRL, 135(19), 191601. (www)

  @article{ , abstract = {We introduce a novel method to compute gravitational wave amplitudes within the framework of effective field theory. By reinterpreting the Feynman diagram expansion as a Born series, our method offers several key advantages. It directly yields partial wave amplitudes, streamlining the matching with black hole perturbation theory. Long-distance gravitational interactions are unambiguously factorized from short-distance tidal effects, including dissipation, which are systematically incorporated via an in-in worldline effective action. Crucially, at every order in perturbation theory, integrals are expressed in terms of harmonic polylogarithms, enabling an end-to-end computation scalable to arbitrary orders. We illustrate the method with new predictions for scalar black hole Love numbers and their renormalization group equations to O ( G 7 ) .}, archive = {J_PRL}, author = {Simon Caron-Huot and Miguel Correia and Giulia Isabella and Mikhail Solon}, doi = {10.1103/qd3c-nfz6}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191601}, shortjournal = {Phys. Rev. Lett.}, title = {Gravitational wave scattering via the born series: Scalar tidal matching to O(G7) and beyond}, volume = {135}, year = {2025}, }
• (2025). Black hole airy tail. PRL, 135(19), 191501. (www)

  @article{ , abstract = {In Jackiw-Teitelboim (JT) gravity, which is dual to a random matrix ensemble, the annealed entropy differs from the quenched entropy at low temperatures and goes negative. However, computing the quenched entropy in JT gravity requires a replica limit that is poorly understood. To circumvent this, we define an intermediate quantity called the semiquenched entropy, which has the positivity properties of the quenched entropy, while requiring a much simpler replica trick. We compute this in JT gravity in different regimes using (i) a bulk calculation involving wormholes corresponding to the Airy limit of the dual matrix integral and (ii) a boundary calculation involving one-eigenvalue instanton saddles proposed by Hernández-Cuenca, demonstrating consistency between these two calculations in their common regime of validity. We also clarify why similar one-eigenvalue instanton saddles cannot be used to compute the quenched entropy due to a breakdown of the saddle-point approximation for the one-eigenvalue instanton in the replica limit. Our results show how to use the gravitational path integral to prove that black holes in JT gravity have isolated ground states and to study their properties.}, archive = {J_PRL}, author = {Stefano Antonini and Luca V. Iliesiu and Pratik Rath and Patrick Tran}, doi = {10.1103/ft96-b212}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191501}, shortjournal = {Phys. Rev. Lett.}, title = {Black hole airy tail}, volume = {135}, year = {2025}, }
• (2025). Can premature collapse form black holes in the upper and lower mass gaps?. PRL, 135(19), 191401. (www)

  @article{ , abstract = {Observations of gravitational waves from binary black hole mergers, including the recent signals GW231123 and GW230529, have revealed multiple progenitor black holes in the so-called upper and lower mass gaps, respectively. It is generally assumed that massive stars cannot form black holes in the upper mass gap because pair instabilities in the late stage of stellar evolution disrupt the stars, whereas the lower mass gap refers to the gap between the maximum allowed neutron-star mass and the smallest black hole mass expected to form in supernova explosions. Here we explore a premature collapse scenario in which upper mass gap stars collapse and form black holes before they reach the late stage of stellar evolution. The mechanism for triggering a premature collapse is the capture of a smaller black hole, possibly primordial in nature. A similar capture scenario can occur to produce black holes in the lower mass gap. At least for massive stars, typical stellar rotation rates would likely result in rapidly rotating black holes in such a scenario, naturally explaining the rapid spins inferred from GW231123. Even though our estimates hinge on several parameters with rather large uncertainties, they suggest that, at least in galactic disks, the likelihood of such a capture is small for stars in the upper mass gap, but may lead to a significant population of black holes in the lower mass gap and, in fact, even below the lower mass gap.}, archive = {J_PRL}, author = {Thomas W. Baumgarte and Stuart L. Shapiro}, doi = {10.1103/26yd-1mhd}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191401}, shortjournal = {Phys. Rev. Lett.}, title = {Can premature collapse form black holes in the upper and lower mass gaps?}, volume = {135}, year = {2025}, }
• (2025). Sub-GeV dark matter direct detection with neutrino observatories. PRL, 135(19), 191003. (www)

  @article{ , abstract = {We present a new technique for sub-GeV dark matter (DM) searches and a new use of neutrino observatories. DM-electron scattering in an observatory can excite or ionize target molecules, which then produce light that can be detected by the photomultiplier tubes (PMTs). While individual DM scatterings are indistinguishable, the aggregate rate from many independent scatterings can be isolated from the total PMT dark rate using the expected DM annual modulation. We showcase this technique with the example of JUNO, a 20 000-ton scintillator detector, showing that its potential sensitivity in some mass ranges exceeds other techniques and reaches key particle-theory benchmarks.}, archive = {J_PRL}, author = {Rebecca K. Leane and John F. Beacom}, doi = {10.1103/mcyx-g4pd}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191003}, shortjournal = {Phys. Rev. Lett.}, title = {Sub-GeV dark matter direct detection with neutrino observatories}, volume = {135}, year = {2025}, }
• (2025). Mirages and large TeV halo-pulsar offsets from cosmic-ray propagation. PRL, 135(19), 191002. (www)

  @article{ , abstract = {The study of extended -ray sources usually assumes symmetric diffusion of cosmic rays. However, recent observations of multiple sources near single pulsars and significant offsets between TeV halo centroids and their parent pulsars suggest that this assumption is overly simplistic. In this Letter, we demonstrate that asymmetric propagation of cosmic rays near their accelerators may create multiple TeV sources instead of a single symmetric source. This mechanism also explains the large offsets between TeV halo centroids and their parent pulsars. We demonstrate that several perplexing detected sources can be naturally interpreted without invoking additional invisible accelerators.}, archive = {J_PRL}, author = {Yiwei Bao and Gwenael Giacinti and Ruo-Yu Liu and Hai-Ming Zhang and Yang Chen}, doi = {10.1103/xqvb-lkrr}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191002}, shortjournal = {Phys. Rev. Lett.}, title = {Mirages and large TeV halo-pulsar offsets from cosmic-ray propagation}, volume = {135}, year = {2025}, }
• (2025). Search for axion dark matter from 1.1 to 1.3 GHz with ADMX. PRL, 135(19), 191001. (www)

  @article{ , abstract = {Axion dark matter can satisfy the conditions needed to account for all of the dark matter and solve the strong problem. The Axion Dark Matter eXperiment (ADMX) is a direct dark matter search using a haloscope to convert axions to photons in an external magnetic field. Key to this conversion is the use of a microwave resonator that enhances the sensitivity at the frequency of interest. The ADMX experiment boosts its sensitivity using a dilution refrigerator and near quantum-limited amplifier to reduce the noise level in the experimental apparatus. In the most recent run, ADMX searched for axions between 1.10 and 1.31 GHz to extended Kim-Shifman-Vainshtein-Zakharov sensitivity. This Letter reports on the results of that run, as well as unique aspects of this experimental setup.}, archive = {J_PRL}, author = {G. Carosi and C. Cisneros and N. Du and S. Durham and N. Robertson and C. Goodman and M. Guzzetti and C. Hanretty and K. Enzian and L. J. Rosenberg and G. Rybka and J. Sinnis and D. Zhang and John Clarke and I. Siddiqi and A. S. Chou and M. Hollister and A. Sonnenschein and S. Knirck and T. J. Caligiure and J. R. Gleason and A. T. Hipp and P. Sikivie and M. E. Solano and N. S. Sullivan and D. B. Tanner and R. Khatiwada and L. D. Duffy and C. Boutan and T. Braine and E. Lentz and N. S. Oblath and M. S. Taubman and E. J. Daw and C. Mostyn and M. G. Perry and C. Bartram and J. Laurel and A. Yi and T. A. Dyson and S. Ruppert and M. O. Withers and C. L. Kuo and B. T. McAllister and J. H. Buckley and C. Gaikwad and J. Hoffman and K. Murch and M. Goryachev and E. Hartman and A. Quiskamp and M. E. Tobar and ADMX Collaboration}, doi = {10.1103/d7mg-6sqq}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {191001}, shortjournal = {Phys. Rev. Lett.}, title = {Search for axion dark matter from 1.1 to 1.3 GHz with ADMX}, volume = {135}, year = {2025}, }
• (2025). Noise constraints on sensitivity scaling in quantum nonlinear metrology. PRL, 135(19), 190802. (www)

  @article{ , abstract = {Quantum-enhanced metrology surpasses classical metrology by improving estimation precision scaling with a resource N (e.g., particle number or energy) from 1 / N to 1 / N . Through the use of nonlinear effects, Roy and Braunstein [Exponentially enhanced quantum metrology, Phys. Rev. Lett. 100 , 220501 (2008) ] derived a 1 / 2 N scaling. However, later works argued this exponential improvement is unphysical and that even modest gains, like 1 / N 2 , may vanish under noise. We show that, in the presence of small errors, the nonlinear interactions enabling metrological enhancement induce emergent errors. The errors propagate through the sensing protocol and are magnified proportional to any intended nonlinear enhancement. We identify a critical value of the parameter to be estimated, for a fixed error, below which the emergent errors can be avoided.}, archive = {J_PRL}, author = {Noah Lordi and John Drew Wilson and Murray J. Holland and Joshua Combes}, doi = {10.1103/pwzb-xbzf}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190802}, shortjournal = {Phys. Rev. Lett.}, title = {Noise constraints on sensitivity scaling in quantum nonlinear metrology}, volume = {135}, year = {2025}, }
• (2025). Device-independent quantum key activation. PRL, 135(19), 190801. (www)

  @article{ , abstract = {Device-independent quantum key distribution (DIQKD) allows two distant parties to establish a secret key, based only on the observed Bell nonlocal distribution. It remains unclear, however, what the minimal resources for enabling DIQKD are and how to maximize the key rate from a given distribution. In the present Letter, we consider a scenario where several copies of a given quantum distribution are jointly processed via a local and classical wiring operation. We find that, under few assumptions, it is possible to activate device-independent key, that is, starting from a distribution that is useless in a DIQKD protocol, we obtain a positive asymptotic key rate by wiring several copies together. We coin this effect device-independent key activation. Our analysis focuses on the standard DIQKD protocol with one-way postprocessing, and we resort to semidefinite programming techniques for computing lower bounds on the key rate.}, archive = {J_PRL}, author = {Bora Ulu and Nicolas Brunner and Mirjam Weilenmann}, doi = {10.1103/f8jc-q1kg}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190801}, shortjournal = {Phys. Rev. Lett.}, title = {Device-independent quantum key activation}, volume = {135}, year = {2025}, }
• (2025). From light-cone to supersonic propagation of correlations by competing short- and long-range couplings. PRL, 135(19), 190402. (www)

  @article{ , abstract = {We investigate the dynamical spreading of correlations in many-body quantum systems with competing short- and global-range couplings. We monitor the nonequilibrium dynamics of the correlations following a quench, showing that for strong short-range couplings the propagation of correlations is dominated at short and intermediate distances by a causal, light-cone dynamics, resembling the purely short-range quantum systems. However, the interplay of short- and global-range couplings leads to a crossover between space-time regions in which the light cone persists to regions where a supersonic, distance-independent spreading of the correlations occurs. We identify the important ingredients needed for capturing the supersonic spreading and demonstrate our findings in systems of interacting bosonic atoms, in which the global-range coupling is realized by a coupling to a cavity light field or atomic long-range interactions, respectively. We show that our results hold in both one and two dimensions and in the presence of dissipation. Furthermore, we characterize the short-time power-law scaling of the distance-independent growth of the density-density correlations.}, archive = {J_PRL}, author = {Catalin-Mihai Halati and Ameneh Sheikhan and Giovanna Morigi and Corinna Kollath and Simon B. Jäger}, doi = {10.1103/tt11-vcpr}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190402}, shortjournal = {Phys. Rev. Lett.}, title = {From light-cone to supersonic propagation of correlations by competing short- and long-range couplings}, volume = {135}, year = {2025}, }
• (2025). Dynamical complexity of non-gaussian many-body systems with dissipation. PRL, 135(19), 190401. (www)

  @article{ , abstract = {We characterize the dynamical state of many-body bosonic and fermionic many-body models with intersite Gaussian couplings, on-site non-Gaussian interactions, and local dissipation comprising incoherent particle loss, particle gain, and dephasing. We first establish that, for fermionic systems, if the dephasing noise is larger than the non-Gaussian interactions, irrespective of the Gaussian coupling strength, the system state is a convex combination of Gaussian states at all times. Furthermore, for bosonic systems, we show that if the particle loss and particle gain rates are larger than the Gaussian intersite couplings, the system remains in a separable state at all times. Building on this characterization, we establish that at noise rates above a threshold, there exists a classical algorithm that can efficiently sample from the system state of both the fermionic and bosonic models. Finally, we show that, unlike fermionic systems, bosonic systems can evolve into states that are not convex Gaussian even when the dissipation is much higher than the on-site non-Gaussianity. Similarly, unlike bosonic systems, fermionic systems can generate entanglement even with noise rates much larger than the intersite couplings.}, archive = {J_PRL}, author = {Guillermo González-García and Alexey V. Gorshkov and J. Ignacio Cirac and Rahul Trivedi}, doi = {10.1103/rd56-b8tc}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190401}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical complexity of non-gaussian many-body systems with dissipation}, volume = {135}, year = {2025}, }
• (2025). Simplest kochen-specker set. PRL, 135(19), 190203. (www)

  @article{ , abstract = {Kochen-Specker (KS) sets are fundamental in physics. Every time nature produces bipartite correlations attaining the nonsignaling limit, or two parties always win a nonlocal game impossible to always win classically, it is because the parties are measuring a KS set. The simplest quantum system in which all these phenomena occur is a pair of three-level systems. However, the simplest KS sets known in dimension three are asymmetrical and require a large number of bases (the current minimum is 16, set by Peres and Penrose). Here, we present a KS set that is much more symmetrical and easier to prove than any previous example. It sets a new record for minimum number of bases, 14, and enables us to refute Conjecture 2 in Cabello Simplest bipartite perfect quantum strategies, Phys. Rev. Lett. 134 , 010201 (2025) , setting a new record for qutrit-qutrit perfect strategies with a minimum number of inputs: 5–9. We establish the fundamental nature of this set in quantum theory.}, archive = {J_PRL}, author = {Adán Cabello}, doi = {10.1103/fx9d-488z}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190203}, shortjournal = {Phys. Rev. Lett.}, title = {Simplest kochen-specker set}, volume = {135}, year = {2025}, }
• (2025). Semiclassical approach to quantum fisher information. PRL, 135(19), 190202. (www)

  @article{ , abstract = {Quantum sensors driven into the quantum chaotic regime can have dramatically enhanced sensitivity, which, however, depends intricately on the details of the underlying classical phase space. Here, we develop an accurate semiclassical approach that provides direct and efficient access to the phase-space-resolved quantum Fisher information (QFI), the central quantity that quantifies the ultimate achievable sensitivity. This approximation reveals, in very concrete terms, that the QFI is large whenever a specific dynamical quantity tied to the sensing parameter displays a large variance over the course of the corresponding classical time evolution. Applied to a paradigmatic system of quantum chaos, the kicked top, we show that the semiclassical description is accurate already for modest quantum numbers, i.e., deep in the quantum regime, and it extends seamlessly to very high quantum numbers that are beyond the reach of other methods.}, archive = {J_PRL}, author = {Mahdi RouhbakhshNabati and Daniel Braun and Henning Schomerus}, doi = {10.1103/h4sg-mq1m}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190202}, shortjournal = {Phys. Rev. Lett.}, title = {Semiclassical approach to quantum fisher information}, volume = {135}, year = {2025}, }
• (2025). Subsystem decompositions of quantum evolutions and transformations between causal perspectives. PRL, 135(19), 190201. (www)

  @article{ , abstract = {One can theoretically conceive of processes in which quantum operations are composed cyclically in a way that is incompatible with a well-defined causal order. Some of these processes can be realized within standard quantum temporal evolutions on systems that are delocalized in time. In this Letter, we introduce the “circuit (super)operator,” a tool that allows one to express how a (possibly cyclic) quantum circuit transforms under arbitrary changes of subsystem decompositions. This framework concisely captures the link between causally indefinite processes and their temporal realizations. We apply it to the quantum switch, a paradigmatic example of a causally indefinite process, and consider two distinct temporal realizations. These correspond to the “causal perspectives” or “causal reference frames” of the two parties involved, describing the process from their respective viewpoints. Surprisingly, we show that these causal perspectives cannot be related by a change of subsystem decomposition, i.e., they cannot be seen as two equivalent descriptions of the same process.}, archive = {J_PRL}, author = {Julian Wechs and Ognyan Oreshkov}, doi = {10.1103/9mk4-8sn5}, journal = {Physical Review Letters}, month = {11}, number = {19}, pages = {190201}, shortjournal = {Phys. Rev. Lett.}, title = {Subsystem decompositions of quantum evolutions and transformations between causal perspectives}, volume = {135}, year = {2025}, }
• (2025). Erratum: Persistence of spin coherence in a crystalline environment [Phys. rev. lett. 133, 056901 (2024)]. PRL, 135(18), 189901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 189901 (2025)}, archive = {J_PRL}, author = {Gerald Curran, III and Zachary Rex and Casper Xallan Wilson and Luke J. Weaver and Ivan Biaggio}, doi = {10.1103/6vzz-8zys}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {189901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Persistence of spin coherence in a crystalline environment [Phys. rev. lett. 133, 056901 (2024)]}, volume = {135}, year = {2025}, }
• (2025). Ma and cui reply:. PRL, 135(18), 189301. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 189301 (2025)}, archive = {J_PRL}, author = {Yinfeng Ma and Xiaoling Cui}, doi = {10.1103/wcfn-lyb8}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {189301}, shortjournal = {Phys. Rev. Lett.}, title = {Ma and cui reply:}, volume = {135}, year = {2025}, }
• (2025). Confinement reduces surface accumulation of swimming bacteria. PRL, 135(18), 188401. (www)

  @article{ , abstract = {Many swimming bacteria naturally inhabit confined environments, yet how confinement influences their swimming behaviors remains unclear. Here, we combine experiments, continuum modeling, and particle-based simulations to investigate near-surface bacterial swimming in dilute suspensions under varying confinement. Confinement reduces near-surface accumulation and facilitates bacterial escape. These effects are quantitatively captured by models incorporating the force quadrupole, a higher-order hydrodynamic singularity, that generates a rotational flow reorienting bacteria away from surfaces. Under strong confinement, bacterial trajectories straighten due to the balancing torques exerted by opposing surfaces. These findings highlight the role of hydrodynamic quadrupole interactions in near-surface bacterial motility, with implications for microbial ecology, infection control, and industrial applications.}, archive = {J_PRL}, author = {Da Wei and Shiyuan Hu and Tangmiao Tang and Yaochen Yang and Fanlong Meng and Yi Peng}, doi = {10.1103/dvc8-tlh1}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {188401}, shortjournal = {Phys. Rev. Lett.}, title = {Confinement reduces surface accumulation of swimming bacteria}, volume = {135}, year = {2025}, }
• (2025). Reentrant transition to collective actuation in active solids with a polarizing field. PRL, 135(18), 188302. (www)

  @article{ , abstract = {Collective actuation in active solids—the spontaneous coherent excitation of a few vibrational modes—emerges from feedback between structural deformations and the orientation of active forces. It is an excellent candidate as a basic mechanism for oscillatory dynamics and regulation in dense living systems, and better control over its onset would open new avenues in the life sciences. Combining model experiments, simulations, and theory, we study the dynamics of such an active solid in the presence of an external field that polarizes the active forces. The experiments reveal a novel oscillatory regime absent at zero field. The theoretical analysis of a single agent demonstrates that the small field oscillations and the large field ones can be mapped onto the bounded and unbounded phase dynamics of a nonlinear pendulum. In the many-agents case, the transition to collective actuation is promoted at low field, leading to a reentrant transition.}, archive = {J_PRL}, author = {Paul Baconnier and Mathéo Aksil and Vincent Démery and Olivier Dauchot}, doi = {10.1103/qj64-m15g}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {188302}, shortjournal = {Phys. Rev. Lett.}, title = {Reentrant transition to collective actuation in active solids with a polarizing field}, volume = {135}, year = {2025}, }
• (2025). Rheologically tuned modes of collective transport in active viscoelastic films. PRL, 135(18), 188301. (www)

  @article{ , abstract = {While many living biological media combine both viscous and elastic properties, most theoretical studies employ either purely fluid or solidlike descriptions. We here use a unified framework for active films on substrates capable of describing a range of viscoelastic behavior to explore the interplay between activity and rheology. The core of the study is a comprehensive state diagram showing a rich world of spatiotemporal dynamic states. Our results demonstrate the potential of tunable rheology to realize modes of controlled active transport on the microscale.}, archive = {J_PRL}, author = {Henning Reinken and Andreas M. Menzel}, doi = {10.1103/gbm1-p9cg}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {188301}, shortjournal = {Phys. Rev. Lett.}, title = {Rheologically tuned modes of collective transport in active viscoelastic films}, volume = {135}, year = {2025}, }
• (2025). Toughness of double network hydrogels: The role of reduced stress propagation. PRL, 135(18), 188201. (www)

  @article{ , abstract = {Double network hydrogels show remarkable mechanical performance, combining high strength and fracture toughness with sufficient stiffness to bear load, despite containing only a low density of cross-linked polymer molecules in water. We introduce a simple mesoscale model of a double network material, detailed enough to resolve the salient microphysics of local plastic bond breakage, yet simple enough to address macroscopic cracking. Load sharing between the networks results in a delocalization of stress such that the double network inherits both the stiffness of its stiff-and-brittle sacrificial network and the ductility of its soft-and-ductile matrix network. The underlying mechanism is a reduction in the Eshelby stress propagator between sacrificial bonds, inhibiting the tendency for the plastic failure of one sacrificial bond to propagate stress to neighboring sacrificial bonds and cause a follow-on cascade of breakages. The mechanism of brittle macroscopic cracking is thereby suppressed, giving instead ductile deformation via diffusely distributed microcracking.}, archive = {J_PRL}, author = {Samuel B. Walker and Suzanne M. Fielding}, doi = {10.1103/kck9-tc46}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {188201}, shortjournal = {Phys. Rev. Lett.}, title = {Toughness of double network hydrogels: The role of reduced stress propagation}, volume = {135}, year = {2025}, }
• (2025). Non-markovian linear vibrational absorption spectroscopy for nonharmonic bond potentials: A perturbative approach. PRL, 135(18), 188002. (www)

  @article{ , abstract = {The dynamic coupling of a vibrating molecular bond to its responsive liquid environment can be described by non-Markovian friction in the framework of the generalized Langevin equation (GLE) and gives rise to line shifts as well as homogeneous and inhomogeneous spectral line broadening. By perturbation theory, we investigate how the interplay of nonharmonic bond-potential contributions and non-Markovian friction determines vibrational line shapes and positions. The accuracy of our perturbation theory is checked by simulations of the GLE. Based on bond potentials and time-dependent friction functions extracted from ab initio molecular dynamics simulations, our analytic theory traces the inhomogeneous line broadening of the infrared OH-stretch band of liquid water back to the coupling of non-Markovian friction to cubic and quartic bond-potential contributions.}, archive = {J_PRL}, author = {Hélène Colinet and Florian N. Brünig and Roland R. Netz}, doi = {10.1103/btts-7ym9}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {188002}, shortjournal = {Phys. Rev. Lett.}, title = {Non-markovian linear vibrational absorption spectroscopy for nonharmonic bond potentials: A perturbative approach}, volume = {135}, year = {2025}, }
• (2025). Secular dipolar order of nuclear spins in rotating solids. PRL, 135(18), 188001. (www)

  @article{ , abstract = {Nuclear spins’ dipolar order is created under magic angle spinning through the first-order process made possible by simultaneous implementation of dipolar recoupling and adiabatic demagnetization in a reference frame reached out through nested transformations, first from the laboratory frame into the rotating frame, and then into the spin coordinate system nutating inside its parent frame. In such a nutating frame, both the static and resonantly rotating radio-frequency (rf) fields are invisible, and the reintroduced dipolar interaction provides a secular eigenstate on which dipolar order develops with assist of an additional portion of rf field designed to implement adiabatic demagnetization in the nutating frame.}, archive = {J_PRL}, author = {Kohei Suzuki and Kazuyuki Takeda}, doi = {10.1103/qt29-gskn}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {188001}, shortjournal = {Phys. Rev. Lett.}, title = {Secular dipolar order of nuclear spins in rotating solids}, volume = {135}, year = {2025}, }
• (2025). Universal roughness and the dynamics of urban expansion. PRL, 135(18), 187403. (www)

  @article{ , abstract = {Urban sprawl reshapes cities, yet its quantitative laws remain elusive. Analyzing built-up expansion in 19 cities (1985–2015) with tools from surface growth physics in radial geometry, we reveal anisotropic, branchlike growth and a piecewise linear scaling between area and population. We uncover a robust local roughness exponent , coexisting with variable and . This unusual coexistence of universal and variable exponents offers a rare empirical test bed for nonequilibrium growth and an empirical basis for modeling urban sprawl.}, archive = {J_PRL}, author = {Ulysse Marquis and Oriol Artime and Riccardo Gallotti and Marc Barthelemy}, doi = {10.1103/rlkq-t36n}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {187403}, shortjournal = {Phys. Rev. Lett.}, title = {Universal roughness and the dynamics of urban expansion}, volume = {135}, year = {2025}, }
• (2025). Nonreciprocal spin-glass transition and aging. PRL, 135(18), 187402. (www)

  @article{ , abstract = {Disordered systems generically exhibit aging and a glass transition. Previous studies have long suggested that nonreciprocity tends to destroy glassiness. Here, we show that this is not always the case using a bipartite spherical Sherrington-Kirkpatrick model that describes the antagonistic coupling between two identical complex agents modeled as macroscopic spin glasses. Our dynamical mean-field theory calculations reveal an exceptional-point-mediated transition from a static disorder phase to an oscillating amorphous phase as well as nonreciprocal aging with slow dynamics and oscillations.}, archive = {J_PRL}, author = {Giulia Garcia Lorenzana and Ada Altieri and Giulio Biroli and Michel Fruchart and Vincenzo Vitelli}, doi = {10.1103/PhysRevLett.135.187402}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {187402}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal spin-glass transition and aging}, volume = {135}, year = {2025}, }
• (2025). Partial information rate decomposition. PRL, 135(18), 187401. (www)

  @article{ , abstract = {Partial information decomposition (PID) is a principled and flexible method to unveil complex high-order interactions in multiunit network systems. Though being defined exclusively for random variables, PID is ubiquitously applied to multivariate time series taken as realizations of random processes with temporal statistical structure. Here, to overcome the incomplete and sometimes misleading depiction of high-order effects by PID schemes applied to dynamic networks, we introduce the framework of “partial information rate decomposition (PIRD).” PIRD is first formalized applying lattice theory to decompose the information shared dynamically between a target random process and a set of source processes, and then implemented for Gaussian processes through a spectral expansion of information rates. The PIRD framework is validated in simulated network systems and demonstrated in the practical analysis of time series from large-scale climate oscillations.}, archive = {J_PRL}, author = {Luca Faes and Laura Sparacino and Gorana Mijatovic and Yuri Antonacci and Leonardo Ricci and Daniele Marinazzo and Sebastiano Stramaglia}, doi = {10.1103/nrwj-n8lj}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {187401}, shortjournal = {Phys. Rev. Lett.}, title = {Partial information rate decomposition}, volume = {135}, year = {2025}, }
• (2025). Acoustic nanoparticle trapping is driven by synergy between acoustic and hydrodynamic interactions. PRL, 135(18), 187201. (www)

  @article{ , abstract = {Acoustic forces occurring in resonant microfluidic chambers allow the handling of micrometer-sized particles. Trapping of nanoparticles has been shown for high particle concentrations and after preseeding the chamber with larger particles. We show that the trapping mechanism is due to synergy between hydrodynamic shielding and acoustic forces. Acoustic interactions are significant only when seed particles are involved and are negligible when trapping monodisperse particles. Density-selective nanoparticle trapping is suggested based on the numerical results.}, archive = {J_PRL}, author = {Alen Pavlič and Thierry Baasch}, doi = {10.1103/6l7z-bjzy}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {187201}, shortjournal = {Phys. Rev. Lett.}, title = {Acoustic nanoparticle trapping is driven by synergy between acoustic and hydrodynamic interactions}, volume = {135}, year = {2025}, }
• (2025). Topological temporal boundary states in a non-hermitian spatial crystal. PRL, 135(18), 187101. (www)

  @article{ , abstract = {Periodic modulation of the material index in time opens momentum gaps. Such systems are regarded as the temporal analog of common spatial crystals, wherein the band gaps open in frequency space. Recent studies have also led to the theoretical prediction of topological temporal boundary states (TTBSs) in such momentum gaps. In this Letter, we report the discovery and experimental realization of a new type of TTBS, appearing in a non-Hermitian spatial crystal with spatially periodic loss and gain, wherein the emergence of the Bloch momentum gap is associated with a parity-time broken phase, instead of relying on temporal modulation. By inducing a sudden flip of signs of the loss and gain profile, a mode emerges in the middle of the Bloch momentum gap and peaks at the flipping instant, which is regarded as a temporal boundary. Remarkably, we found that the temporal flip induces a topological transition in time, and the said mode is a TTBS that is a temporal analog of the Jackiw-Rebbi state. The TTBS is experimentally observed in a one-dimensional active mechanical lattice, and it can generically emerge in a wide range of non-Hermitian systems. By linking non-Hermitian physics with spatiotemporal topological systems, our results not only deepen the understanding of temporal topological phases but also open new grounds for controlling transient waves by topological means.}, archive = {J_PRL}, author = {Ming-Wei Li and Jian-Wei Liu and Xulong Wang and Wen-Jie Chen and Guancong Ma and Jian-Wen Dong}, doi = {10.1103/9b46-d2ry}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {187101}, shortjournal = {Phys. Rev. Lett.}, title = {Topological temporal boundary states in a non-hermitian spatial crystal}, volume = {135}, year = {2025}, }
• (2025). Transition from optically excited to intrinsic spin polarization in WSe2. PRL, 135(18), 186903. (www)

  @article{ , abstract = {Layered 2D van der Waals materials, such as transition metal dichalcogenides, are promising for nanoscale spintronic and optoelectronic applications. Harnessing their full potential requires understanding both intrinsic transport and the dynamics of optically excited spin and charge carriers, particularly the transition between excited spin polarization and the conduction band’s intrinsic spin texture. Here, we investigate the spin polarization of the conduction bands of bulk using static and time-resolved spin-resolved photoemission spectroscopy, complemented by photocurrent calculations. Electron doping reveals the intrinsic spin polarization, while time-resolved measurements trace the evolution of excited spin carriers. We find that intervalley scattering is spin-conserving, with spin transport initially governed by photoexcited carriers and aligning with the intrinsic conduction band spin polarization after .}, archive = {J_PRL}, author = {S. Hedwig and G. Zinke and J. Braun and B. Arnoldi and A. Pulkkinen and J. Minár and H. Ebert and M. Aeschlimann and B. Stadtmüller}, doi = {10.1103/lc2p-kl4y}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186903}, shortjournal = {Phys. Rev. Lett.}, title = {Transition from optically excited to intrinsic spin polarization in WSe2}, volume = {135}, year = {2025}, }
• (2025). Robust purely optical signatures of floquet states in laser-dressed crystals. PRL, 135(18), 186901. (www)

  @article{ , abstract = {Strong light-matter interactions can create nonequilibrium materials with on-demand novel functionalities. For periodically driven solids, the Floquet-Bloch theory provides the natural states to characterize the physical properties of these laser-dressed systems. However, signatures of such Floquet states are needed, as common experimental conditions, such as pulsed laser excitation and dissipative many-body dynamics, can disrupt their formation and survival. Here, we identify a tell-tale signature of Floquet states in the linear optical response of laser-dressed solids that remains prominent even in the presence of the strong spectral congestion of bulk matter. To do so, we introduce a computationally efficient strategy based on the Floquet formalism to finally capture the full frequency dependence in the optical response properties of realistic laser-dressed crystals, and use it investigate the Floquet engineering in a first-principle model for ZnO of full dimensionality. The computations reveal intense, spectrally isolated, laser-controllable, absorption and stimulated emission features at midinfrared energies present for a wide range of laser-driving conditions that arise due to the hybridization of the Floquet states. As such, these spectral features open a purely optical pathway to investigate the birth and survival of Floquet states in crystals while avoiding the experimental challenges of fully reconstructing the band structure of laser-dressed materials.}, archive = {J_PRL}, author = {Vishal Tiwari and Roman Korol and Ignacio Franco}, doi = {10.1103/5ywx-7dbs}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186901}, shortjournal = {Phys. Rev. Lett.}, title = {Robust purely optical signatures of floquet states in laser-dressed crystals}, volume = {135}, year = {2025}, }
• (2025). Single-mode magnon-polariton lasing and amplification controlled by dissipative coupling. PRL, 135(18), 186704. (www)

  @article{ , abstract = {We demonstrate single-mode lasing of magnon polaritons in a cavity magnonic system enabled by dissipative coupling between two passive modes, microwave cavity mode and magnon mode in a ferrimagnetic spin ensemble. The cavity mode is partially compensated through a feedback circuit, which reduces its linewidth but retains its dissipative nature. By tuning the compensation strength and dissipative coupling strength, we reach a system cooperativity of unity, marking the lasing threshold and the formation of a zero-linewidth polariton mode. This mode also corresponds to a perfect Friedrich–Wintgen bound state in the continuum. Further increase of the cooperativity drives the system into the strong dissipative coupling regime, where magnon-polariton amplification arises between two real-frequency scattering poles. These results reveal that dissipative coupling cooperativity carries a clear physical meaning and serves as a key parameter for controlling phase transitions. Dissipative coupling offers an alternative paradigm for tailoring light-matter interactions, paving the way for advances in both information processing and quantum technologies.}, archive = {J_PRL}, author = {Zi-Qi Wang and Zi-Yuan Wang and Yi-Pu Wang and J. Q. You}, doi = {10.1103/bnyn-mbwv}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186704}, shortjournal = {Phys. Rev. Lett.}, title = {Single-mode magnon-polariton lasing and amplification controlled by dissipative coupling}, volume = {135}, year = {2025}, }
• (2025). Observation of chiral magnon band splitting in altermagnetic hematite. PRL, 135(18), 186703. (www)

  @article{ , abstract = {Altermagnets, a new frontier for spintronics, represent a distinct magnet class with nonrelativistic splitting of both electronic and chiral magnon bands, yet experimental verification of their unique magnon dynamics remains scarce. In this Letter, inelastic neutron scattering experiments on reveal a clear magnon band splitting about 3 meV at . We trace the origin of this splitting to the alternating exchange interactions between the 13th nearest neighbors, as supported by first-principles calculations, and confirm that the magnons have chiral splits by theoretical modeling. This definitive characterization of chiral magnons in hematite provides the fundamental insight needed to design and control spin transport in novel spintronic applications.}, archive = {J_PRL}, author = {Qiyang Sun and Jiasen Guo and Dan Wang and Douglas L. Abernathy and Wei Tian and Chen Li}, doi = {10.1103/7yhz-jptc}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186703}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of chiral magnon band splitting in altermagnetic hematite}, volume = {135}, year = {2025}, }
• (2025). X-ray free-electron laser observation of giant and anisotropic magnetostriction in β−O2 at 110 tesla. PRL, 135(18), 186702. (www)

  @article{ , abstract = {In strong magnetic fields beyond 100 T, the significant Zeeman energy competes with the lattice interactions, where a considerable magnetostriction is expected. However, the microscopic observation of the magnetostriction above 100 T has been hindered due to the short pulse duration of microseconds and the coil’s destruction. Here, we report the observation of the giant and anisotropic magnetostriction of at 110 T in the spin-controlled crystal by combining the single-shot diffraction of an x-ray free-electron laser (XFEL) and the newly developed portable 100 T generator (PINK-02). The soft and anisotropic response of should originate in the competing van der Waals force and exchange interaction and also the frustration of spin and lattice on the triangular network. The XFEL experiment above 100 T using PINK-02 enables microscopic investigations on materials’ properties at high magnetic fields, providing insights into how spins contribute to the stability of crystal structures.}, archive = {J_PRL}, author = {Akihiko Ikeda and Yuya Kubota and Yuto Ishii and Xuguang Zhou and Shiyue Peng and Hiroaki Hayashi and Yasuhiro H. Matsuda and Kosuke Noda and Tomoya Tanaka and Kotomi Shimbori and Kenta Seki and Hideaki Kobayashi and Dilip Bhoi and Masaki Gen and Kamini Gautam and Mitsuru Akaki and Shiro Kawachi and Shusuke Kasamatsu and Toshihiro Nomura and Yuichi Inubushi and Makina Yabashi}, doi = {10.1103/r7br-qnrn}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186702}, shortjournal = {Phys. Rev. Lett.}, title = {X-ray free-electron laser observation of giant and anisotropic magnetostriction in β−O2 at 110 tesla}, volume = {135}, year = {2025}, }
• (2025). Coupling between orbital and spin degrees of freedom in jahn-teller ions for Co1−xFexV2O4. PRL, 135(18), 186701. (www)

  @article{ , abstract = {It is found that a small distortion caused by magnetostriction and a structural phase transition caused by Jahn-Teller distortion are continuously connected in under variation of . Spin-orbit coupling in Jahn-Teller-active ions gives rise to this novel correlation between spins, orbitals, and the lattice distortion in this series of compounds.}, archive = {J_PRL}, author = {Minato Nakano and Taichi Kobayashi and Takuro Katsufuji}, doi = {10.1103/5kwm-sljw}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186701}, shortjournal = {Phys. Rev. Lett.}, title = {Coupling between orbital and spin degrees of freedom in jahn-teller ions for Co1−xFexV2O4}, volume = {135}, year = {2025}, }
• (2025). Quantum hall effect without chern bands. PRL, 135(18), 186603. (www)

  @article{ , abstract = {The quantum Hall effect was originally observed in a two-dimensional electron gas forming Landau levels when exposed to a strong perpendicular magnetic field and was later generalized to Chern insulators without net magnetization. Here, further extending the realm of the quantum Hall effect, we report on the robust occurrence of an integer quantized transverse conductance at the onset of disorder in a microscopic lattice model, all bands of which are topologically trivial (zero Chern number). We attribute this phenomenon to the energetic separation of nonquantized Berry fluxes within those bands. Adding disorder then nudges the system into a quantum Hall phase from an extended critical regime obtained by placing the Fermi energy within a broad window inside a trivial band. This natural integer-rounding mechanism manifests as the mobility-gap-induced quantization of a nonuniversal Hall conductance. Our results are corroborated by numerical transport simulations and the analysis of two complementary topological markers.}, archive = {J_PRL}, author = {Benjamin Michen and Jan Carl Budich}, doi = {10.1103/dgd8-4gzf}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186603}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum hall effect without chern bands}, volume = {135}, year = {2025}, }
• (2025). Flux attachment theory of fractional excitonic insulators. PRL, 135(18), 186602. (www)

  @article{ , abstract = {The search for fractional quantized Hall phases in the absence of a magnetic field has primarily targeted flat-band systems that mimic the features of a Landau level. In an alternative approach, the fractional excitonic insulator (FEI) has been proposed as a correlated electron-hole fluid that arises near a band inversion between bands of different angular momentum with strong interactions. It remains an interesting challenge to find Hamiltonians with realistic interactions that stabilize this state. Here, we describe composite boson and composite fermion theories that highlight the importance of excitonic pairing in stabilizing FEIs in a class of band inversion models. We predict a sequence of Jain-like and Laughlin-like FEI states, the simplest of which has the topological order of the bosonic fractional quantized Hall state. We discuss implications for recent numerical studies on a chiral spin liquid phase in interacting Chern insulator models.}, archive = {J_PRL}, author = {Steven Gassner and Ady Stern and C. L. Kane}, doi = {10.1103/x789-kxy3}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186602}, shortjournal = {Phys. Rev. Lett.}, title = {Flux attachment theory of fractional excitonic insulators}, volume = {135}, year = {2025}, }
• (2025). From fractionalization to chiral topological superconductivity in a flat chern band. PRL, 135(18), 186601. (www)

  @article{ , abstract = {We show that interacting electrons in a flat Chern band can form, in addition to fractional Chern insulators, a chiral -wave topological superconductor that hosts neutral Majorana fermion edge modes. Superconductivity emerges from an interaction-induced metallic state that exhibits anomalous Hall effect, as observed in rhombohedral graphene and near the fractional Chern insulator in twisted transition metal dichalcogenides.}, archive = {J_PRL}, author = {Daniele Guerci and Ahmed Abouelkomsan and Liang Fu}, doi = {10.1103/zm39-dstj}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186601}, shortjournal = {Phys. Rev. Lett.}, title = {From fractionalization to chiral topological superconductivity in a flat chern band}, volume = {135}, year = {2025}, }
• (2025). Coexistence of insulatorlike paramagnon and metallic spin-orbit exciton modes in SrIrO3. PRL, 135(18), 186506. (www)

  @article{ , abstract = {We probe the spectrum of elementary excitations in by using heterostructured [ ] samples to approach the bulk limit. Our resonant inelastic x-ray scattering (RIXS) measurements at the Ir edge reveal a robust low-lying collective magnetic mode with an antiferromagnetic (AFM) dispersion similar to the insulators and , albeit with a large gap and much larger linewidth. At higher energies we find the spin-orbit exciton, also strongly broadened, but with an inverted dispersion and doubled periodicity that are controlled by the charge hopping. These results demonstrate that the AFM paramagnon persists, somewhat counterintuitively, far into the metallic regime of the insulator-metal transition driven by the degree of confinement in the heterostructure. We conclude that these two excitations, which are contrasting but coexisting hallmarks of strong AFM pseudospin and charge fluctuations in a spin-orbit-coupled Mott-Slater material, are properties intrinsic to the ground state of semimetallic perovskite .}, archive = {J_PRL}, author = {E. Paris and W. Zhang and Y. Tseng and A. Efimenko and C. Sahle and V. N. Strocov and E. Skoropata and K. Rolfs and T. Shang and J. Lyu and E. Pomjakushina and M. Medarde and H. M. Rønnow and B. Normand and M. Radovic and T. Schmitt}, doi = {10.1103/96fl-5zlh}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186506}, shortjournal = {Phys. Rev. Lett.}, title = {Coexistence of insulatorlike paramagnon and metallic spin-orbit exciton modes in SrIrO3}, volume = {135}, year = {2025}, }
• (2025). λ-jellium model for the anomalous hall crystal. PRL, 135(18), 186505. (www)

  @article{ , abstract = {The jellium model is a paradigmatic problem in condensed matter physics, exhibiting a phase transition between metallic and Wigner crystal phases. However, its vanishing Berry curvature makes it ill suited for studying recent experimental platforms that combine strong interactions with nontrivial quantum geometry. These experiments inspired the anomalous Hall crystal (AHC)—a topological variant of the Wigner crystal. The AHC spontaneously breaks continuous translation symmetry but has a nonzero Chern number. In this Letter, we introduce -jellium, a minimal extension of the two-dimensional jellium model. Its Berry curvature distribution is controlled by a single parameter , where corresponds to the standard jellium model. This setup facilitates the systematic exploration of Berry curvature’s impact on electron crystallization. The phase diagram of this model, established using self-consistent Hartree Fock calculations, reveals several interesting features: (i) The AHC phase occupies a large region of the phase diagram. (ii) Two distinct Wigner crystal phases, the latter enabled by quantum geometry, and two distinct Fermi liquid phases are present. (iii) A continuous phase transition separates the AHC and one of the Wigner crystal phases. (iv) In some parts of the AHC phase, the lattice geometry is nontriangular, unlike in the classical Wigner crystal. In addition to elucidating the physics of correlated electrons with nonzero Berry curvature, we expect that the simplicity of the model makes it an excellent starting point for more advanced numerical methods.}, archive = {J_PRL}, author = {Tomohiro Soejima (副島智大 and Junkai Dong (董焌锴 and Ashvin Vishwanath and Daniel E. Parker}, doi = {10.1103/x53d-12s6}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186505}, shortjournal = {Phys. Rev. Lett.}, title = {λ-jellium model for the anomalous hall crystal}, volume = {135}, year = {2025}, }
• (2025). Emergence of chiral order driven by quenched disorder. PRL, 135(18), 186504. (www)

  @article{ , abstract = {Quenched disorder can destroy magnetic order, for example, when a random field is applied in a two-dimensional Ising model. Even when an order exists in the presence of quenched disorder, it is usually only the survival of the order of the clean model. We present here a surprising phenomenon where an order emerges, driven by quenched disorder. This order has nothing in common with the order present in the clean model. This type of order by disorder differs from the usual thermal or quantum one. The classical Heisenberg model on the kagome lattice is studied by parallel tempering Monte Carlo simulations, with site dilution. After analyzing the effect of a few vacancies on the ground state, favoring noncoplanar configurations, we show the emergence of a low-temperature chiral phase and the progressive destruction of the collinear Potts order, the only order present in the absence of vacancies.}, archive = {J_PRL}, author = {Coraline Letouzé and Pascal Viot and Laura Messio}, doi = {10.1103/yyzf-jjc6}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186504}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of chiral order driven by quenched disorder}, volume = {135}, year = {2025}, }
• (2025). Field induced density wave in a kagome superconductor. PRL, 135(18), 186503. (www)

  @article{ , abstract = {On the kagome lattice, electrons benefit from the simultaneous presence of band topology, flat electronic bands, and Van Hove singularities, forming competing or cooperating orders. Understanding the interrelation between these distinct order parameters remains a significant challenge, leaving much of the associated physics unexplored. In the kagome superconductor , which exhibits a charge density wave (CDW) state below , we uncover an unpredicted field-induced phase transition below 6 K. The observed transition is marked by a hysteretic anomaly in the resistivity, nonlinear electrical transport, and a change in the symmetry of the electronic response as probed via the angular dependence of the magnetoresistivity. These observations surprisingly suggest the emergence of an unanticipated broken symmetry state coexisting with the original CDW. To understand this experimental observation, we developed a theoretical minimal model for the normal state inside the high-temperature parent CDW phase, where an incommensurate CDW order emerges as an instability subleading to superconductivity. The incommensurate CDW emerges when superconducting fluctuations become fully suppressed by large magnetic fields. Our results suggest that, in kagome superconductors, quantum states can either coexist or are nearly degenerate in energy, indicating that these are rich platforms to expose new correlated phenomena.}, archive = {J_PRL}, author = {Md. Shafayat Hossain and Qi Zhang and Julian Ingham and Jinjin Liu and Sen Shao and Yangmu Li and Yuxin Wang and Bal K. Pokharel and Zi-Jia Cheng and Yu-Xiao Jiang and Maksim Litskevich and Byunghoon Kim and Xian Yang and Yongkai Li and Tyler A. Cochran and Yugui Yao and Dragana Popović and Zhiwei Wang and Ronny Thomale and Luis Balicas and M. Zahid Hasan}, doi = {10.1103/5f9f-bsqw}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186503}, shortjournal = {Phys. Rev. Lett.}, title = {Field induced density wave in a kagome superconductor}, volume = {135}, year = {2025}, }
• (2025). High-temperature superconductivity from finite-range attractive interaction. PRL, 135(18), 186502. (www)

  @article{ , abstract = {In this Letter we consider -dimensional interacting Fermi liquids, and demonstrate that an attractive interaction with a finite range that is much greater than the Fermi wavelength breaks the conventional BCS theory of superconductivity. In contrast to the BCS prediction of a finite superconducting gap for all attractive contact interactions, we show that a finite-range interaction does not induce a superconducting gap. Instead, the pair susceptibility develops a power-law singularity at zero momentum and zero frequency signaling quantum critical behavior without long-range ordering. Starting from this, we show that superconductivity can be stabilized by adding a short-range attractive interaction, which is always present in real electronic systems. As an example, we consider a layered quasi-two-dimensional material with attractive electron-electron interactions mediated by optical phonons. We demonstrate a dome shape of the critical temperature versus doping, strongly suppressed isotope effect, and a weak dependence of the optimal doping and maximal on the interaction range at , is the Fermi energy. We believe that these results could be relevant to high-temperature superconductors.}, archive = {J_PRL}, author = {Dmitry Miserev and Joel Hutchinson and Herbert Schoeller and Jelena Klinovaja and Daniel Loss}, doi = {10.1103/glch-3385}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186502}, shortjournal = {Phys. Rev. Lett.}, title = {High-temperature superconductivity from finite-range attractive interaction}, volume = {135}, year = {2025}, }
• (2025). Polaronic quasiparticles in the valence-transition compound TmSe1−xTex. PRL, 135(18), 186501. (www)

  @article{ , abstract = {Exotic quasiparticle states have been proposed in mixed-valent compounds exhibiting valence transitions. However, clear spectroscopic evidence identifying these states has remained elusive. Using synchrotron-based hard x-ray and extreme ultraviolet photoemission spectroscopy, we have probed the Tm 3 d and 4 f emissions in TmSe 1 − x Te x , where a Te concentration-dependent semimetal–insulator transition occurs alongside the valence transition. Our photoemission results, which are characteristic of the bulk, track this combined transition across the critical concentration ( x c = 0.29 ). Notably, our results reveal a noninteger valence for the insulating phase and a novel quasiparticle excitation in the semimetallic phase: a Holstein polaron that extends beyond the standard periodic Anderson model.}, archive = {J_PRL}, author = {C.-H. Min and S. Müller and W. J. Choi and L. Dudy and V. Zabolotnyy and M. Heber and J. D. Denlinger and C.-J. Kang and M. Kalläne and N. Wind and M. Scholz and T. L. Lee and C. Schlueter and A. Gloskovskii and E. D. L. Rienks and V. Hinkov and H. Bentmann and Y. S. Kwon and F. Reinert and H.-D. Kim and K. Rossnagel}, doi = {10.1103/72dv-ynm2}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186501}, shortjournal = {Phys. Rev. Lett.}, title = {Polaronic quasiparticles in the valence-transition compound TmSe1−xTex}, volume = {135}, year = {2025}, }
• (2025). Real-time edge dynamics of non-hermitian lattices. PRL, 135(18), 186401. (www)

  @article{ , abstract = {We derive the asymptotic forms of the Green’s function at the open edges of general non-Hermitian band systems in all dimensions in the longtime limit, using a modified saddle point approximation and the analytic continuation of the momentum. The edge dynamics is determined by the “dominant saddle point,” a complex momentum which, contrary to previous conjectures, may lie outside the generalized Brillouin zone. From this result, we obtain the effective edge Hamiltonians that evidently, as demonstrated by extensive numerical simulations, characterize the dynamics on the edges and can be probed in real-time experiments or spectroscopies.}, archive = {J_PRL}, author = {Tian-Hua Yang and Chen Fang}, doi = {10.1103/llbb-pcgk}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186401}, shortjournal = {Phys. Rev. Lett.}, title = {Real-time edge dynamics of non-hermitian lattices}, volume = {135}, year = {2025}, }
• (2025). Quantum anomalous hall effect in ferromagnetic metals. PRL, 135(18), 186302. (www)

  @article{ , abstract = {The quantum anomalous Hall (QAH) effect holds fundamental importance in topological physics and technological promise for electronics. It is generally believed that the QAH effect can only be realized in insulators. In this Letter, we theoretically demonstrate that the QAH effect can also be realized in metallic systems, representing a phase distinct from the conventional QAH phase in insulators. This phase is characterized by the coexistence of chiral edge channels and isotropic bulk conduction channels without a bulk energy gap. Notably, in a six-terminal Hall bar, our calculations show that, the quantized Hall conductivity and nonzero longitudinal conductivity can emerge due to dephasing, despite the Hall resistivity itself never becoming quantized. Furthermore, the quantized Hall conductivity exhibits remarkable robustness against disorder. Our findings not only extend the range of materials capable of hosting the QAH effect from insulators to metals, but also provide insights that may pave the way for the experimental realization of the QAH effect at elevated temperatures.}, archive = {J_PRL}, author = {Yu-Hao Wan and Peng-Yi Liu and Qing-Feng Sun}, doi = {10.1103/8vs2-jvc4}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186302}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum anomalous hall effect in ferromagnetic metals}, volume = {135}, year = {2025}, }
• (2025). Distributed current injection into a one-dimensional ballistic edge channel. PRL, 135(18), 186301. (www)

  @article{ , abstract = {We generalize Landauer’s theory of ballistic transport in a one-dimensional (1D) conductor to situations where charge carrier injection and extraction are not any more confined to electrodes at either end of the channel, but may occur along its whole length. This type of distributed injection is expected to occur from the two-dimensional (2D) bulk of, e.g., a quantum spin (or anomalous) Hall insulator to its topologically protected edge states. We apply our conceptual solution to the case of two metal electrodes contacting the 2D bulk, enabling us to derive criteria that discriminate ballistic from resistive edge channels in multiterminal transport experiments.}, archive = {J_PRL}, author = {Kristof Moors and Christian Wagner and Helmut Soltner and Felix Lüpke and F. Stefan Tautz and Bert Voigtländer}, doi = {10.1103/l47r-plxq}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186301}, shortjournal = {Phys. Rev. Lett.}, title = {Distributed current injection into a one-dimensional ballistic edge channel}, volume = {135}, year = {2025}, }
• (2025). Water-induced current determines heat generation during double layer charging. PRL, 135(18), 186201. (www)

  @article{ , abstract = {Understanding heat generation during charging processes of electrical double layer (EDL) systems is crucial for electrochemical technologies in practical scenarios. Existing kinetic models, attributing heat to ionic transports, however, fail to capture experimentally observed thermal behaviors in EDLs. Herein, we employ constant-potential molecular simulations to investigate heat generation in aqueous systems under nonquasistatic processes. Atomic-scale analyses via a modified kinetic equation reveal that the water-induced electric current, neglected in existing models, is essential to heat generation in both the bulk electrolyte and EDLs. In the bulk, heat deviates from Joule heating, attributed to the nonmonotonic reorientation of water dipoles driving non-Ohmic currents; within EDLs, heat exhibits damped endothermic and exothermic oscillations, originating from water reorientation that induces alternating electric fields and unidirectional currents. These findings unveil an underappreciated mechanism of heat generation governed by solvent dynamics and establish a kinetic framework for exploring thermal behavior in EDL systems.}, archive = {J_PRL}, author = {Liang Zeng and Nan Huang and Guang Feng}, doi = {10.1103/79nl-455r}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186201}, shortjournal = {Phys. Rev. Lett.}, title = {Water-induced current determines heat generation during double layer charging}, volume = {135}, year = {2025}, }
• (2025). Body-centered-cubic phase transformation in gold at TPa pressures. PRL, 135(18), 186101. (www)

  @article{ , abstract = {In situ x-ray diffraction at both the National Ignition Facility and Omega-EP Laser Facility has been utilized to determine the crystallographic state of ramp and shock-ramp compressed gold up to 1.2 TPa ( atmospheres). In this Letter, we describe a series of experiments that explore a variety of pressure-temperature states in Au, accessed using tailored laser pulses. We find that the ambient pressure face-centered-cubic phase is stable under ramp compression to pressures of at least 1 TPa where the body-centered-cubic phase is observed simultaneously.}, archive = {J_PRL}, author = {Amy L. Coleman and Saransh Singh and Tom E. Lockard and Ian K. Ocampo and Amy E. Lazicki and Martin G. Gorman and Stefano Racioppi and Andrew G. Krygier and Christopher E. Wehrenberg and Rasool Ahmad and Marius Millot and Sebastien Hamel and Sirus Han and Mary Kate Ginnane and Damian C. Swift and Stanimir A. Bonev and Eva Zurek and Thomas S. Duffy and Jon H. Eggert and James McNaney and Raymond F. Smith}, doi = {10.1103/yzzv-2w81}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {186101}, shortjournal = {Phys. Rev. Lett.}, title = {Body-centered-cubic phase transformation in gold at TPa pressures}, volume = {135}, year = {2025}, }
• (2025). Free energy source of the mirror instability: Nonresonant particles. PRL, 135(18), 185201. (www)

  @article{ , abstract = {The mirror instability is a fundamental phenomenon in plasma physics. Given the historical discussion regarding the role of resonant particles in driving this instability—which is at odds with its presence in magnetohydrodynamic (MHD) models that only describe fluid plasma behavior—we seek to clarify the free energy source of this instability through a detailed investigation of velocity space. We introduce a method for calculating the wave-particle energy transfer rate. This diagnostic identifies that the free energy source of the mirror instability originates from nonresonant particles. This leads to a more coherent understanding of the origins of the instability within both MHD theory and plasma kinetic theory. Because of the opposing diamagnetic drift motions of the nonresonant and resonant particle populations, energy from nonresonant particles is transferred into the mirror mode waves, while resonant particles absorb energy from these waves. Consequently, both particle populations play critical roles in determining the growth rate of the linear mirror instability.}, archive = {J_PRL}, author = {Xudong Guo and Jinsong Zhao and Kristopher G. Klein and Huasheng Xie}, doi = {10.1103/x12v-h3xq}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {185201}, shortjournal = {Phys. Rev. Lett.}, title = {Free energy source of the mirror instability: Nonresonant particles}, volume = {135}, year = {2025}, }
• (2025). Data-driven construction of a generalized kinetic collision operator from molecular dynamics. PRL, 135(18), 185101. (www)

  @article{ , abstract = {We introduce a data-driven approach to learn generalized collision operators from molecular dynamics. Unlike conventional models (e.g., Landau), the present operator takes a symmetry-breaking form that depends not only on the relative velocity but also on the average velocity of the collision pair, capturing heterogeneous energy transfer arising from collective interactions with the environment. Numerical results show that preserving this overlooked anisotropy is crucial for predicting plasma kinetics and transport coefficients in the moderate coupling regime, where the Landau model fails.}, archive = {J_PRL}, author = {Yue Zhao and Joshua Burby and Andrew Christlieb and Huan Lei}, doi = {10.1103/gml7-f2ng}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {185101}, shortjournal = {Phys. Rev. Lett.}, title = {Data-driven construction of a generalized kinetic collision operator from molecular dynamics}, volume = {135}, year = {2025}, }
• (2025). Nonlocal coherent optical nonlinearities of a macroscopic quantum system. PRL, 135(18), 183801. (www)

  @article{ , abstract = {The optical responses of solids are typically understood to be local in space. Whether locality holds for the optical response of a macroscopic quantum system has, however, been largely unexplored. Here, we use multidimensional coherent spectroscopy at the optical diffraction limit to demonstrate nonlocal optical nonlinearities in a semiconductor microcavity. These nonlocal optical responses are both coherent and quantum in nature, deriving from the macroscopic length scale of confined exciton-polariton wave functions.}, archive = {J_PRL}, author = {Albert Liu and Eric W. Martin and Jiaqi Hu and Zhaorong Wang and Hui Deng and Steven T. Cundiff}, doi = {10.1103/jrds-3tyk}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183801}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlocal coherent optical nonlinearities of a macroscopic quantum system}, volume = {135}, year = {2025}, }
• (2025). Quantum-enhanced interferometer for multiphase sensing. PRL, 135(18), 183602. (www)

  @article{ , abstract = {Quantum-enhanced interferometers have been widely used in single-parameter precision measurement, and multiparameter precision measurement is the building block of numerous sensing and imaging applications. However, it remains challenging to realize high-sensitivity multiparameter sensing without increasing power, which is crucial for biological science. Here, we propose and demonstrate a deterministic quantum-enhanced interferometer, where high-sensitivity multiparameter sensing is realized by effectively squeezing noises and amplifying signals. Key technologies are essential to the results, including the parallel and sequential use of squeezed states inside the interferometer. Notably, in the quantum-enhanced three-arm interferometer, not only joint but also individual values of three signals are simultaneously measured with a signal-to-noise ratio of more than compared with that of the conventional interferometer under the same phase-sensing power. These advances constitute a critical step toward observing multiple elusive signals and give rise to a wide range of sensing and imaging applications.}, archive = {J_PRL}, author = {Yanni Feng and Zhaoqing Zeng and Jialin Cheng and Zhaolin You and Huadong Lu and Zhihui Yan and Xiaojun Jia and Changde Xie and Kunchi Peng}, doi = {10.1103/2hsx-5qfr}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183602}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-enhanced interferometer for multiphase sensing}, volume = {135}, year = {2025}, }
• (2025). Time-resolved and superradiantly amplified unruh effect. PRL, 135(18), 183601. (www)

  @article{ , abstract = {We identify low-acceleration conditions under which the Unruh effect manifests as an early superradiant burst in a collection of excited atoms. The resulting amplified Unruh signal is resolved from the inertial signal both in time and intensity. We demonstrate theoretically that these conditions are realized inside a subresonant cavity that highly suppresses the response of an inertial atom, while allowing significant response from an accelerated atom as, owing to the acceleration-induced spectral broadening, it can still couple to the available field modes. The setup thus selectively amplifies the modified field fluctuations underlying the Unruh effect into an early superradiant burst. In comparison, the field fluctuations perceived inertially would cause a superradiant burst much later. In this way, we simultaneously address the extreme acceleration requirement, the weak Unruh signal, and the dominance of the inertial signal, all within a single experimental arrangement.}, archive = {J_PRL}, author = {Akhil Deswal and Navdeep Arya and Kinjalk Lochan and Sandeep K. Goyal}, doi = {10.1103/6z1l-kkmk}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183601}, shortjournal = {Phys. Rev. Lett.}, title = {Time-resolved and superradiantly amplified unruh effect}, volume = {135}, year = {2025}, }
• (2025). Exact perturbative expansion of the transport coefficients of a normal low-temperature fermi gas with contact interactions. PRL, 135(18), 183402. (www)

  @article{ , abstract = {We compute the shear viscosity, thermal conductivity, and spin diffusivity of a Fermi gas with short-range interactions in the Fermi liquid regime of the normal phase, that is, at temperatures much lower than the Fermi temperature and larger than the superfluid critical temperature . In line with recent advances in the precision of cold atom experiments, we provide exact results up to the second order in the interaction strength. We extend the Landau-Salpeter equation to compute the collision amplitude beyond the forward-scattering limit, covering all collisions on the Fermi surface. We treat the collision kernel exactly, leading to significant corrections beyond relaxation-time or variational approximations. The transport coefficients, as functions of the wave scattering length and Fermi wave number , follow up to corrections of order , with a positive coefficient for the viscosity and negative one for the thermal conductivity and spin diffusivity.}, archive = {J_PRL}, author = {Pierre-Louis Taillat and Hadrien Kurkjian}, doi = {10.1103/c6fd-x57s}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183402}, shortjournal = {Phys. Rev. Lett.}, title = {Exact perturbative expansion of the transport coefficients of a normal low-temperature fermi gas with contact interactions}, volume = {135}, year = {2025}, }
• (2025). Observation of temperature effects on false vacuum decay in atomic quantum gases. PRL, 135(18), 183401. (www)

  @article{ , abstract = {Temperature plays a crucial role in metastable phenomena, not only by contributing to determine the state (phase) of a system, but also ruling the decay probability to more stable states. Such a situation is encountered in many different physical systems, ranging from chemical reactions to magnetic structures. The characteristic decay timescale is not always straightforward to estimate since it depends on the microscopic details of the system. A paradigmatic example in quantum field theories is the decay of the false vacuum, manifested via the nucleation of bubbles. In this Letter, we measure the temperature dependence of the timescale for the false vacuum decay mechanism in an ultracold atomic quantum spin mixture which exhibits ferromagnetic properties. Our results show that the false vacuum decay rate scales with temperature as predicted by the finite-temperature extension of the instanton theory, and confirm atomic systems as an ideal platform where to study out-of-equilibrium field theories.}, archive = {J_PRL}, author = {Riccardo Cominotti and Cosetta Baroni and Chiara Rogora and Diego Andreoni and Giacomo Guarda and Giacomo Lamporesi and Gabriele Ferrari and Alessandro Zenesini}, doi = {10.1103/l396-yysb}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183401}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of temperature effects on false vacuum decay in atomic quantum gases}, volume = {135}, year = {2025}, }
• (2025). Photoionization time delays probe electron correlations. PRL, 135(18), 183202. (www)

  @article{ , abstract = {The photoelectric effect explained by Einstein is often regarded as a one-electron phenomenon, whereas the interaction of the escaping electron with other electrons, referred to as electron correlation, plays an important role in multielectron systems. In this Letter, we study the attosecond photoionization of the outer subshell of argon in its substantial minimum cross-section region formed by electron correlation, which was theoretically predicted in 1972 and experimentally confirmed using synchrotron radiation. Combining high-spectral resolution attosecond interferometry experiments and novel theoretical calculations allows us to identify the most essential electron correlations affecting the time of photoemission, solving the long-standing inconsistency between measurements and theories, and demonstrating the contribution of coherent couplings with shakeup channels. The measurement of time delays gives unprecedented insight into the photoionization process, unraveling details of the atomic potential experienced by the escaping electron and capturing its dynamics.}, archive = {J_PRL}, author = {Mingxuan Li and Huiyong Wang and Rezvan Tahouri and Robin Weissenbilder and Jialong Li and Wentao Wang and Jiaao Cai and Xiaochun Hong and Xiaosen Shi and Liang-Wen Pi and David Busto and Mathieu Gisselbrecht and Kiyoshi Ueda and Philipp V. Demekhin and Anne L’Huillier and Jan Marcus Dahlström and Eva Lindroth and Dajun Ding and Sizuo Luo}, doi = {10.1103/ll25-15dm}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183202}, shortjournal = {Phys. Rev. Lett.}, title = {Photoionization time delays probe electron correlations}, volume = {135}, year = {2025}, }
• (2025). Search for exotic spin-dependent interactions with dressed atoms. PRL, 135(18), 183201. (www)

  @article{ , abstract = {We present a method to engineer the Landé factor of alkali-metal atoms using spin-exchange collisions and nonresonant radio-frequency (rf) magnetic-field dressing. We analyze schemes with both linearly and circularly polarized rf dressing to generate dressed states, allowing the responses to magnetic and nonmagnetic spin-dependent interactions, such as the spin-gravity interaction, to be distinguished in the output signal. Our method provides a complementary approach to conventional comagnetometry in the investigation of exotic spin-dependent interactions and gyroscopes.}, archive = {J_PRL}, author = {Xiyu Liu and Wei Xiao and Meng Liu and Xiang Peng and Teng Wu and Hong Guo}, doi = {10.1103/gg1j-4bst}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183201}, shortjournal = {Phys. Rev. Lett.}, title = {Search for exotic spin-dependent interactions with dressed atoms}, volume = {135}, year = {2025}, }
• (2025). Atomic real-space imaging of molecular statics and dynamics at confined states. PRL, 135(18), 183001. (www)

  @article{ , abstract = {Atomic imaging of molecules and intermolecular interactions is important for obtaining a deeper understanding of the related physics and chemistry. At a confined state in reticular matrix, molecular architecture can be stabilized for studying its static and dynamic behaviors, which is a milestone for molecular science but is still challenging in real space. Here, we use the coordination interactions between reticular building units of UiO-66 framework to maintain small molecules in a quasistatic structure. Low-dose electron microscopy is applied to resolving the atomic structures of these confined-state molecules. Meanwhile, the UiO-66 framework allows us modifying metal node structures for a controlled molecular manipulation by stretching and compressing. Then, the molecular statics and dynamics during stretching and compressing can be unraveled by directly measuring projected atomic positions, bond lengths, and peak widths via intensity profile analysis. These results perfectly support the predictions from our first-principles calculations, indicating the elastic deformation of coordination bonds and the varied vibration of rings. This Letter not only represents an efficient strategy for atomically controlling and imaging the molecular statics and dynamics in reticular chemistry, but also opens up a new pathway for studying other molecular behaviors and interactions at confined states from new perspectives of atoms and bonds.}, archive = {J_PRL}, author = {Yusheng Liu (刘雨生 and Liang Xu (许亮 and Xiao Chen (陈晓 and Ning Huang (黄宁 and Mengmeng Ma (马蒙蒙 and Huiqiu Wang (王挥遒 and Bin Song (宋斌 and Tao Cheng (程涛 and Fei Wei (魏飞 and Boyuan Shen (申博渊}, doi = {10.1103/sd72-g4t8}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {183001}, shortjournal = {Phys. Rev. Lett.}, title = {Atomic real-space imaging of molecular statics and dynamics at confined states}, volume = {135}, year = {2025}, }
• (2025). Measurement of F19(p,αγ)O16 reaction reopens the fluorine conundrums in stars. PRL, 135(18), 182701. (www)

  @article{ , abstract = {Fluorine abundance in stars is a sensitive indicator of the physical conditions and processes occurring within their interiors. Recent extrapolated results on the fluorine destruction cross section suggested an increase of the astrophysical factor by several orders of magnitude at astrophysical energies, with profound implications for our understanding of stellar evolution and nucleosynthesis. We have indirectly measured the cross section using the Trojan horse method, fully covering astrophysical energies with no need of extrapolations. The strength of the 11 keV resonance was extracted and a significant reduction of the reaction rate was determined, compared to previous studies. The analysis of the astrophysical impact suggests that our measurement challenges existing predictions about fluorine and heavier elements’ abundances, reigniting unresolved questions in the field.}, archive = {J_PRL}, author = {X. D. Su and M. La Cognata and N. Vukman and G. G. Rapisarda and M. Mazzocco and A. A. Oliva and L. Roberti and G. L. Zhang and B. Becherini and S. Cherubini and M. Costa and A. Di Pietro and P. Figuera and G. L. Guardo and M. Gulino and S. Hayakawa and I. Indelicato and M. La Commara and L. Lamia and D. Lattuada and S. Palmerini and R. G. Pizzone and S. M. R. Puglia and S. Romano and M. L. Sergi and R. Spartà and C. Spitaleri and D. Torresi and O. Trippella and A. Tumino}, doi = {10.1103/cq71-jy7s}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {182701}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of F19(p,αγ)O16 reaction reopens the fluorine conundrums in stars}, volume = {135}, year = {2025}, }
• (2025). Revealing the harmonic structure of nuclear two-body correlations in high-energy heavy-ion collisions. PRL, 135(18), 182301. (www)

  @article{ , abstract = {Smashing nuclei at ultrarelativistic speeds and analyzing the momentum distribution of outgoing debris provides a powerful method to probe the many-body properties of the incoming nuclear ground states. Within a perturbative description of initial-state fluctuations in the quark-gluon plasma, we express the measurement of anisotropic flow in ultracentral heavy-ion collisions as the quantum-mechanical average of a specific set of operators measuring the harmonic structure of the two-body azimuthal correlations among nucleons in the colliding states. These observables shed a new light on spatial correlations in atomic nuclei while enabling us to test the complementary pictures of nuclear structure delivered by low- and high-energy experiments on the basis of state-of-the-art theoretical approaches rooted in quantum chromodynamics.}, archive = {J_PRL}, author = {Thomas Duguet and Giuliano Giacalone and Sangyong Jeon and Alexander Tichai}, doi = {10.1103/v2z7-wlnr}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {182301}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing the harmonic structure of nuclear two-body correlations in high-energy heavy-ion collisions}, volume = {135}, year = {2025}, }
• (2025). LHC as an axion-photon collider. PRL, 135(18), 181801. (www)

  @article{ , abstract = {Assuming the existence of an axionlike particle (ALP), beams of relativistic particles emit fluxes of quasireal ALPs, analogous to the photon fluxes described by Weizsäcker-Williams-type approximations. Consequently, ALP-ALP and ALP-photon collisions can occur at the LHC. We initiate the study of the LHC as an ALP collider, and show that ALP collisions provide competitive probes of certain ALP couplings. We show that ALP fluxes from heavy ions are suppressed relative to those from protons, unlike their photon counterpart. As a result, the most likely processes are ALP-photon collisions occurring in the proton-ion ( ) ultraperipheral collisions. Using our implementation of ALP fluxes in simulation tools, we show that ALP-photon collisions in efficiently probe ALP couplings to third generation fermions. LHC data with realistic luminosity can constrain the product of ALP couplings to nucleons and top quarks at the level of . Notably, ALP-photon collisions naturally provide the leading probe of ALP flavor-violating couplings to the top quark. We suggest that the 2016 dataset collected at CMS, ATLAS, and LHCb should be explored for evidence of such collisions.}, archive = {J_PRL}, author = {Sergio Barbosa and Matheus Coelho and Sylvain Fichet and Gustavo Gil da Silveira and Magno Machado}, doi = {10.1103/t1rl-4926}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181801}, shortjournal = {Phys. Rev. Lett.}, title = {LHC as an axion-photon collider}, volume = {135}, year = {2025}, }
• (2025). Diagrammatic derivation of hidden zeros and exact factorization of pion scattering amplitudes. PRL, 135(18), 181601. (www)

  @article{ , abstract = {Pion scattering amplitudes were recently found to vanish on specific kinematic loci, and to factorize close to these loci into a product of two lower-point amplitudes of an extended theory. We propose a diagrammatic representation of pion amplitudes that makes their vanishing on the loci manifest diagram by diagram. Moreover, we provide evidence that there is a closed-form expression for the amplitudes that generalizes the near-zero factorization in an exact manner, not only close to the loci but for all kinematic configurations. Our approach crucially relies on a novel formulation of the effective field theory of pions, in which tree-level scattering amplitudes are extracted from classical field equations for a set of covariantly conserved currents and emergent composite gauge fields.}, archive = {J_PRL}, author = {Yang Li (李阳 and Tianzhi Wang (王天志 and Tomáš Brauner and Diederik Roest}, doi = {10.1103/1krs-lfqv}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181601}, shortjournal = {Phys. Rev. Lett.}, title = {Diagrammatic derivation of hidden zeros and exact factorization of pion scattering amplitudes}, volume = {135}, year = {2025}, }
• (2025). Kerr black hole in a uniform bertotti-robinson magnetic field: An exact solution. PRL, 135(18), 181401. (www)

  @article{ , abstract = {A new class of exact spacetimes in Einstein’s gravity, which are Kerr black holes immersed in an external uniform magnetic (or electric) field that is oriented along the rotational axis, is presented. These are axisymmetric stationary solutions to the Einstein-Maxwell equations such that (unlike in the Plebański-Demiański spacetime) the null directions of the Faraday tensor are not aligned with either of the two principal null directions of the Weyl tensor of algebraic type D (unlike the Kerr-Melvin spacetime). Three physical parameters are the black hole mass m , its rotation a , and the external field value B . For vanishing B the metric directly reduces to standard Boyer-Lindquist form of the Kerr black hole, while for zero m we recover a conformally flat Bertotti-Robinson universe with a uniform Maxwell field. For zero a , the spacetime is contained in the Van den Bergh–Carminati solutions which can be understood as the Schwarzschild black hole in a magnetic field. Our family of black holes with nonaligned Maxwell hair—that can be called the Kerr-Bertotti-Robinson black holes—may find application in various studies ranging from mathematical relativity to relativistic astrophysics.}, archive = {J_PRL}, author = {Jiří Podolský and Hryhorii Ovcharenko}, doi = {10.1103/rfgv-ybz5}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181401}, shortjournal = {Phys. Rev. Lett.}, title = {Kerr black hole in a uniform bertotti-robinson magnetic field: An exact solution}, volume = {135}, year = {2025}, }
• (2025). All-sky search for individual primordial black hole bursts with LHAASO. PRL, 135(18), 181005. (www)

  @article{ , abstract = {Primordial black holes (PBHs) are hypothetical black holes with a wide range of masses that formed in the early Universe. As a result, they may play an important cosmological role and provide a unique probe of the early Universe. A PBH with an initial mass of approximately is expected to explode today in a final burst of Hawking radiation. In this Letter, we conduct an all-sky search for individual PBH burst events using the data collected from March 2021 to July 2024 by the Water Cherenkov Detector Array of the Large High Altitude Air Shower Observatory (LHAASO). Three PBH burst durations, 10, 20, and 100 s, are searched in the gamma-ray energy range from about 1 to 15 TeV, with no significant PBH bursts observed. The upper limit on the local PBH burst rate density is set to be as low as at 99% confidence level, representing the most stringent limit achieved to date.}, archive = {J_PRL}, author = {LHAASO Collaboration and Zhen Cao and F. Aharonian and Y. X. Bai and Y. W. Bao and D. Bastieri and X. J. Bi and Y. J. Bi and W. Bian and A. V. Bukevich and C. M. Cai and W. Y. Cao and Zhe Cao and J. Chang and J. F. Chang and A. M. Chen and E. S. Chen and G. H. Chen and H. X. Chen and Liang Chen and Long Chen and M. J. Chen and M. L. Chen and Q. H. Chen and S. Chen and S. H. Chen and S. Z. Chen and T. L. Chen and X. B. Chen and X. J. Chen and Y. Chen and N. Cheng and Y. D. Cheng and M. C. Chu and M. Y. Cui and S. W. Cui and X. H. Cui and Y. D. Cui and B. Z. Dai and H. L. Dai and Z. G. Dai and Danzengluobu and Y. X. Diao and X. Q. Dong and K. K. Duan and J. H. Fan and Y. Z. Fan and J. Fang and J. H. Fang and K. Fang and C. F. Feng and H. Feng and L. Feng and S. H. Feng and X. T. Feng and Y. Feng and Y. L. Feng and S. Gabici and B. Gao and C. D. Gao and Q. Gao and W. Gao and W. K. Gao and M. M. Ge and T. T. Ge and L. S. Geng and G. Giacinti and G. H. Gong and Q. B. Gou and M. H. Gu and F. L. Guo and J. Guo and X. L. Guo and Y. Q. Guo and Y. Y. Guo and Y. A. Han and O. A. Hannuksela and M. Hasan and H. H. He and H. N. He and J. Y. He and X. Y. He and Y. He and S. Hernández-Cadena and B. W. Hou and C. Hou and X. Hou and H. B. Hu and S. C. Hu and C. Huang and D. H. Huang and J. J. Huang and T. Q. Huang and W. J. Huang and X. T. Huang and X. Y. Huang and Y. Huang and Y. Y. Huang and X. L. Ji and H. Y. Jia and K. Jia and H. B. Jiang and K. Jiang and X. W. Jiang and Z. J. Jiang and M. Jin and S. Kaci and M. M. Kang and I. Karpikov and D. Khangulyan and D. Kuleshov and K. Kurinov and B. B. Li and Cheng Li and Cong Li and D. Li and F. Li and H. B. Li and H. C. Li and Jian Li and Jie Li and K. Li and L. Li and R. L. Li and S. D. Li and T. Y. Li and W. L. Li and X. R. Li and Xin Li and Y. Li and Y. Z. Li and Zhe Li and Zhuo Li and E. W. Liang and Y. F. Liang and S. J. Lin and B. Liu and C. Liu and D. Liu and D. B. Liu and H. Liu and H. D. Liu and J. Liu and J. L. Liu and J. R. Liu and M. Y. Liu and R. Y. Liu and S. M. Liu and W. Liu and X. Liu and Y. Liu and Y. N. Liu and Y. Q. Lou and Q. Luo and Y. Luo and H. K. Lv and B. Q. Ma and L. L. Ma and X. H. Ma and J. R. Mao and Z. Min and W. Mitthumsiri and G. B. Mou and H. J. Mu and A. Neronov and K. C. Y. Ng and M. Y. Ni and L. Nie and L. J. Ou and P. Pattarakijwanich and Z. Y. Pei and J. C. Qi and M. Y. Qi and J. J. Qin and A. Raza and C. Y. Ren and D. Ruffolo and A. Sáiz and D. Semikoz and L. Shao and O. Shchegolev and Y. Z. Shen and X. D. Sheng and Z. D. Shi and F. W. Shu and H. C. Song and Yu. V. Stenkin and V. Stepanov and Y. Su and D. X. Sun and H. Sun and Q. N. Sun and X. N. Sun and Z. B. Sun and N. H. Tabasam and J. Takata and P. H. T. Tam and H. B. Tan and Q. W. Tang and R. Tang and Z. B. Tang and W. W. Tian and C. N. Tong and L. H. Wan and C. Wang and G. W. Wang and H. G. Wang and J. C. Wang and K. Wang and Kai Wang and L. P. Wang and L. Y. Wang and R. Wang and W. Wang and X. G. Wang and X. J. Wang and X. Y. Wang and Y. Wang and Y. D. Wang and Z. H. Wang and Z. X. Wang and Zheng Wang and D. M. Wei and J. J. Wei and Y. J. Wei and T. Wen and S. S. Weng and C. Y. Wu and H. R. Wu and Q. W. Wu and S. Wu and X. F. Wu and Y. S. Wu and S. Q. Xi and J. Xia and J. J. Xia and G. M. Xiang and D. X. Xiao and G. Xiao and Y. L. Xin and Y. Xing and D. R. Xiong and Z. Xiong and D. L. Xu and R. F. Xu and R. X. Xu and W. L. Xu and L. Xue and D. H. Yan and T. Yan and C. W. Yang and C. Y. Yang and F. F. Yang and L. L. Yang and M. J. Yang and R. Z. Yang and W. X. Yang and Z. H. Yang and Z. G. Yao and X. A. Ye and L. Q. Yin and N. Yin and X. H. You and Z. Y. You and Q. Yuan and H. Yue and H. D. Zeng and T. X. Zeng and W. Zeng and X. T. Zeng and M. Zha and B. B. Zhang and B. T. Zhang and C. Zhang and F. Zhang and H. Zhang and H. M. Zhang and H. Y. Zhang and J. L. Zhang and Li Zhang and P. F. Zhang and P. P. Zhang and R. Zhang and S. R. Zhang and S. S. Zhang and W. Y. Zhang and X. Zhang and X. P. Zhang and Yi Zhang and Yong Zhang and Z. P. Zhang and J. Zhao and L. Zhao and L. Z. Zhao and S. P. Zhao and X. H. Zhao and Z. H. Zhao and F. Zheng and W. J. Zhong and B. Zhou and H. Zhou and J. N. Zhou and M. Zhou and P. Zhou and R. Zhou and X. X. Zhou and B. Y. Zhu and C. G. Zhu and F. R. Zhu and H. Zhu and K. J. Zhu and Y. C. Zou and X. Zuo and S. Wang and Xin Zhang}, doi = {10.1103/nkby-9cs3}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181005}, shortjournal = {Phys. Rev. Lett.}, title = {All-sky search for individual primordial black hole bursts with LHAASO}, volume = {135}, year = {2025}, }
• (2025). Scalable architecture for dark photon searches: Superconducting-qubit proof of principle. PRL, 135(18), 181004. (www)

  @article{ , abstract = {The dark photon is a well-motivated dark matter candidate that appears in many extensions of the standard model. A fundamental mass-range-sensitivity dilemma is always haunting the dark photon search experiments: resonant haloscopes have excellent sensitivity but are narrowband, while nonresonant haloscopes are broadband but not as sensitive as the resonant ones. A scalable architecture integrating numerous resonant haloscopes would be a desirable solution to this dilemma. However, even the concept of a scalable search remains rarely explored due to the size limitation of conventional haloscopes imposed by the dark photon wavelength. Here, we propose and demonstrate a novel architecture using superconducting qubits as subwavelength haloscope units. By virtue of the scalability of superconducting qubits, it is possible to integrate multiple qubits with different frequencies on a chip-scale device. Furthermore, the frequencies of the qubits can be tuned to extend the search mass range. Thus, our scalable architectures allow for sweepable high-sensitivity dark photon searches at multiple frequencies simultaneously. As a proof-of-principle experiment, we designed and fabricated a three-qubit chip and successfully demonstrated a scalable dark-photon search. Our Letter established constraints on dark photons in the mass range of 15.632–15.638, 15.838–15.845, and , simultaneously, and the constraints are much more stringent than the cosmology constraints. In the future, our Letter can be scaled up to boost the scrutiny of new physics.}, archive = {J_PRL}, author = {Runqi Kang and Qingqin Hu and Xiao Cai and Wenlong Yu and Jingwei Zhou and Xing Rong and Jiangfeng Du}, doi = {10.1103/9p1t-vc9j}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181004}, shortjournal = {Phys. Rev. Lett.}, title = {Scalable architecture for dark photon searches: Superconducting-qubit proof of principle}, volume = {135}, year = {2025}, }
• (2025). Current constraints on cosmological scenarios with very low reheating temperatures. PRL, 135(18), 181003. (www)

  @article{ , abstract = {We present a comprehensive analysis of the effects of models with very low reheating scenarios [ ] on the cosmological observables and derive corresponding bounds on the reheating temperature. With respect to previous work, our Letter includes a more precise computation of neutrino distribution functions, leveraging the latest datasets from cosmological surveys. We perform a joint analysis that combines constraints from big bang nucleosynthesis, the cosmic microwave background, and galaxy surveys, alongside separate investigations of these datasets, carefully assessing the impact of different choices of priors. At the 95% confidence level, we establish a lower bound on the reheating temperature of , representing the most stringent constraint to date.}, archive = {J_PRL}, author = {Nicola Barbieri and Thejs Brinckmann and Stefano Gariazzo and Massimiliano Lattanzi and Sergio Pastor and Ofelia Pisanti}, doi = {10.1103/j5rj-dz1k}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181003}, shortjournal = {Phys. Rev. Lett.}, title = {Current constraints on cosmological scenarios with very low reheating temperatures}, volume = {135}, year = {2025}, }
• (2025). Probing a new regime of neutrino self-interactions with astrophysical neutrinos and the relativistic cosmic neutrino background. PRL, 135(18), 181002. (www)

  @article{ , abstract = {Neutrino self-interactions beyond the standard model have profound implications in astrophysics and cosmology. In this Letter, we study an uncharted scenario in which one of the three neutrino species has a mass smaller than the temperature of the cosmic neutrino background. This results in a relativistic component that significantly broadens the absorption feature on the astrophysical neutrino spectra, in contrast to the sharply peaked absorption expected in the extensively studied scenarios assuming a fully nonrelativistic cosmic neutrino background. By solving the Boltzmann equations for neutrino absorption and regeneration, we demonstrate that this mechanism provides novel sensitivity to sub-keV mediator masses, well below the traditional range. Future observations of the diffuse supernova neutrino background with Hyper-Kamiokande could probe coupling strengths down to , surpassing existing constraints by orders of magnitude. These findings open new directions for discoveries and offer crucial insights into the interplay between neutrinos and the dark sector.}, archive = {J_PRL}, author = {Isaac R. Wang and Xun-Jie Xu and Bei Zhou}, doi = {10.1103/9ddp-j1z9}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181002}, shortjournal = {Phys. Rev. Lett.}, title = {Probing a new regime of neutrino self-interactions with astrophysical neutrinos and the relativistic cosmic neutrino background}, volume = {135}, year = {2025}, }
• (2025). Apparent w<−1 and a lower s8 from dark axion and dark baryons interactions. PRL, 135(18), 181001. (www)

  @article{ , abstract = {We show that a simple coupling between dark energy and dark matter can simultaneously address two distinct hints at new physics coming from cosmological observations. The first is the recent evidence from the DESI project and supernovae observations that the dark energy equation of state is evolving over cosmic time from an earlier value that is to a present-day value . The second observation is the so-called tension, describing the suppression of the growth of matter overdensities compared to that expected in the model. We propose a stable, technically natural particle physics implementation of this idea, in which dark matter consists of dark baryons in a strongly coupled hidden sector, and the dark energy field is the associated dark axion. The time variation of the dark matter mass results in an effective dark energy equation of state that exhibits a phantom crossing behavior consistent with recent results. It also results in a slight delay in matter-radiation equality, which suppresses the overall growth of density perturbations.}, archive = {J_PRL}, author = {Justin Khoury and Meng-Xiang Lin and Mark Trodden}, doi = {10.1103/w4qb-plk8}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {181001}, shortjournal = {Phys. Rev. Lett.}, title = {Apparent w<−1 and a lower s8 from dark axion and dark baryons interactions}, volume = {135}, year = {2025}, }
• (2025). Frequency-noise-insensitive universal control of kerr-cat qubits. PRL, 135(18), 180801. (www)

  @article{ , abstract = {We theoretically study the influence of frequency uncertainties on the operation of a Kerr-cat qubit. As the mean photon number increases, Kerr-cat qubits provide an increasing level of protection against phase errors induced by unknown frequency shifts during idling and rotations. However, realizing rotations about the other principal axes (e.g., and axes) while preserving robustness is nontrivial. To address this challenge, we propose a universal set of gate schemes which circumvents the trade-off between protection and controllability in Kerr-cat qubits and retains robustness to unknown frequency shifts to at least first order. Assuming an effective Kerr oscillator model, we theoretically and numerically analyze the robustness of elementary gates on Kerr-cat qubits, with special focus on gates along nontrivial rotation axes. An appealing application of this qubit design would include tunable superconducting platforms, where the induced protection against frequency noise would allow for a more flexible choice of operating point and thus the potential mitigation of the impact of spurious two-level systems.}, archive = {J_PRL}, author = {Lennart Maximilian Seifert and Connor T. Hann and Kyungjoo Noh}, doi = {10.1103/fyft-6kqg}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {180801}, shortjournal = {Phys. Rev. Lett.}, title = {Frequency-noise-insensitive universal control of kerr-cat qubits}, volume = {135}, year = {2025}, }
• (2025). Offset charge dependence of measurement-induced transitions in transmons. PRL, 135(18), 180603. (www)

  @article{ , abstract = {A key challenge in achieving scalable fault tolerance in superconducting quantum processors is readout fidelity, which lags behind one- and two-qubit gate fidelity. A major limitation in improving qubit readout is measurement-induced transitions, also referred to as qubit ionization, caused by multiphoton qubit-resonator excitation occurring at specific photon numbers. Since ionization can involve highly excited states, it has been predicted that in transmons—the most widely used superconducting qubit—the photon number at which measurement-induced transitions occur is gate-charge dependent. This dependence is expected to persist deep in the transmon regime where the qubit frequency is gate-charge insensitive. We experimentally confirm this prediction by characterizing measurement-induced transitions with increasing resonator photon population while actively calibrating the transmon’s gate charge. Furthermore, because highly excited states are involved, achieving quantitative agreement between theory and experiment requires accounting for higher-order harmonics in the transmon Hamiltonian.}, archive = {J_PRL}, author = {Mathieu Féchant and Marie Frédérique Dumas and Denis Bénâtre and Nicolas Gosling and Philipp Lenhard and Martin Spiecker and Simon Geisert and Sören Ihssen and Wolfgang Wernsdorfer and Benjamin D’Anjou and Alexandre Blais and Ioan M. Pop}, doi = {10.1103/yljv-b4kj}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {180603}, shortjournal = {Phys. Rev. Lett.}, title = {Offset charge dependence of measurement-induced transitions in transmons}, volume = {135}, year = {2025}, }
• (2025). Counterdiabatic driving with performance guarantees. PRL, 135(18), 180602. (www)

  @article{ , abstract = {Counterdiabatic (CD) driving has the potential to speed up adiabatic quantum state preparation by suppressing unwanted excitations. However, existing approaches either require intractable classical computations or are based on approximations that do not have performance guarantees. We propose and analyze a nonvariational, system-agnostic CD expansion method and analytically show that it converges exponentially quickly in the expansion order. In finite systems, the required resources scale inversely with the spectral gap, which we argue is asymptotically optimal. To extend our method to the thermodynamic limit and suppress errors stemming from high-frequency transitions, we leverage finite-time adiabatic protocols. In particular, we show that a time determined by the quantum speed limit is sufficient to prepare the desired ground state, without the need to optimize the adiabatic trajectory. Numerical tests of our method on the quantum Ising chain show that our method can outperform state-of-the-art variational CD approaches.}, archive = {J_PRL}, author = {Jernej Rudi Finžgar and Simone Notarnicola and Madelyn Cain and Mikhail D. Lukin and Dries Sels}, doi = {10.1103/pqhl-nbtk}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {180602}, shortjournal = {Phys. Rev. Lett.}, title = {Counterdiabatic driving with performance guarantees}, volume = {135}, year = {2025}, }
• (2025). Nonequilibrium thermodynamics of precision through a quantum-centric computation. PRL, 135(18), 180601. (www)

  @article{ , abstract = {Thermodynamic uncertainty relations (TURs) are a set of inequalities expressing a fundamental trade-off between precision and dissipation in nonequilibrium classical and quantum thermodynamic processes. TURs show that achieving low fluctuations in a thermodynamic quantity (e.g., heat or work) requires a minimum entropy production, with profound implications for the efficiency of biological and artificial thermodynamic processes. The accurate evaluation of TURs is a necessary requirement to quantify the fluctuation and dissipation entailed by a thermodynamic process, and ultimately to optimize the performance of quantum devices, whose operation is fundamentally a quantum thermodynamic process. Here, we simulate TURs in a transverse-field Ising model subjected to a time-dependent driving protocol, using quantum and classical computers in concert. Varying the duration and strength of the drive as well as the system size, we verify the validity of TURs, identify quantum signatures in the work statistics within the linear response regime, and observe TUR saturation in the high-temperature limit.}, archive = {J_PRL}, author = {Mario Motta and Antonio Mezzacapo and Giacomo Guarnieri}, doi = {10.1103/nrzn-h5ph}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {180601}, shortjournal = {Phys. Rev. Lett.}, title = {Nonequilibrium thermodynamics of precision through a quantum-centric computation}, volume = {135}, year = {2025}, }
• (2025). Liouvillian spectral transition in noisy quantum many-body scars. PRL, 135(18), 180401. (www)

  @article{ , abstract = {Understanding the behavior of quantum many-body systems under decoherence is essential for developing robust quantum technologies. Here, we examine the fate of weak ergodicity breaking in systems hosting quantum many-body scars when subject to local pure dephasing—an experimentally relevant form of environmental noise. Focusing on a large class of models with an approximate su(2)-structured scar subspace, we show that scarred eigenmodes of the Liouvillian exhibit a transition reminiscent of spontaneous -symmetry breaking as the dephasing strength increases. Unlike previously studied non-Hermitian mechanisms, this transition arises from a distinct quantum jump effect. Remarkably, in platforms such as the XY spin ladder and PXP model of Rydberg atom arrays, the critical dephasing rate shows only weak dependence on the system size, revealing an unexpected robustness of scarred dynamics in noisy environments.}, archive = {J_PRL}, author = {Jin-Lou Ma and Zexian Guo and Yu Gao and Zlatko Papić and Lei Ying}, doi = {10.1103/4my3-vk6c}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {180401}, shortjournal = {Phys. Rev. Lett.}, title = {Liouvillian spectral transition in noisy quantum many-body scars}, volume = {135}, year = {2025}, }
• (2025). Partial independence suffices to rule out real quantum theory experimentally. PRL, 135(18), 180201. (www)

  @article{ , abstract = {The role of complex quantities in quantum theory has been puzzling physicists since the beginnings. It is, thus, natural to ask whether, in order to describe our experiments, the mathematical structure of the complex Hilbert spaces it is built on is really necessary. Recently, it was shown that this structure is inevitable in network scenarios with independent sources. More precisely, Real Quantum Theory cannot explain the predictions of (Complex) Quantum Theory [Renou et al. , Nature (London) 600 , 625 (2021) .]. Here, we revisit the independence assumption underlying this work. We show that assuming partial independence is sufficient for showing the inadequacy of Real Quantum Theory. We derive a tradeoff between source independence and the Bell value achievable in Real Quantum Theory, which also lower bounds the source correlations required to explain previous experiments by means of real quantum systems. We further show that 1 bit of entanglement is necessary and sufficient for recovering the complex quantum correlations by means of Real Quantum Theory in the scenario from [Renou et al. , Nature (London) 600 , 625 (2021) .]. Finally, building on [McKague et al. , Phys. Rev. Lett. 102, 2009 ], we provide a construction to simulate any complex quantum setup with independent sources by means of Real Quantum Theory by allowing the sources to share an real-qubit entangled state in the first round of the experiment.}, archive = {J_PRL}, author = {Mirjam Weilenmann and Nicolas Gisin and Pavel Sekatski}, doi = {10.1103/3fv7-p8cs}, journal = {Physical Review Letters}, month = {10}, number = {18}, pages = {180201}, shortjournal = {Phys. Rev. Lett.}, title = {Partial independence suffices to rule out real quantum theory experimentally}, volume = {135}, year = {2025}, }
• (2025). Flocking phase separation in inertial active matter. PRL, 135(17), 178301. (www)

  @article{ , abstract = {A large population of motile agents can display remarkable collective behaviors. Here, we study collective motion of inertia-dominated macroscopic agents using a model system of millimeter-sized magnetic rollers with tunable motile behaviors. In this system, we observe first-order flocking phase separation, where a uniform flock propagates through an isotropic gaseous phase. The flocking phase and the coexisting gaseous phase exhibit distinct particle exchange dynamics and maintain different effective temperatures, which are unattainable in equilibrium systems. Combining experiments, agent-based simulations, and phenomenological theories, we demonstrate that inelastic collisions between inertial and externally driven magnetic rollers produce positive feedback between high density and polar motion, driving flocking phase separation. Our Letter reveals a novel mode of collective motion in inertial active matter, with potential implications for controlling biological flocks and designing robotic swarms.}, archive = {J_PRL}, author = {Nan Luo and Longfei Li and Mingcheng Yang and Yi Peng}, doi = {10.1103/hb7b-wp95}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {178301}, shortjournal = {Phys. Rev. Lett.}, title = {Flocking phase separation in inertial active matter}, volume = {135}, year = {2025}, }
• (2025). Observing the glass and jamming transitions of dense granular material in microgravity. PRL, 135(17), 178203. (www)

  @article{ , abstract = {The present Letter investigates a weakly pulsed granular system of polystyrene spheres under longtime microgravity conditions on the International Space Station. The spheres are measured using diffusing wave spectroscopy (DWS) and are described by mean square displacements (MSDs). Our aim is to use this technique to provide the first experimental evidence for glassy dynamics in dense granular media in microgravity and subsequently compare these results with ground-based measurements to see how the nature of these dynamics changes without the influence of gravity. Our results show that as we densify the sample in microgravity, glassy dynamics appear at a volume fraction 1.6% lower than on ground. We also show how the influence of gravity can affect how dense a granular system one can prepare by comparing the final jamming point of our sample on the ISS compared to our ground setup. We show that jamming occurs at a volume fraction 0.5% lower in space compared to on ground, showing that we can create denser states when a granular system is in the presence of a stronger gravitational field.}, archive = {J_PRL}, author = {Christopher Mayo and Marlo Kunzner and Matthias Sperl and Jan Philipp Gabriel}, doi = {10.1103/z161-sd1y}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {178203}, shortjournal = {Phys. Rev. Lett.}, title = {Observing the glass and jamming transitions of dense granular material in microgravity}, volume = {135}, year = {2025}, }
• (2025). Disentangling the effects of curvature and misorientation on the shrinkage behavior of loop-shaped grain boundaries. PRL, 135(17), 178202. (www)

  @article{ , abstract = {The material properties of polycrystals are strongly affected by the evolution and coarsening of their internal grain structures. Yet, studying this process is challenging due to the complex interactions within grain boundary networks. Here, we systematically investigate the shrinkage of isolated loop-shaped grain boundaries in 2D colloidal crystals using a combination of simulations and experiments. Unexpectedly, we find that shear coupling decreases with increasing grain misorientation, contrary to geometric predictions. This counterintuitive result is attributed to enhanced concurrent sliding driven by the annihilation of dislocations. Furthermore, by focusing on the evolution of the grain size, we reveal a transition in shrinkage kinetics between small and large loop sizes, providing an explanation for previously observed discrepancies in grain boundary mobility. These findings reveal a more intricate dependence of grain boundary behavior on curvature and misorientation than previously reported, offering new insights into polycrystal coarsening dynamics.}, archive = {J_PRL}, author = {Fabrizio Camerin and Susana Marín-Aguilar and Tim Griffioen and Mathieu G. Baltussen and Roel P. A. Dullens and Berend van der Meer and Marjolein Dijkstra}, doi = {10.1103/krvx-hbt3}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {178202}, shortjournal = {Phys. Rev. Lett.}, title = {Disentangling the effects of curvature and misorientation on the shrinkage behavior of loop-shaped grain boundaries}, volume = {135}, year = {2025}, }
• (2025). Facilitating a 3D granular flow with an obstruction. PRL, 135(17), 178201. (www)

  @article{ , abstract = {Ensuring a smooth rate of efflux of particles from an outlet without unpredictable clogging events is crucial in processing powders and grains. We show by experiments and simulations that an obstacle placed near the outlet can greatly suppress clog formation in a 3-dimensional granular flow; this counterintuitive phenomenon had previously been demonstrated in 2-dimensional systems. Remarkably, clog suppression is very effective even when the obstacle cross section is comparable to that of a single grain and is only a small fraction of the outlet area. Data from two dissimilar obstacle shapes indicate that the underlying mechanism for clog suppression is geometric: while the magnitude of the effect can be affected by dynamical factors, the optimal location of the obstacle is not and follows a simple geometric rule. An optimally placed obstacle arranges for the most probable clogging arch to be at a perilous and unstable spot, where the flow geometry is at a point of local expansion and a slight perturbation leaves the arch without downstream support. This geometric principle does not rely on previously conjectured dynamical mechanisms and admits generalization to other agent-based and particulate systems.}, archive = {J_PRL}, author = {Abhijit Sinha and Jackson Diodati and Narayanan Menon and Shubha Tewari and Shankar Ghosh}, doi = {10.1103/4152-s64f}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {178201}, shortjournal = {Phys. Rev. Lett.}, title = {Facilitating a 3D granular flow with an obstruction}, volume = {135}, year = {2025}, }
• (2025). Machine-learning interatomic potentials for long-range systems. PRL, 135(17), 178001. (www)

  @article{ , abstract = {Machine-learning interatomic potentials have emerged as a revolutionary class of force-field models in molecular simulations, delivering quantum-mechanical accuracy at a fraction of the computational cost and enabling the simulation of large-scale systems over extended timescales. However, they often focus on modeling local environments, neglecting crucial long-range interactions. We propose a sum-of-Gaussians neural network (SOG-Net), a lightweight and versatile framework for integrating long-range interactions into a machine-learning force field. The SOG-Net employs a latent-variable learning network that seamlessly bridges short-range and long-range components, coupled with an efficient Fourier convolution layer that incorporates long-range effects. By learning sum-of-Gaussians multipliers across different convolution layers, the SOG-Net adaptively captures diverse long-range decay behaviors while maintaining close-to-linear computational complexity during training and simulation via nonuniform fast Fourier transforms. The method is demonstrated effective for a broad range of long-range systems.}, archive = {J_PRL}, author = {Yajie Ji and Jiuyang Liang and Zhenli Xu}, doi = {10.1103/ssp9-7s81}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {178001}, shortjournal = {Phys. Rev. Lett.}, title = {Machine-learning interatomic potentials for long-range systems}, volume = {135}, year = {2025}, }
• (2025). Fully flat bands in a photonic dipolar kagome lattice. PRL, 135(17), 176902. (www)

  @article{ , abstract = {Flat bands, characterized by zero group velocity and strong energy localization, enable interaction-enhanced phenomena across both quantum and classical systems. Existing photonic flat-band implementations were limited to evanescent-wave systems, specific lattice symmetries, or complex supercell modulations. A simple, universal, and efficient approach to realizing flat bands without dedicated source excitation is yet to be explored. Here, inspired by geometrically frustrated configurations, we theoretically proposed and experimentally demonstrated threefold-degenerate flat bands by integrating orbital and rotational degrees of freedom in a photonic dipolar kagome lattice. By rotating the dipole orientation, the system exhibits a band flip transition at which point all bands achieve complete flatness and degeneracy across the entire Brillouin zone. In contrast to conventional -orbital kagome lattices with only a single flat band, our approach flattens the entire band structure, eliminating dispersive modes and enabling compatibility with arbitrary excitations. These results establish a new mechanism for flat-band engineering, offering a tunable strategy for enhancing light-matter interactions and may have applications in compact photonic devices and energy-efficient information processing.}, archive = {J_PRL}, author = {Han-Rong Xia and Ziyao Wang and Yunrui Wang and Zhen Gao and Meng Xiao}, doi = {10.1103/bt9s-qsfj}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176902}, shortjournal = {Phys. Rev. Lett.}, title = {Fully flat bands in a photonic dipolar kagome lattice}, volume = {135}, year = {2025}, }
• (2025). Spin-orbital altermagnetism. PRL, 135(17), 176705. (www)

  @article{ , abstract = {Altermagnetism is a newly discovered magnetic phase, characterized by nonrelativistic spin splitting that has been experimentally observed. Here, we introduce a framework dubbed “spin-orbital altermagnetism” to achieve spin-orbital textures in altermagnetic materials. We identify two distinct classes of spin-orbital altermagnetism: intrinsic and extrinsic. The intrinsic type emerges from symmetry-compensated magnetic orders with spontaneously broken parity-time symmetry, while the extrinsic type stems from translational symmetry breaking between sublattices, as exemplified by the Jahn-Teller-driven structural phase transition. In addition to directly measuring the spin-orbital texture, we propose spin conductivity and spin-resolved orbital polarization as effective methods for detecting these altermagnets. Additionally, a symmetry-breaking mechanism induces weak spin magnetization, further revealing the peculiar feature of spin-orbital altermagnetism. We also utilize the staggered susceptibility to illustrate a potential realization of this phase in a two-orbital interacting system. Our Letter provides a new platform to explore spin-orbital locked physics, extending the materials classes that may display complex spin textures from the standard 4 d − 5 d compounds to 3 d compounds.}, archive = {J_PRL}, author = {Zi-Ming Wang and Yang Zhang and Song-Bo Zhang and Jin-Hua Sun and Elbio Dagotto and Dong-Hui Xu and Lun-Hui Hu}, doi = {10.1103/cjzw-j4v7}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176705}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-orbital altermagnetism}, volume = {135}, year = {2025}, }
• (2025). Symmetry-forbidden intraband transitions leading to ultralow gilbert damping in van der waals ferromagnets. PRL, 135(17), 176704. (www)

  @article{ , abstract = {Based upon first-principles calculations, we report ultralow Gilbert damping in two-dimensional (2D) van der Waals ferromagnets. The low damping occurs at weak scattering because mirror symmetry prohibits intraband transitions. The monotonic dependence on the electronic scattering rate suggests the absent lower limit, in contrast to conventional ferromagnetic materials. Breaking mirror symmetry through magnetization rotation, layer stacking, or structural phase transition significantly increases damping by enabling intraband transitions. Topological nodal lines, also protected by mirror symmetry, contribute substantially to interband-transition-mediated damping, which can be tuned by adjusting the Fermi level. Our findings elucidate the unique characteristics of Gilbert damping in 2D van der Waals ferromagnets, providing valuable insights for designing low-dimensional spintronic devices with high energy efficiency.}, archive = {J_PRL}, author = {Weizhao Chen and Yu Zhang and Yi Liu and Zhe Yuan}, doi = {10.1103/j3jy-yl42}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176704}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry-forbidden intraband transitions leading to ultralow gilbert damping in van der waals ferromagnets}, volume = {135}, year = {2025}, }
• (2025). Hallmarks of ballistic terahertz magnon currents in an antiferromagnetic insulator. PRL, 135(17), 176703. (www)

  @article{ , abstract = {Efficient transport of spin angular momentum is expected to play a crucial role in future spintronic devices, which will potentially operate at frequencies reaching the terahertz range. On the other hand, antiferromagnetic insulators exhibit significant potential for facilitating ultrafast pure spin currents by terahertz magnons. Consequently, we here use femtosecond laser pulses to trigger ultrafast spin currents across thin films of the model antiferromagnet NiO in P y ⁢ | N i O | ⁢ P t stacks, where permalloy (Py) and Pt serve as spin-current source and detector, respectively. We find that the spin-current pulses traversing NiO reach a velocity up to 4 ⁢ 0 n m / p s and experience increasing attenuation, delay, and broadening as the NiO thickness is increased. We can consistently explain our observations by ballistic transport of incoherent magnons. The relaxation length of 20 nm is 1 order of magnitude larger than for ballistic conduction-electron spin transport in metals and, thus, relevant for potential applications. Methodologically, our all-optical and contact-free spin-conductance approach has large potential to characterize terahertz magnon transport in insulators with any kind of magnetic order.}, archive = {J_PRL}, author = {Hongsong Qiu and Oliver Franke and Yuanzhe Tian and Zdeněk Kašpar and Reza Rouzegar and Oliver Gueckstock and Ji Wu and Maguang Zhu and Biaobing Jin and Yongbing Xu and Tom S. Seifert and Di Wu and Piet W. Brouwer and Tobias Kampfrath}, doi = {10.1103/mk8h-yzkj}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176703}, shortjournal = {Phys. Rev. Lett.}, title = {Hallmarks of ballistic terahertz magnon currents in an antiferromagnetic insulator}, volume = {135}, year = {2025}, }
• (2025). Exchange surface spin waves in type-A van der waals antiferromagnets. PRL, 135(17), 176702. (www)

  @article{ , abstract = {Surface waves, the evanescent solutions of the wave equation at planar discontinuities, are of fundamental importance in surface physics, optics, phononics, electronics, and magnetism. Here, we predict that van der Waals antiferromagnets support surface spin waves that are unique by their extreme (nanoscale) confinement and high group velocity with application potential in ultrafast, nanoscale magnonic devices. These excitations reside within the bulk magnon band gap of type-A van der Waals antiferromagnets (antiferromagnetically coupled ferromagnetic monolayers). In contrast to conventional magnetostatic Damon-Eshbach modes, they are pure exchange modes owing to reduced interlayer exchange coupling at the surface layers, and thus persist in ultrathin multilayer stacks and at large wave numbers. We show that they can be efficiently excited by electromagnetic waves, with absorption power comparable to or even exceeding that of bulk modes. Moreover, their emitted magnetic stray fields exhibit pronounced even-odd oscillations with the number of monolayers that should be observable by nitrogen-vacancy-center magnetometry.}, archive = {J_PRL}, author = {Zhoujian Sun and Fuxiang Li and Gerrit E. W. Bauer and Ping Tang}, doi = {10.1103/bchp-xqtn}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176702}, shortjournal = {Phys. Rev. Lett.}, title = {Exchange surface spin waves in type-A van der waals antiferromagnets}, volume = {135}, year = {2025}, }
• (2025). Design and theory of switchable linear magnetoelectricity by ferroelectricity in type-I multiferroics. PRL, 135(17), 176701. (www)

  @article{ , abstract = {We present a comprehensive theoretical investigation of magnetoelectric (ME) coupling mechanisms in 19 altermagnetic and 4 ferrimagnetic type-I multiferroics using electronic band structure calculations with spin-orbit coupling, a first-principles ME response framework, and spin-space-group theory analysis. We formulate a universal scheme for realizing nonvolatile ME coupling in type-I multiferroics, where two distinct pathways emerge, each dictated by spin-space symmetry. The first pathway is associated with switching of the spin splitting or the now familiar spin-momentum locking in reciprocal space, characteristic of some altermagnetic multiferroics that exhibit coexisting antiferromagnetism and ferroelectricity. The second pathway involves real-space magnetization switching via electric polarization reversal, characterized by switchable components of the linear ME tensor, despite the traditionally weak coupling in type-I systems due to the independent origins of magnetism and ferroelectricity. We demonstrate that these two intrinsic ME coupling mechanisms are mutually exclusive and propose thermodynamically stable compounds for experimentation. Our findings establish general design principles for controlling robust nonvolatile ME effects in multiferroic materials.}, archive = {J_PRL}, author = {Hui-Min Zhang and Cheng-Ao Ji and Tong Zhu and Hongjun Xiang and Hiroshi Kageyama and Shuai Dong and James M. Rondinelli and Xue-Zeng Lu}, doi = {10.1103/66zq-39yc}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176701}, shortjournal = {Phys. Rev. Lett.}, title = {Design and theory of switchable linear magnetoelectricity by ferroelectricity in type-I multiferroics}, volume = {135}, year = {2025}, }
• (2025). Photonic flat landau levels induced by antisymmetric nonuniform pseudomagnetic fields. PRL, 135(17), 176602. (www)

  @article{ , abstract = {Pseudomagnetic fields (PMFs) have been proven useful for generating Landau levels and controlling wave propagation in classical wave systems. Recently, photonic flat Landau levels residing near the and points induced by PMFs have been realized through uniaxial gradient deformations of superlattices. Here, we report the realization of flat Landau levels near the point in Dirac photonic crystals with wider-range uniaxial gradient deformations, induced by antisymmetric, nonuniform PMFs. The flat Landau levels appear as spatially localized, doubly degenerate bulk modes, and are associated with dispersive valley kink modes. The nonuniform PMF distributions provide an additional degree of freedom that can enhance the flatness of flat Landau levels that extends for an expanded -space range. We experimentally visualized the band dispersion of flat Landau levels and observed both localized flat Landau level modes and chiral valley kink modes. Our results pave a new avenue for manipulating electromagnetic wave localization and transport via PMFs.}, archive = {J_PRL}, author = {Xiao Zhang and Li Liang and Kai Shao and Feifei Li and Biaobing Jin and Huabing Wang and Yin Poo and Wei Chen and C. T. Chan}, doi = {10.1103/3l3j-tfyn}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176602}, shortjournal = {Phys. Rev. Lett.}, title = {Photonic flat landau levels induced by antisymmetric nonuniform pseudomagnetic fields}, volume = {135}, year = {2025}, }
• (2025). Observation of giant nernst plateau in ideal 1D weyl phase. PRL, 135(17), 176601. (www)

  @article{ , abstract = {The search for a giant Nernst effect beyond conventional mechanisms offers advantages for developing advanced thermoelectric devices and understanding charge-entropy conversion. Here, we study the Seebeck and Nernst effects in across a broad range of magnetic fields. Remarkably, the Nernst effect forms a giant plateau at ultrahigh magnetic fields ( ), with the magnitude reaching up to at 2 K. By tracking two magnetic-field-driven phase transitions predicted for weak topological insulators, we find that the giant Nernst plateau exists exclusively in the ideal 1D Weyl phase. Theoretical analysis further demonstrates that such a giant Nernst plateau arises from the unique thermoelectric conversion mechanism inherent to the ideal 1D Weyl phase, where the transverse thermoelectric effect (Nernst effect) is dominated by the longitudinal conduction channel. Our findings expand the understanding of ideal Weyl physics and open new avenues for significantly improving thermoelectric conversion efficiency.}, archive = {J_PRL}, author = {Y. Zhang and J. Q. Cai and Peng-Lu Zhao and Q. Li and Y. C. Qian and Y. Y. Lv and Y. B. Chen and Q. Niu and Hai-Zhou Lu and J. L. Zhang and M. L. Tian}, doi = {10.1103/4zlp-n5qm}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of giant nernst plateau in ideal 1D weyl phase}, volume = {135}, year = {2025}, }
• (2025). Variational diagrammatic monte carlo built on dynamical mean-field theory. PRL, 135(17), 176501. (www)

  @article{ , abstract = {We develop a variational perturbation expansion around dynamical mean-field theory (DMFT) that systematically incorporates nonlocal correlations beyond the local correlations treated by DMFT. We apply this approach to investigate how the DMFT critical temperature is suppressed from its mean-field value and how the critical behavior near the finite-temperature phase transition evolves from the mean-field to the Heisenberg universality class. By identifying the symmetry breaking of paramagnetic diagrammatic expansions as a signature of the Néel transition, we accurately predict the Néel temperature of the three-dimensional cubic Hubbard model across all interaction strengths with low computational cost. Introducing a variational order parameter, our method can be applied to both paramagnetic and long-range ordered states, such as antiferromagnetic order. We compute magnetization and antiferromagnetic susceptibility, demonstrating minor corrections to DMFT solutions in the weak-coupling regime while revealing significant modifications to these properties in the intermediate correlation regime. From the analysis of critical exponents, we establish the emergence of Heisenberg critical behavior beyond the mean-field nature of DMFT.}, archive = {J_PRL}, author = {Yueyi Wang and Kristjan Haule}, doi = {10.1103/dqsl-l8zz}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {176501}, shortjournal = {Phys. Rev. Lett.}, title = {Variational diagrammatic monte carlo built on dynamical mean-field theory}, volume = {135}, year = {2025}, }
• (2025). Pump with broadband probe experiments for single-shot measurements of plasma conditions and crossed-beam energy transfer. PRL, 135(17), 175103. (www)

  @article{ , abstract = {A novel technique for measuring plasma conditions using monochromatic pump-broadband-probe laser interactions has been experimentally demonstrated. Originally proposed in Ludwig et al. [ Phys. Plasmas 26 , 113108 (2019) ], this method utilizes crossed-beam energy transfer between the broadband probe and the pump, mediated by plasma ion acoustic waves. The complete energy transfer spectrum can be captured in a single shot, enabling the inference of plasma parameters such as density, electron and ion temperatures, and flow velocity. Compared to Thomson scattering, this technique offers signal enhancements typically larger than 9 orders of magnitude, significantly reducing the required probe laser intensity and facilitating interactions that are linear and measurements that are nonperturbative of the plasma. Furthermore, it provides a powerful tool for advancing studies of crossed-beam energy transfer under conditions relevant to inertial confinement fusion experiments.}, archive = {J_PRL}, author = {A. Longman and R. Muir and D. E. Mittelberger and E. S. Grace and C. Goyon and G. F. Swadling and G. E. Kemp and T. Chapman and S. Maricle and N. Vanartsdalen and A. Linder and T. Dumbacher and K. Zoromski and B. C. Stuart and F. Albert and J. E. Heebner and P. Michel}, doi = {10.1103/96yh-96pw}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {175103}, shortjournal = {Phys. Rev. Lett.}, title = {Pump with broadband probe experiments for single-shot measurements of plasma conditions and crossed-beam energy transfer}, volume = {135}, year = {2025}, }
• (2025). Revealing the structure and dynamics of self-generated electric and magnetic fields near plasma stagnation in laser-driven hohlraums. PRL, 135(17), 175102. (www)

  @article{ , abstract = {By coupling newly developed triparticle charged particle radiography with radiography reconstruction algorithms and novel reconstruction postprocessing techniques, the spatial structure and time evolution of self-generated electric and magnetic fields in laser-driven vacuum hohlraums have been quantitatively revealed. Through high-fidelity data from a series of experiments, it is shown that late in the hohlraum evolution (after the end of laser drive) these fields are strongly correlated in both space and time, providing evidence that their evolution is primarily dominated by advection with the plasma flow. At these late times, plasma flow velocities inferred from both gross radiography analysis and field reconstructions (and corroborated with Thomson scattering measurements) indicate that the plasma is approaching stagnation near the hohlraum axis. These experiments provide not only new physical insight into spontaneously generated hohlraum fields, but also provide important spatially and temporally resolved information for future benchmarking of numerical codes.}, archive = {J_PRL}, author = {J. A. Pearcy and G. D. Sutcliffe and T. M. Johnson and B. L. Reichelt and S. G. Dannhoff and J. Kuniumune and Y. Lawrence and B. Foo and M. Gatu-Johnson and J. A. Frenje and R. D. Petrasso and C. K. Li}, doi = {10.1103/7t7r-rpmh}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {175102}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing the structure and dynamics of self-generated electric and magnetic fields near plasma stagnation in laser-driven hohlraums}, volume = {135}, year = {2025}, }
• (2025). Stable small plasmas at the density limit in the w7-X stellarator. PRL, 135(17), 175101. (www)

  @article{ , abstract = {Experiments in the Wendelstein 7-X (W7-X) stellarator with plasma density beyond the established density limit in stellarators [Scalings of energy confinement and density limit in stellarator/heliotron devices, Nucl. Fusion 30 , 11 (1990) .] resulted in unusual, reduced size, fully radiative plasmas lasting stably for many confinement times [Small, stable plasmas, fully decoupled from the plasma-facing components in W7-X, Stellarator News 175 , 1 (2021) .]. In these experiments, the plasma had shrunk to a significantly smaller minor radius due to intense edge radiation from a radiating mantle and had no contact with material components, yet it remained relatively well confined for many confinement times with electron temperatures on the order of 1 keV. To our knowledge, this is the first definitive experimental long-time stability demonstration of such high-temperature contactless plasmas in the laboratory. It is shown that the onset and extent of this fully radiative small plasma state is predictable. The stability of the plasma size is elucidated with a simple power-balance model. In other helical devices such as the Large Helical Device (LHD) and the Wendelstein 7-AS (W7-AS), plasmas that start shrinking suffered from core impurity accumulation leading to a collapse whereas this was generally not observed for these W7-X plasmas.}, archive = {J_PRL}, author = {A. Pandey and T. S. Pedersen and G. Fuchert and T. Szepesi and D. Zhang and T. Stange and A. Buzas and T. Romba and F. Reimold and V. Perseo and S. Kwak and G. Kocsis and G. Cseh and T. Gonda and G. Schlisio and M. Hirsch and N. Chaudhary and W7-X team}, doi = {10.1103/cfg9-v8hf}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {175101}, shortjournal = {Phys. Rev. Lett.}, title = {Stable small plasmas at the density limit in the w7-X stellarator}, volume = {135}, year = {2025}, }
• (2025). Exceptional points and lasing thresholds: When lower-Q modes win. PRL, 135(17), 173802. (www)

  @article{ , abstract = {One of the most fundamental questions in laser physics is the following: Which mode of an optical cavity will reach the lasing threshold first when gain is applied? Intuitively, the answer appears straightforward: When a particular mode is both temporally well confined (i.e., exhibits the highest quality factor) and experiences initially the largest increase of the modal gain, it is naturally expected to lase first. However, in this Letter, we demonstrate that this intuition can fail in surprising ways. Specifically, we show that in the presence of non-Hermitian degeneracies, known as exceptional points, the expected mode hierarchy can be dramatically altered. These spectral singularities can give rise to counterintuitive mode switching, where a mode with a lower quality factor and initially smaller increase of modal gain reaches the lasing threshold ahead of a more favorable competitor. Remarkably, this effect can occur even under spatially uniform pumping, underscoring the subtle and profound influence of non-Hermitian physics on lasing dynamics.}, archive = {J_PRL}, author = {Julius Kullig and Qi Zhong and Jan Wiersig and Ramy El-Ganainy}, doi = {10.1103/zc6x-pfw2}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173802}, shortjournal = {Phys. Rev. Lett.}, title = {Exceptional points and lasing thresholds: When lower-Q modes win}, volume = {135}, year = {2025}, }
• (2025). Open transmission channels in multimode fiber cavities with random mode mixing. PRL, 135(17), 173801. (www)

  @article{ , abstract = {The transport of light in disordered media is governed by open transmission channels, which enable nearly complete transmission of the incident power, despite low average transmission. Extensively studied in diffusive media and chaotic cavities, open channels exhibit unique properties such as universal spatial structure and extended dwell times. However, their experimental study is challenging due to the large number of modes required for control and measurement. We propose a multimode fiber cavity (MMFC) as a platform to explore open channels. Leveraging mode confinement and finite angular spread, MMFCs enabled full channel control, yielding an 18-fold power enhancement in experiment by selectively exciting an open channel with a transmission of . By analyzing 100 transmission matrices of MMFC realizations, we observed a bimodal transmission eigenvalue distribution, indicating high channel control and low losses. The scalability of MMFCs, combined with long dwell times and potential for nonlinear phenomena, offers new opportunities for studying complex wave transport.}, archive = {J_PRL}, author = {Guy Pelc and Shay Guterman and Rodrigo Gutiérrez-Cuevas and Arthur Goetschy and Sébastien M. Popoff and Yaron Bromberg}, doi = {10.1103/fvvb-76nn}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173801}, shortjournal = {Phys. Rev. Lett.}, title = {Open transmission channels in multimode fiber cavities with random mode mixing}, volume = {135}, year = {2025}, }
• (2025). Dissipative phase transition in the two-photon dicke model. PRL, 135(17), 173602. (www)

  @article{ , abstract = {We explore the dissipative phase transition of the two-photon Dicke model, a topic that has garnered significant attention recently. Our analysis reveals that while single-photon loss does not stabilize the intrinsic instability in the model, the inclusion of two-photon loss restores stability, leading to the emergence of superradiant states, which coexist with the normal vacuum states. Using a second-order cumulant expansion for the photons, we derive an analytical description of the system in the thermodynamic limit, which agrees well with the exact calculation results. Additionally, we present the Wigner function for the system, shedding light on the breaking of the symmetry inherent in the model. These findings offer valuable insights into stabilization mechanisms in open quantum systems and pave the way for exploring complex nonlinear dynamics in two-photon Dicke models.}, archive = {J_PRL}, author = {Aanal Jayesh Shah and Peter Kirton and Simone Felicetti and Hadiseh Alaeian}, doi = {10.1103/mz92-6l9g}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173602}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipative phase transition in the two-photon dicke model}, volume = {135}, year = {2025}, }
• (2025). Electron-enabled nanoparticle diffraction. PRL, 135(17), 173601. (www)

  @article{ , abstract = {We propose a scheme for generating high-mass quantum superposition states of an optically precooled, levitated nanoparticle through electron diffraction at its subnanometer crystal lattice. When a single electron undergoes Bragg diffraction at a free-falling nanoparticle, momentum conservation implies that the superposition of Bragg momenta is imprinted onto the relative coordinate between electron and nanoparticle, which entangles their wave functions. By imaging the electron interferogram, one maps the nanoparticle state onto a superposition of Bragg momenta, as if it was diffracted by its own lattice. This results in a coherent momentum splitting approximately 1000 times greater than what is achievable with two-photon recoils in conventional standing-wave gratings. Self-interference of the nanoparticle can thus be observed within drastically shorter free-fall times in a time-domain Talbot interferometer configuration, significantly relaxing source requirements and alleviating decoherence from environmental factors such as residual gas and thermal radiation. Shorter interference times also allow for a recapture of the nanoparticle within its initial trapping volume, facilitating its reuse in many rapid experimental duty cycles. This opens new possibilities for experimental tests of macroscopic quantum effects within a transmission electron microscope.}, archive = {J_PRL}, author = {Stefan Nimmrichter and Dennis Rätzel and Isobel C. Bicket and Michael S. Seifner and Philipp Haslinger}, doi = {10.1103/3bvs-ymd7}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173601}, shortjournal = {Phys. Rev. Lett.}, title = {Electron-enabled nanoparticle diffraction}, volume = {135}, year = {2025}, }
• (2025). Interaction induced anderson transition in a kicked one dimensional bose gas. PRL, 135(17), 173403. (www)

  @article{ , abstract = {We investigate the Lieb-Liniger model of one-dimensional bosons subjected to periodic kicks. In both the noninteracting and strongly interacting limits, the system undergoes dynamical localization, leading to energy saturation at long times. However, for finite interactions, we reveal an interaction-driven transition from an insulating to a metallic phase at a critical kicking strength, provided the number of particles is three or more. Using the Bethe ansatz solution of the Lieb-Liniger gas, we establish a formal correspondence between its dynamical evolution and an Anderson model in spatial dimensions, where is the number of particles. This theoretical prediction is supported by extensive numerical simulations for three particles, complemented by finite-time scaling analysis, demonstrating that this transition belongs to the orthogonal Anderson universality class.}, archive = {J_PRL}, author = {H. Olsen and P. Devillard and G. Aupetit-Diallo and P. Vignolo and M. Albert}, doi = {10.1103/dyxq-qkmd}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173403}, shortjournal = {Phys. Rev. Lett.}, title = {Interaction induced anderson transition in a kicked one dimensional bose gas}, volume = {135}, year = {2025}, }
• (2025). Solitons in arbitrary dimensions stabilized by photon-mediated interactions. PRL, 135(17), 173402. (www)

  @article{ , abstract = {We propose a scheme to generate solitons in arbitrary dimensions, in a matter-wave interferometer, without the need of quantum degeneracy. In our setting, solitons emerge by balancing the single-particle dispersion with engineered cavity-mediated exchange interactions between two wave packets, which, at the appropriate conditions, remain bound to each other and dispersion-free. For detection in thermal gases, we propose an interferometric probing scheme instead of traditional time-of-flight imaging.}, archive = {J_PRL}, author = {Haoqing Zhang and Anjun Chu and Chengyi Luo and James K. Thompson and Ana Maria Rey}, doi = {10.1103/qrk6-phhk}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173402}, shortjournal = {Phys. Rev. Lett.}, title = {Solitons in arbitrary dimensions stabilized by photon-mediated interactions}, volume = {135}, year = {2025}, }
• (2025). Creating and melting a supersolid by heating a quantum dipolar system. PRL, 135(17), 173401. (www)

  @article{ , abstract = {Recent experiments have shown that raising the temperature of a dipolar gas under certain conditions leads to a transition to a supersolid state. Here, we employ the path integral Monte Carlo method, which exactly accounts for both thermal and correlation effects, to study that phenomenology in a system of atoms in the canonical ensemble. Our microscopic description allows the quantitative characterization of the emergence of spatial order and superfluidity, the two ingredients that define a supersolid state. Our calculations prove that temperature on its own can promote the formation of a supersolid in a dipolar system. Furthermore, we bridge this exotic phenomenology with the more usual melting of the supersolid at a higher temperature. Our results offer insight into the interplay between thermal excitations, the dipole-dipole interaction, quantum statistics, and supersolidity.}, archive = {J_PRL}, author = {R. Bombín and J. Boronat and F. Mazzanti and J. Sánchez-Baena}, doi = {10.1103/nkm3-1725}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {173401}, shortjournal = {Phys. Rev. Lett.}, title = {Creating and melting a supersolid by heating a quantum dipolar system}, volume = {135}, year = {2025}, }
• (2025). Reconciliation between neutron skin thickness from PREX-2 experiment and neutron-star tidal polarizability from GW170817 event: The key role of symmetry energy curvature. PRL, 135(17), 172701. (www)

  @article{ , abstract = {The GW170817 neutron star merger event and the PREX-2 experiment probing neutron skin thickness provide crucial clues for understanding the nuclear equation of state (EoS). However, an apparent inconsistency exists between the tidal polarizability Λ 1.4 inferred from GW170817 and the neutron skin thickness R np 208 of Pb 208 measured by PREX-2, based on relativistic energy density functionals (EDFs). This Letter employs both relativistic and nonrelativistic EDFs to identify a multipole correlation involving Λ 1.4 , R np 208 , and the symmetry energy curvature K sym at saturation density. We demonstrate the essential role of K sym in reconciling the conflicting Λ 1.4 − R np 208 correlations derived from nonrelativistic versus relativistic EDFs and in resolving the discrepancy between the GW170817 and PREX-2 data constraints. Furthermore, we obtain a joint constraint on K sym from these datasets, providing a vital constraint on the symmetry energy of the nuclear EoS.}, archive = {J_PRL}, author = {Z. Y. Guan (管中原 and Y. F. Niu (牛一斐}, doi = {10.1103/6m4p-wmv3}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {172701}, shortjournal = {Phys. Rev. Lett.}, title = {Reconciliation between neutron skin thickness from PREX-2 experiment and neutron-star tidal polarizability from GW170817 event: The key role of symmetry energy curvature}, volume = {135}, year = {2025}, }
• (2025). Chiral symmetry and peripheral neutron-α scattering. PRL, 135(17), 172502. (www)

  @article{ , abstract = {We propose and demonstrate that peripheral neutron- scattering at low energies can serve as a sensitive and clean probe of the long-range three-nucleon forces. To this aim, we perform ab initio quantum Monte Carlo calculations using two- and three-nucleon interactions derived in chiral effective field theory up to third expansion order. We show that the longest-range three-nucleon force stemming from the two-pion exchange plays a crucial role in the proper description of the neutron- -wave phase shifts. Our Letter reveals the predictive power of chiral symmetry in the few-body sector and opens a new direction for probing and constraining three-nucleon forces.}, archive = {J_PRL}, author = {Yilong Yang (杨一龙 and Evgeny Epelbaum and Jie Meng (孟杰 and Lu Meng (孟璐 and Pengwei Zhao (赵鹏巍}, doi = {10.1103/45g7-bmp6}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {172502}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral symmetry and peripheral neutron-α scattering}, volume = {135}, year = {2025}, }
• (2025). Toward a microscopic description of nucleus-nucleus collisions. PRL, 135(17), 172501. (www)

  @article{ , abstract = {We present the first results of a comprehensive microscopic approach to describe nucleus-nucleus elastic collisions by means of an optical potential derived at first order in multiple-scattering theory and computed by folding the projectile and target nuclear densities with the nucleon-nucleon matrix, which describes the interaction between each nucleon of the projectile and each nucleon of the target. Chiral interactions are consistently used in the calculation of the matrix and of the nonlocal nuclear densities, which are computed within the ab initio no-core shell model. Cross sections calculated for collisions on and at projectile energies in the range 100–300 MeV are presented and compared with available data. For momentum transfer up to about our results are in good agreement with the experimental data, whereas for higher momenta a reduction of the imaginary contributions is needed.}, archive = {J_PRL}, author = {Matteo Vorabbi and Michael Gennari and Paolo Finelli and Carlotta Giusti and Petr Navrátil}, doi = {10.1103/qxtf-5b4y}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {172501}, shortjournal = {Phys. Rev. Lett.}, title = {Toward a microscopic description of nucleus-nucleus collisions}, volume = {135}, year = {2025}, }
• (2025). QT slicing with multiple jets. PRL, 135(17), 171903. (www)

  @article{ , abstract = {Modern collider phenomenology requires unprecedented precision for the theoretical predictions, for which slicing techniques provide an essential tool at next-to-next-to-leading order (NNLO) in the strong coupling. The most popular slicing variable is based on the transverse momentum of a color-singlet final state, but its generalization to final states with jets is known to be very difficult. Here we propose two generalizations of that can be used for jet processes, providing proof of concept with an NLO slicing for jets. We present factorization formulas that enable our approach to NNLO, calculate the NNLO collinear-soft function, and demonstrate slicing at this order for jets. One of these generalizations of only applies to planar Born processes, such as jets, but offers a dramatic simplification of the soft function. We also discuss how our approach can directly be extended to obtain predictions for the fragmentation of hadrons. This presents a promising path for high-precision QCD calculations with multijet final states.}, archive = {J_PRL}, author = {Rong-Jun Fu and Rudi Rahn and Ding Yu Shao and Wouter J. Waalewijn and Bin Wu}, doi = {10.1103/htvz-wz1p}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171903}, shortjournal = {Phys. Rev. Lett.}, title = {QT slicing with multiple jets}, volume = {135}, year = {2025}, }
• (2025). Identified hadron production at hadron colliders in next-to-next-to-leading-order QCD. PRL, 135(17), 171902. (www)

  @article{ , abstract = {In this Letter we calculate for the first time the next-to-next-to leading order (NNLO) QCD corrections to identified hadron production at hadron colliders. The inclusion of the NNLO correction has an important impact on all observables considered in this Letter. Higher order corrections reduce scale uncertainty and in almost all cases are moderate. Overall, good perturbative convergence is observed across kinematics and observables. The uncertainty due to missing higher orders is relatively small and, in many cases, smaller than the experimental uncertainty. The largest source of theoretical uncertainty at present is from the knowledge of the nonperturbative parton-to-hadron fragmentation functions (FFs), which dwarfs the scale uncertainty in most kinematic ranges. The inclusion of NNLO corrections demonstrates the precision studies potential of this class of observables. To fully realize this potential, however, a new generation of improved fragmentation functions may be needed. The results of the present Letter will enable global fits of FFs with NNLO precision.}, archive = {J_PRL}, author = {Michał Czakon and Terry Generet and Alexander Mitov and Rene Poncelet}, doi = {10.1103/mhkl-vt96}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171902}, shortjournal = {Phys. Rev. Lett.}, title = {Identified hadron production at hadron colliders in next-to-next-to-leading-order QCD}, volume = {135}, year = {2025}, }
• (2025). First observation of quantum correlations in e+e−→XDD¯ and C-even constrained DD¯ pairs. PRL, 135(17), 171901. (www)

  @article{ , abstract = {The study of meson pairs produced with quantum correlations gives direct access to parameters that are challenging to measure in other systems. In this Letter, the existence of quantum correlations due to charge-conjugation symmetry C are demonstrated in D D ¯ pairs produced through the processes e + e − → D D ¯ , e + e − → D * D ¯ , and e + e − → D * D ¯ * , where the lack of charge superscripts refers to an admixture of neutral-charm-meson particle and antiparticle states, using 7.13 fb − 1 of e + e − collision data collected by the BESIII experiment between center-of-mass energies of 4.13–4.23 GeV. Processes with either C -even or C -odd constraints are identified and separated. A procedure is presented that harnesses the entangled production process to enable measurements of D 0 -meson hadronic parameters. This Letter provides the first confirmation of quantum correlations in e + e − → X D D ¯ processes and the first observation of a C -even constrained D D ¯ system. The procedure is applied to measure δ K π D , the strong phase between the D 0 → K − π + and D ¯ 0 → K − π + decay amplitudes, which results in the determination of δ K π D = ( 192.8 − 12.4 − 2.4 + 11.0 + 1.9 ) ° . The potential for measurements of other hadronic decay parameters and charm mixing with these and future datasets is also discussed.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. Gao and Y. N. Gao and Y. Y. Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. L. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Q. A. Malik and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. J. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and L. Q. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Y. P. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/dkgg-9twj}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171901}, shortjournal = {Phys. Rev. Lett.}, title = {First observation of quantum correlations in e+e−→XDD¯ and C-even constrained DD¯ pairs}, volume = {135}, year = {2025}, }
• (2025). First event-by-event identification of cherenkov radiation from sub-mev particles in liquid argon. PRL, 135(17), 171804. (www)

  @article{ , abstract = {This Letter reports the event-by-event observation of Cherenkov light from sub-MeV electrons in a high scintillation light-yield liquid argon detector by the coherent CAPTAIN-Mills (CCM) experiment. The CCM200 detector, located at Los Alamos National Laboratory, instruments seven tons (fiducial volume) of liquid argon with 200 eight-inch photomultiplier tubes, 80% of which are coated in a wavelength-shifting material and the remaining 20% are uncoated. In the prompt time region of an event, defined as relative to the event start time , the uncoated photomultiplier tubes are primarily sensitive to visible Cherenkov photons. Using gamma rays from a source for production of sub-MeV electrons, we isolated prompt Cherenkov light with confidence and developed a selection to obtain a low-background electromagnetic sample. This is the first event-by-event observation of Cherenkov photons from sub-MeV electrons in a high-yield scintillator detector and represents a milestone in low-energy particle detector development.}, archive = {J_PRL}, author = {CCM Collaboration and A. A. Aguilar-Arevalo and S. Biedron and J. Boissevain and M. Borrego and L. Bugel and M. Chavez-Estrada and J. M. Conrad and R. L. Cooper and J. R. Distel and J. C. D’Olivo and E. Dunton and B. Dutta and D. E. Fields and M. Gold and E. Guardincerri and E. C. Huang and N. Kamp and D. Kim and K. Knickerbocker and W. C. Louis and C. F. Macias-Acevedo and R. Mahapatra and J. Mezzetti and J. Mirabal and M. J. Mocko and D. A. Newmark and P. deNiverville and C. O’Connor and V. Pandey and D. Poulson and H. Ray and E. Renner and T. J. Schaub and A. Schneider and M. H. Shaevitz and D. Smith and W. Sondheim and A. M. Szelc and C. Taylor and A. Thompson and W. H. Thompson and M. Tripathi and R. T. Thornton and R. Van Berg and R. G. Van de Water}, doi = {10.1103/bklh-w3dn}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171804}, shortjournal = {Phys. Rev. Lett.}, title = {First event-by-event identification of cherenkov radiation from sub-mev particles in liquid argon}, volume = {135}, year = {2025}, }
• (2025). First differential measurement of the single π+ production cross section in neutrino neutral-current scattering. PRL, 135(17), 171803. (www)

  @article{ , abstract = {Since its first observation in the 1970s, neutrino-induced neutral-current single positive pion production ( ) has remained an elusive and poorly understood interaction channel. This process is a significant background in neutrino oscillation experiments and studying it further is critical for the physics program of next-generation accelerator-based neutrino oscillation experiments. In this Letter, we present the first double-differential cross-section measurement of interactions using data from the ND280 detector of the T2K experiment collected in -beam mode. The measured flux-averaged integrated cross section is . We compare the results on a hydrocarbon target to the predictions of several neutrino interaction generators and final-state-interaction models. While model predictions agree with the differential results, the data show a weak preference for a cross-section normalization approximately 30% higher than predicted by most models studied in this Letter.}, archive = {J_PRL}, author = {T2K Collaboration and K. Abe and S. Abe and R. Akutsu and H. Alarakia-Charles and Y. I. Alj Hakim and S. Alonso Monsalve and L. Anthony and S. Aoki and K. A. Apte and T. Arai and T. Arihara and S. Arimoto and Y. Ashida and E. T. Atkin and N. Babu and V. Baranov and G. J. Barker and G. Barr and D. Barrow and P. Bates and L. Bathe-Peters and M. Batkiewicz-Kwasniak and N. Baudis and V. Berardi and L. Berns and S. Bhattacharjee and A. Blanchet and A. Blondel and S. Bolognesi and S. Bordoni and S. B. Boyd and C. Bronner and A. Bubak and M. Buizza Avanzini and J. A. Caballero and F. Cadoux and N. F. Calabria and S. Cao and S. Cap and D. Carabadjac and S. L. Cartwright and M. P. Casado and M. G. Catanesi and J. Chakrani and A. Chalumeau and A. Chvirova and G. Collazuol and F. Cormier and A. A. L. Craplet and A. Cudd and D. D’ago and C. Dalmazzone and T. Daret and P. Dasgupta and C. Davis and Yu. I. Davydov and G. De Rosa and T. Dealtry and C. Densham and A. Dergacheva and R. Dharmapal Banerjee and F. Di Lodovico and G. Diaz Lopez and S. Dolan and D. Douqa and T. A. Doyle and O. Drapier and K. E. Duffy and J. Dumarchez and P. Dunne and K. Dygnarowicz and A. Eguchi and J. Elias and S. Emery-Schrenk and G. Erofeev and A. Ershova and G. Eurin and D. Fedorova and S. Fedotov and M. Feltre and L. Feng and D. Ferlewicz and A. J. Finch and M. D. Fitton and C. Forza and M. Friend and Y. Fujii and Y. Fukuda and Y. Furui and J. García-Marcos and A. C. Germer and L. Giannessi and C. Giganti and V. Glagolev and M. Gonin and R. González Jiménez and J. González Rosa and E. A. G. Goodman and K. Gorshanov and P. Govindaraj and M. Grassi and M. Guigue and F. Y. Guo and D. R. Hadley and S. Han and D. A. Harris and R. J. Harris and T. Hasegawa and C. M. Hasnip and S. Hassani and N. C. Hastings and Y. Hayato and I. Heitkamp and D. Henaff and Y. Hino and J. Holeczek and A. Holin and T. Holvey and N. T. Hong Van and T. Honjo and M. C. F. Hooft and K. Hosokawa and J. Hu and A. K. Ichikawa and K. Ieki and M. Ikeda and T. Ishida and M. Ishitsuka and A. Izmaylov and N. Jachowicz and S. J. Jenkins and C. Jesús-Valls and M. Jia and J. J. Jiang and J. Y. Ji and T. P. Jones and P. Jonsson and S. Joshi and M. Kabirnezhad and A. C. Kaboth and H. Kakuno and J. Kameda and S. Karpova and V. S. Kasturi and Y. Kataoka and T. Katori and Y. Kawamura and M. Kawaue and E. Kearns and M. Khabibullin and A. Khotjantsev and T. Kikawa and S. King and V. Kiseeva and J. Kisiel and A. Klustová and L. Kneale and H. Kobayashi and L. Koch and S. Kodama and M. Kolupanova and A. Konaka and L. L. Kormos and Y. Koshio and K. Kowalik and Y. Kudenko and Y. Kudo and A. Kumar Jha and R. Kurjata and V. Kurochka and T. Kutter and L. Labarga and M. Lachat and K. Lachner and J. Lagoda and S. M. Lakshmi and M. Lamers James and A. Langella and D. H. Langridge and J.-F. Laporte and D. Last and N. Latham and M. Laveder and M. Lawe and D. Leon Silverio and S. Levorato and S. V. Lewis and B. Li and C. Lin and R. P. Litchfield and S. L. Liu and W. Li and A. Longhin and A. Lopez Moreno and L. Ludovici and X. Lu and T. Lux and L. N. Machado and L. Magaletti and K. Mahn and K. K. Mahtani and M. Mandal and S. Manly and A. D. Marino and D. G. R. Martin and D. A. Martinez Caicedo and L. Martinez and M. Martini and T. Matsubara and R. Matsumoto and V. Matveev and C. Mauger and K. Mavrokoridis and N. McCauley and K. S. McFarland and J. McKean and A. Mefodiev and G. D. Megias and L. Mellet and M. Mezzetto and S. Miki and V. Mikola and E. W. Miller and A. Minamino and O. Mineev and S. Mine and J. Mirabito and M. Miura and S. Moriyama and P. Morrison and Th. A. Mueller and D. Munford and A. Muñoz and L. Munteanu and Y. Nagai and T. Nakadaira and K. Nakagiri and M. Nakahata and Y. Nakajima and K. D. Nakamura and Y. Nakano and S. Nakayama and T. Nakaya and K. Nakayoshi and C. E. R. Naseby and D. T. Nguyen and V. Q. Nguyen and K. Niewczas and S. Nishimori and Y. Nishimura and Y. Noguchi and T. Nosek and F. Nova and J. C. Nugent and H. M. O’Keeffe and L. O’Sullivan and R. Okazaki and W. Okinaga and K. Okumura and T. Okusawa and N. Onda and N. Ospina and L. Osu and Y. Oyama and V. Paolone and J. Pasternak and M. Pfaff and L. Pickering and B. Popov and A. J. Portocarrero Yrey and M. Posiadala-Zezula and Y. S. Prabhu and H. Prasad and F. Pupilli and B. Quilain and P. T. Quyen and E. Radicioni and B. Radics and M. A. Ramirez and R. Ramsden and P. N. Ratoff and M. Reh and G. Reina and C. Riccio and D. W. Riley and E. Rondio and S. Roth and N. Roy and A. Rubbia and L. Russo and A. Rychter and W. Saenz and K. Sakashita and F. Sánchez and E. M. Sandford and Y. Sato and T. Schefke and C. M. Schloesser and K. Scholberg and M. Scott and Y. Seiya and T. Sekiguchi and H. Sekiya and T. Sekiya and D. Seppala and D. Sgalaberna and A. Shaikhiev and M. Shiozawa and Y. Shiraishi and A. Shvartsman and N. Skrobova and K. Skwarczynski and D. Smyczek and M. Smy and J. T. Sobczyk and H. Sobel and F. J. P. Soler and A. J. Speers and R. Spina and A. Srivastava and P. Stowell and Y. Stroke and I. A. Suslov and A. Suzuki and S. Y. Suzuki and M. Tada and S. Tairafune and A. Takeda and Y. Takeuchi and H. K. Tanaka and H. Tanigawa and V. V. Tereshchenko and N. Thamm and N. Tran and T. Tsukamoto and M. Tzanov and Y. Uchida and M. Vagins and M. Varghese and I. Vasilyev and G. Vasseur and E. Villa and U. Virginet and T. Vladisavljevic and T. Wachala and D. Wakabayashi and H. T. Wallace and J. G. Walsh and L. Wan and D. Wark and M. O. Wascko and A. Weber and R. Wendell and M. J. Wilking and C. Wilkinson and J. R. Wilson and K. Wood and C. Wret and J. Xia and K. Yamamoto and T. Yamamoto and Y. Yang and T. Yano and N. Yershov and U. Yevarouskaya and M. Yokoyama and Y. Yoshimoto and N. Yoshimura and R. Zaki and A. Zalewska and J. Zalipska and G. Zarnecki and J. Zhang and X. Y. Zhao and H. Zheng and H. Zhong and T. Zhu and M. Ziembicki and E. D. Zimmerman and M. Zito and S. Zsoldos}, doi = {10.1103/6d32-l452}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171803}, shortjournal = {Phys. Rev. Lett.}, title = {First differential measurement of the single π+ production cross section in neutrino neutral-current scattering}, volume = {135}, year = {2025}, }
• (2025). Hitting the thermal target for leptophilic dark matter at future lepton colliders. PRL, 135(17), 171802. (www)

  @article{ , abstract = {We study future lepton collider prospects for testing predictive models of leptophilic dark matter (DM) candidates with a thermal origin. We calculate experimental milestones for testing the parameter space compatible with freeze-out and the associated collider signals at past, present, and future facilities. This analysis places new limits on such models by leveraging the utility of lepton colliders. At machines, we make projections using precision -pole observables from signatures at large electron-positron collider and future projections for future circular collider (ee) in these channels. Additionally, a muon collider could also probe new thermal relic parameter space in this scenario via , where is any easily identifiable standard model object. Collectively, these processes can probe much of the parameter space for which DM direct annihilation to yields the observed relic density in Higgs-like models with mass-proportional couplings to charged leptons.}, archive = {J_PRL}, author = {Cari Cesarotti and Gordan Krnjaic}, doi = {10.1103/w1bw-w7wt}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171802}, shortjournal = {Phys. Rev. Lett.}, title = {Hitting the thermal target for leptophilic dark matter at future lepton colliders}, volume = {135}, year = {2025}, }
• (2025). Observation of D+→KS0π0μ+νμ, test of lepton flavor universality, and first angular analysis of D+→K¯*(892)0ℓ+νℓ. PRL, 135(17), 171801. (www)

  @article{ , abstract = {We report a study of the semileptonic decays ( , ) based on of collision data collected at the center-of-mass energy of 3.773 GeV with the BESIII detector. The decay is observed for the first time, with a branching fraction of , and the branching fraction of is determined with the improved precision as . From the analysis of the dynamics, we observe that the dominant component is accompanied by an -wave contribution, which accounts for of the total decay rate of the channel and of the channel. Assuming a single-pole dominance parametrization, the hadronic form factor ratios are extracted to be and . Based on the first comprehensive angular and the decay-rate asymmetry analysis, the full set of averaged angular and asymmetry observables are measured as a function of the momentum-transfer squared; they are consistent with expectations from the standard model. No evidence for violation of lepton-flavor universality is observed in either the full range or the five chosen bins of momentum-transfer squared.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. Gao and Y. N. Gao and Y. Y. Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Q. A. Malik and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. J. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and L. Q. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Y. P. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/w9vz-4fq9}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171801}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of D+→KS0π0μ+νμ, test of lepton flavor universality, and first angular analysis of D+→K¯*(892)0ℓ+νℓ}, volume = {135}, year = {2025}, }
• (2025). Stimulated emission or absorption of gravitons by light. PRL, 135(17), 171501. (www)

  @article{ , abstract = {We study the exchange of energy between gravitational and electromagnetic waves in an extended Mach-Zehnder or Sagnac type geometry that is analogous to an “optical Weber bar.” In the presence of a gravitational wave (such as the ones measured by the Laser Interferometer Gravitational Wave Observatory), we find that it should be possible to observe (via interference or beating effects after a delay line) signatures of stimulated emission or absorption of gravitons with present-day technology. Apart from marking the transition from passively observing to actively manipulating such a natural phenomenon, this could also be used as a complementary detection scheme. Nonclassical photon states may improve the sensitivity and might even allow us to test certain quantum aspects of the gravitational field.}, archive = {J_PRL}, author = {Ralf Schützhold}, doi = {10.1103/xd97-c6d7}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171501}, shortjournal = {Phys. Rev. Lett.}, title = {Stimulated emission or absorption of gravitons by light}, volume = {135}, year = {2025}, }
• (2025). Late-time tails in nonlinear evolutions of merging black holes. PRL, 135(17), 171401. (www)

  @article{ , abstract = {We uncover late-time gravitational-wave tails in fully nonlinear dimensional numerical relativity simulations of merging black holes, using the highly accurate s p ec code. We achieve this result by exploiting the strong magnification of late-time tails due to binary eccentricity, recently observed in perturbative evolutions, and showcase here the tail presence in head-on configurations for several mass ratios close to unity. We validate the result through a large battery of numerical tests and detailed comparison with a perturbative evolution, which display striking agreement with full nonlinear ones in the ringdown regime, and very similar tail morphologies. Our results offer yet another confirmation of the highly predictive power of black hole perturbation theory in the presence of a source, even when applied to nonlinear solutions. The late-time tail signal is much more prominent than anticipated until recently, and possibly within reach of gravitational-wave detector measurements, unlocking observational investigations of an additional set of general relativistic predictions on the long-range gravitational dynamics.}, archive = {J_PRL}, author = {Marina De Amicis and Hannes R. Rüter and Gregorio Carullo and Simone Albanesi and C. Melize Ferrus and Keefe Mitman and Leo C. Stein and Vitor Cardoso and Sebastiano Bernuzzi and Michael Boyle and Nils Deppe and Lawrence E. Kidder and Jordan Moxon and Alessandro Nagar and Kyle C. Nelli and Harald P. Pfeiffer and Mark A. Scheel and William Throwe and Nils L. Vu and An𝚤l Zenginoğlu}, doi = {10.1103/2brx-xnyr}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171401}, shortjournal = {Phys. Rev. Lett.}, title = {Late-time tails in nonlinear evolutions of merging black holes}, volume = {135}, year = {2025}, }
• (2025). Warm inflation with the standard model. PRL, 135(17), 171002. (www)

  @article{ , abstract = {We show for the first time that warm inflation is feasible with standard model (SM) gauge interactions alone. Our model consists of a minimal extension of the SM by a single scalar inflaton field with an axionlike coupling to gluons and a monomial potential. The effects of light fermions, which were previously argued to render warm inflation with the SM impossible, are alleviated by Hubble dilution of their chiral chemical potentials. Our model features only one adjustable combination of parameters and accommodates all inflationary observables. We briefly discuss implications for axion experiments, dark matter, and the strong problem.}, archive = {J_PRL}, author = {Kim V. Berghaus and Marco Drewes and Sebastian Zell}, doi = {10.1103/9nn9-bsm9}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171002}, shortjournal = {Phys. Rev. Lett.}, title = {Warm inflation with the standard model}, volume = {135}, year = {2025}, }
• (2025). Search for QCD coupled axion dark matter with data from the MICROSCOPE space experiment. PRL, 135(17), 171001. (www)

  @article{ , abstract = {Axion dark matter coupled via QCD induces a nonzero differential acceleration between test masses of different composition. Tests of the equivalence principle, like the recent MICROSCOPE space mission, are sensitive to such a signal. We use the final released data of the MICROSCOPE experiment to search for this effect. We find no positive signal consistent with the dark matter model, and set upper limits on the axion-gluon coupling that improve existing laboratory bounds by up to 2 orders of magnitude for axion masses in the to range.}, archive = {J_PRL}, author = {Jordan Gué and Peter Wolf and Aurélien Hees}, doi = {10.1103/fwzv-g1jg}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {171001}, shortjournal = {Phys. Rev. Lett.}, title = {Search for QCD coupled axion dark matter with data from the MICROSCOPE space experiment}, volume = {135}, year = {2025}, }
• (2025). Optimal and feasible contextuality-based randomness generation. PRL, 135(17), 170805. (www)

  @article{ , abstract = {Semi-device-independent randomness generation protocols based on Kochen-Specker contextuality offer the attractive features of compact devices, high rates, and ease of experimental implementation over fully device-independent (DI) protocols. Here, we investigate this paradigm and derive four results to improve the state of the art. Firstly, we introduce a family of simple, experimentally feasible orthogonality graphs (measurement compatibility structures) for which the maximum violation of the corresponding noncontextuality inequalities allows the certification of the maximum amount of log 2 d bits of randomness from a qudit system with projective measurements for d ≥ 3 . We analytically derive the Lovász theta and fractional packing number for this graph family, and thereby prove their utility for optimal randomness generation in both randomness expansion and amplification tasks. Secondly, a central additional assumption in contextuality-based protocols over fully DI ones is that the measurements are repeatable and satisfy an intended compatibility structure. We frame a relaxation of this condition in terms of ϵ -orthogonality graphs for a parameter ϵ > 0 , and derive quantum correlations that allow the certification of randomness for arbitrary relaxation ϵ ∈ [ 0 , 1 ) . Thirdly, it is well-known that a single qubit is noncontextual, i.e., the qubit correlations can be explained by a noncontextual hidden variable model. We show however that a single qubit is almost contextual in that there exist qubit correlations that cannot be explained by ϵ -faithful noncontextual hidden variable models for small ϵ > 0 . Finally, we point out possible attacks by quantum and general consistent (nonsignaling) adversaries for certain classes of contextuality tests over and above those considered in DI scenarios.}, archive = {J_PRL}, author = {Yuan Liu and Ravishankar Ramanathan}, doi = {10.1103/cn3m-j743}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170805}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal and feasible contextuality-based randomness generation}, volume = {135}, year = {2025}, }
• (2025). Coexistence of continuous-variable quantum key distribution and classical data over 120 km fiber. PRL, 135(17), 170804. (www)

  @article{ , abstract = {Integrating quantum key distribution (QKD) with classical data transmission over the same fiber is crucial for scalable quantum-secured communication. However, noise from classical channels limits QKD distance. We demonstrate the longest-distance continuous-variable QKD (CV-QKD) over 120 km (20 dB loss) in the asymptotic regime, and over 100 km (17 dB loss) in the finite-size regime, both coexisting with a fully populated coarse wavelength division multiplexing system. Natural mode filtering of the local oscillator and phase noise mitigation enabled this without additional filtering or wavelength reallocation. Benchmarking against a commercial discrete-variable QKD system and considering finite-size effects confirms the feasibility of CV-QKD as a plug-and-play solution for typical 80–100 km long-haul optical networks. Our results set a record fiber distance for CV-QKD, showing its potential for cost-effective, large-scale deployment in existing network infrastructure.}, archive = {J_PRL}, author = {Adnan A. E. Hajomer and Ivan Derkach and Vladyslav C. Usenko and Ulrik L. Andersen and Tobias Gehring}, doi = {10.1103/zy2d-m3ch}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170804}, shortjournal = {Phys. Rev. Lett.}, title = {Coexistence of continuous-variable quantum key distribution and classical data over 120 km fiber}, volume = {135}, year = {2025}, }
• (2025). Wideband covariance magnetometry below the diffraction limit. PRL, 135(17), 170803. (www)

  @article{ , abstract = {We experimentally demonstrate a method for measuring correlations of wideband magnetic signals with spatial resolution below the optical diffraction limit. Our technique employs two nitrogen-vacancy (NV) centers in diamond as nanoscale magnetometers, spectrally resolved by inhomogeneous optical transitions. Using high-fidelity optical readout and long spin coherence time, we probe correlated megahertz-range noise with sensitivity of . In addition, we use this system for correlated relaxometry, enabling correlation measurements of gigahertz-range noise. Under such externally applied noise, while individual NV centers exhibit featureless relaxation, their correlation displays rich coherent and incoherent dynamics reminiscent of superradiance physics. This capability to probe high-frequency correlations provides a powerful tool for investigating a variety of condensed-matter phenomena characterized by nonlocal correlations.}, archive = {J_PRL}, author = {Xuan Hoang Le and Pavel E. Dolgirev and Piotr Put and Eric L. Peterson and Arjun Pillai and Alexander A. Zibrov and Eugene Demler and Hongkun Park and Mikhail D. Lukin}, doi = {10.1103/7xlj-52xt}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170803}, shortjournal = {Phys. Rev. Lett.}, title = {Wideband covariance magnetometry below the diffraction limit}, volume = {135}, year = {2025}, }
• (2025). Near-perfect broadband quantum memory enabled by intelligent spin-wave compaction. PRL, 135(17), 170802. (www)

  @article{ , abstract = {Quantum memory, a pivotal hub in quantum information processing, is expected to achieve temporal storage and coherent manipulation of quantum states with memory efficiency exceeding 90% and quantum fidelity surpassing the noncloning limit. However, the current performance falls short of these requirements due to the inherent trade-off between memory efficiency enhancement and noise amplification, which not only imposes significant demands on quantum purification but also fundamentally impedes continuous-variable quantum information processing. In this Letter, we break through these constraints by unveiling a Hankel transform spatiotemporal mapping for light-spin-wave conversion in quantum memory and proposing an intelligently light-manipulated strategy for spin wave compaction, which maximizes memory efficiency while suppressing excess noise. This strategy is experimentally demonstrated for a Raman quantum memory in warm atomic vapor with an efficiency up to and a low noise level of only photon per pulse. The unconditional fidelity reaches with an average of 1.0 photon per pulse for a 17 ns input signal. Our results successfully demonstrate a practical benchmark for broadband quantum memory that may facilitate advancements in high-speed quantum networks, quantum state manipulation, and scalable quantum computation.}, archive = {J_PRL}, author = {Jinxian Guo and Zeliang Wu and Guzhi Bao and Peiyu Yang and Yuan Wu and L. Q. Chen and Weiping Zhang}, doi = {10.1103/kbwj-md9n}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170802}, shortjournal = {Phys. Rev. Lett.}, title = {Near-perfect broadband quantum memory enabled by intelligent spin-wave compaction}, volume = {135}, year = {2025}, }
• (2025). Temporal asymmetry in entanglement distillation. PRL, 135(17), 170801. (www)

  @article{ , abstract = {Entanglement, while central to quantum technologies, suffers from fragility when exposed to realistic noise. Conventional entanglement distillation tackles this by treating the noisy outputs of an entangling channel as static resources, applying local operations and classical communication after the fact. We challenge this static view. Our approach considers the entangling channel itself as a dynamic, consumable resource, actively purifying it by interposing optimally tailored local unitaries before the channel. We prove that preprocessing achieves entanglement fidelities fundamentally unreachable by any free postprocessing, exposing an intrinsic temporal asymmetry in distillation. Our experimental demonstration not only confirms these findings but also shows that preprocessing can elevate teleportation beyond the classical limit. By integrating theoretical framework with experimental realization, this Letter emphasizes the importance of embracing entanglement’s dynamic nature, paving a more efficient path for optimizing quantum information processing.}, archive = {J_PRL}, author = {Yuhang Li and Junjing Xing and Dengke Qu and Huixia Gao and Lei Xiao and Jin-Ming Liu and Yunlong Xiao and Peng Xue}, doi = {10.1103/glc7-xy8t}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170801}, shortjournal = {Phys. Rev. Lett.}, title = {Temporal asymmetry in entanglement distillation}, volume = {135}, year = {2025}, }
• (2025). Classically estimating observables of noiseless quantum circuits. PRL, 135(17), 170602. (www)

  @article{ , abstract = {We present a classical algorithm based on Pauli propagation for estimating expectation values of arbitrary observables on random unstructured quantum circuits across all circuit architectures and depths, including those with all-to-all connectivity. We prove that, for any architecture where each circuit layer is randomly sampled from a distribution invariant under single-qubit rotations, our algorithm achieves a small error on all circuits except for a small fraction . The computational time is polynomial in qubit count and circuit depth for any small constant , and quasipolynomial for inverse-polynomially small , . Our results show that estimating observables of quantum circuits exhibiting chaotic and locally scrambling behavior is classically tractable across all geometries.}, archive = {J_PRL}, author = {Armando Angrisani and Alexander Schmidhuber and Manuel S. Rudolph and M. Cerezo and Zoë Holmes and Hsin-Yuan Huang}, doi = {10.1103/lh6x-7rc3}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170602}, shortjournal = {Phys. Rev. Lett.}, title = {Classically estimating observables of noiseless quantum circuits}, volume = {135}, year = {2025}, }
• (2025). Tile codes: High-efficiency quantum codes on a lattice with boundary. PRL, 135(17), 170601. (www)

  @article{ , abstract = {We introduce tile codes , a simple yet powerful way of constructing quantum codes that are local on a planar 2D lattice. Tile codes generalize the usual surface code by allowing for a bit more flexibility in terms of locality and stabilizer weight. Our construction does not compromise on the fact that the codes are local on a lattice with open boundary conditions. Despite its simplicity, we use our construction to find codes with parameters [ [ 288 , 8 , 12 ] ] using weight-6 stabilizers and [ [ 288 , 8 , 14 ] ] using weight-8 stabilizers, outperforming all previously known constructions in this direction. Allowing for a slightly higher nonlocality, we find a [ [ 512 , 18 , 19 ] ] code using weight-8 stabilizers, which outperforms the rotated surface code by a factor of more than 12. Our approach provides a unified framework for understanding the structure of codes that are local on a 2D planar lattice and offers a systematic way to explore the space of possible code parameters. In particular, due to its simplicity, the construction naturally accommodates various types of boundary conditions and stabilizer configurations, making it a versatile tool for quantum error-correction code design.}, archive = {J_PRL}, author = {Vincent Steffan and Shin Ho Choe and Nikolas P. Breuckmann and Francisco Revson Fernandes Pereira and Jens Niklas Eberhardt}, doi = {10.1103/l4mx-l3xx}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170601}, shortjournal = {Phys. Rev. Lett.}, title = {Tile codes: High-efficiency quantum codes on a lattice with boundary}, volume = {135}, year = {2025}, }
• (2025). Minimizing dissipation via interacting environments: Quadratic convergence to landauer bound. PRL, 135(17), 170404. (www)

  @article{ , abstract = {We explore the fundamental limits on thermodynamic irreversibility when cooling a quantum system in the presence of a finite-size reservoir. First, we prove that, for any noninteracting -particle reservoir, the entropy production decays at most linearly with . Instead, we derive a cooling protocol in which , which is, in fact, the best possible scaling. This becomes possible due to the presence of interactions in the finite-size reservoir, which must be prepared at the verge of a phase transition. We further show numerically that an intermediate scaling of with can be achieved using a star-network configuration for the reservoir. Our results open the possibility of cooling with a higher energetic efficiency via interacting reservoirs.}, archive = {J_PRL}, author = {Patryk Lipka-Bartosik and Martí Perarnau-Llobet}, doi = {10.1103/5w1r-1nzs}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170404}, shortjournal = {Phys. Rev. Lett.}, title = {Minimizing dissipation via interacting environments: Quadratic convergence to landauer bound}, volume = {135}, year = {2025}, }
• (2025). Measurement-induced lévy flights of quantum information. PRL, 135(17), 170403. (www)

  @article{ , abstract = {We explore a model of free fermions in one dimension, subject to frustrated (noncommuting) local measurements across adjacent sites, which resolves the fermions into nonorthogonal orbitals, misaligned from the underlying lattice. For maximal misalignment, superdiffusive behavior emerges from the vanishing of the measurement-induced quasiparticle decay rate at one point in the Brillouin zone, which generates fractal-scaling entanglement entropy for a subsystem of length . We derive an effective nonlinear sigma model with long-range couplings responsible for Lévy flights in entanglement propagation, which we confirm with large-scale numerical simulations. When the misalignment is reduced, the entanglement exhibits, with increasing , consecutive regimes of superdiffusive, diffusive, and localized, behavior. Our findings show how intricate fractal-scaling entanglement can be produced for local Hamiltonians and measurements.}, archive = {J_PRL}, author = {Igor Poboiko and Marcin Szyniszewski and Christopher J. Turner and Igor V. Gornyi and Alexander D. Mirlin and Arijeet Pal}, doi = {10.1103/tx71-1cd9}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170403}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement-induced lévy flights of quantum information}, volume = {135}, year = {2025}, }
• (2025). Semigroup influence matrices for nonequilibrium quantum impurity models. PRL, 135(17), 170402. (www)

  @article{ , abstract = {We introduce a framework for describing the real-time dynamics of quantum impurity models out of equilibrium which is based on the influence matrix approach. By replacing the dynamical map of a large fermionic quantum environment with an effective semigroup influence matrix (SGIM) which acts on a reduced auxiliary space, we overcome the limitations of previous proposals, achieving high accuracy at long evolution times. This SGIM corresponds to a uniform matrix-product state representation of the influence matrix and can be obtained by an efficient algorithm presented in this Letter. We benchmark this approach by computing the spectral function of the single impurity Anderson model with high resolution. Further, the spectrum of the effective dynamical map allows us to obtain relaxation rates of the impurity toward equilibrium following a quantum quench. Finally, for a quantum impurity model with on-site two-fermion loss, we compute the spectral function and confirm the emergence of Kondo physics at large loss rates.}, archive = {J_PRL}, author = {Michael Sonner and Valentin Link and Dmitry A. Abanin}, doi = {10.1103/5gfn-l7w7}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170402}, shortjournal = {Phys. Rev. Lett.}, title = {Semigroup influence matrices for nonequilibrium quantum impurity models}, volume = {135}, year = {2025}, }
• (2025). Scaling theory of fading ergodicity. PRL, 135(17), 170401. (www)

  @article{ , abstract = {In most noninteracting quantum systems, the scaling theory of localization predicts one-parameter scaling flow in both ergodic and localized regimes. A corresponding scaling theory of many-body ergodicity breaking is still missing. Here, we introduce a scaling theory of ergodicity breaking in interacting systems, in which the divergent relaxation time follows from the Fermi golden rule, and the observable fluctuations in proximity of the ergodicity breaking critical point are described by the recently introduced fading ergodicity scenario. We argue that, in general, the one-parameter scaling is insufficient, and we show that the scaling theory predicts the critical exponent ν = 1 at the ergodicity breaking critical point. Our theoretical framework may serve as a building block for two-parameter scaling theories of many-body systems.}, archive = {J_PRL}, author = {Rafał Świętek and Miroslav Hopjan and Carlo Vanoni and Antonello Scardicchio and Lev Vidmar}, doi = {10.1103/4l42-l7pk}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170401}, shortjournal = {Phys. Rev. Lett.}, title = {Scaling theory of fading ergodicity}, volume = {135}, year = {2025}, }
• (2025). Computation and verification of spectra for non-hermitian systems. PRL, 135(17), 170202. (www)

  @article{ , abstract = {We establish a connection between quantum mechanics and computation, revealing fundamental limitations for algorithms computing spectra, especially in non-Hermitian settings. Introducing the concept of locally trivial pseudospectra, we show such assumptions are necessary for spectral computation. Locally trivial pseudospectra adapt dynamically to system energies, enabling spectral analysis across a broad class of challenging non-Hermitian problems. Exploiting this framework, we overcome a longstanding obstacle by computing the eigenvalues and eigenfunctions of the imaginary cubic oscillator with error bounds and no spurious modes—yielding, to our knowledge, the first such error-controlled result. We confirm, for instance, the 100th eigenvalue as . Here, truncation-induced -symmetry breaking causes spurious eigenvalues—a pitfall our method avoids, highlighting the link between truncation and physics. Finally, we illustrate the approach’s generality via spectral computations for a range of physically relevant operators. This Letter provides a rigorous framework linking computational theory to quantum mechanics and offers a precise tool for spectral calculations with error bounds.}, archive = {J_PRL}, author = {Catherine Drysdale and Matthew Colbrook and Michael T. M. Woodley}, doi = {10.1103/hf8s-v93b}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170202}, shortjournal = {Phys. Rev. Lett.}, title = {Computation and verification of spectra for non-hermitian systems}, volume = {135}, year = {2025}, }
• (2025). State–Entanglement-witness contraction. PRL, 135(17), 170201. (www)

  @article{ , abstract = {We construct linear and nonlinear entanglement witnesses, by tensoring and partial tracing existing states and witnesses. We show that little shared quantum resources allow one to employ decomposable witnesses to obtain larger ones detecting locally undistillable states and find analytic witnesses for multipartite entangled states that are undistillable across all bipartitions. Crucially, we show how to efficiently optimize multicopy witnesses to desired states, which is a current challenge. As an example of both theoretical and experimental interest, existing trace polynomial witnesses are significantly improved while preserving their symmetries and implementability with randomized measurements. In addition to detecting entanglement, we also find new witnesses detecting -copy distillability. A recipe for the single-copy case is shown to be effective for generic and Werner states.}, archive = {J_PRL}, author = {Albert Rico}, doi = {10.1103/d6q5-k7sh}, journal = {Physical Review Letters}, month = {10}, number = {17}, pages = {170201}, shortjournal = {Phys. Rev. Lett.}, title = {State–Entanglement-witness contraction}, volume = {135}, year = {2025}, }
• (2025). Erratum: Elastic screening of pseudogauge fields in graphene [Phys. rev. lett. 134, 046404 (2025)]. PRL, 135(16), 169901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 169901 (2025)}, archive = {J_PRL}, author = {Christophe De Beule and Robin Smeyers and Wilson Nieto Luna and E. J. Mele and Lucian Covaci}, doi = {10.1103/ptgg-frh1}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {169901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Elastic screening of pseudogauge fields in graphene [Phys. rev. lett. 134, 046404 (2025)]}, volume = {135}, year = {2025}, }
• (2025). Defects, parcellation, and renormalized negative diffusivities in nonhomogeneous oscillatory media. PRL, 135(16), 168401. (www)

  @article{ , abstract = {Spatial nonhomogeneities can synchronize clusters of spatially extended oscillators in different frequency plateaus. Motivated by physiological rhythms, we fully characterize the phase diagram of a Ginzburg-Landau (GL) model with a gradient of frequencies. For large gradients and diffusion, the rest state is stable, and the linear spectrum around it maps onto the non-Hermitian Bloch-Torrey equation. When complex pairs of eigenvalues turn unstable, precursors of plateaus grow, separated by defects where the GL amplitude vanishes. Nonlinear effects either saturate the amplitude of plateaus or lead to a phase-locked state, with saddle-node bifurcations separating the two regimes. In the region of plateaus, we trace the formation of defects to a nonlinear renormalization of the diffusivity, and determine the scaling of their number and length vs dynamical parameters.}, archive = {J_PRL}, author = {Marie Sellier-Prono and Massimo Cencini and David Kleinfeld and Massimo Vergassola}, doi = {10.1103/8njd-qd14}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {168401}, shortjournal = {Phys. Rev. Lett.}, title = {Defects, parcellation, and renormalized negative diffusivities in nonhomogeneous oscillatory media}, volume = {135}, year = {2025}, }
• (2025). Tuning steady shear rheology through active dopants. PRL, 135(16), 168302. (www)

  @article{ , abstract = {We numerically investigate the steady shear rheology of mixtures of active and passive Brownian particles, with varying fractions of active components. We find that even a small fraction of active dopants triggers fluidization with comparable efficiency to fully active systems. A combined parameter, active energy, given by the dopant fraction multiplied by the propulsion speed squared controls the steady shear rheology and glass transition of the active-passive mixtures. These results together provide a quantitative strategy for fine-tuning the mechanical properties of a soft material with small amounts of active dopants.}, archive = {J_PRL}, author = {Amir Shee and Ritwik Bandyopadhyay and Haicen Yue}, doi = {10.1103/qvr9-rvw4}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {168302}, shortjournal = {Phys. Rev. Lett.}, title = {Tuning steady shear rheology through active dopants}, volume = {135}, year = {2025}, }
• (2025). Spontaneous emergence of run-and-tumble-like dynamics in a robotic analog of chlamydomonas: Experiment and theory. PRL, 135(16), 168301. (www)

  @article{ , abstract = {Run-and-tumble (RT) motion is commonly observed in flagellated microswimmers, arising from synchronous and asynchronous flagellar beating. One such example is a biflagellated alga, called Chlamydomonas reinhardtii . Its flagellar synchronization is not only affected by hydrodynamic interactions but also through contractile stress fibers that mechanically couple the flagella, enabling adaptable swimming behavior. To explore this, we design a macroscopic mechanical system that comprises dry, self-propelled robots linked by a rigid rod to model this organism. By varying the attachment points of the two ends of the rod on each robot, the model incorporates the effect of fiber contractility observed in the real organism. To mimic a low Reynolds number environment, we program each robot to undergo overdamped active Brownian (AB) motion. We find that such a system exhibits RT-like behavior, characterized by sharp, direction-reversing tumbles and exponentially distributed run times, consistent with the real organism. Moreover, we quantify tumbling frequency and demonstrate its tunability across experimental parameters. Additionally, we provide a theoretical model that reproduces our results, elucidating physical mechanisms governing RT dynamics. Thus, our robotic system not only replicates RT motion but also captures several subtle characteristics, offering valuable insights into the underlying physics of microswimmer motility.}, archive = {J_PRL}, author = {Somnath Paramanick and Umashankar Pardhi and Harsh Soni and Nitin Kumar}, doi = {10.1103/7hcf-p1yk}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {168301}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous emergence of run-and-tumble-like dynamics in a robotic analog of chlamydomonas: Experiment and theory}, volume = {135}, year = {2025}, }
• (2025). Dynamical phase transitions in nonequilibrium networks. PRL, 135(16), 167402. (www)

  @article{ , abstract = {Dynamical phase transitions (DPTs) characterize critical changes in system behavior occurring at finite times, providing a lens to study nonequilibrium phenomena beyond conventional equilibrium physics. While extensively studied in quantum systems, DPTs have remained largely unexplored in classical settings. Recent experiments on complex systems, from social networks to financial markets, have revealed abrupt dynamical changes analogous to quantum DPTs, motivating the search for a theoretical understanding. Here, we present a minimal model for nonequilibrium networks, demonstrating that nonlinear interactions among network edges naturally give rise to DPTs. Specifically, we show that network degree diverges at a finite critical time, following a universal hyperbolic scaling, consistent with empirical observations. Our analytical results predict that key network properties, including degree distributions and clustering coefficients, exhibit critical scaling as criticality approaches. These findings establish a theoretical foundation for understanding emergent nonequilibrium criticality across diverse complex systems.}, archive = {J_PRL}, author = {Jiazhen Liu and Nathaniel M. Aden and Debasish Sarker and Chaoming Song}, doi = {10.1103/yls4-kdvj}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {167402}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical phase transitions in nonequilibrium networks}, volume = {135}, year = {2025}, }
• (2025). Principled model selection for stochastic dynamics. PRL, 135(16), 167401. (www)

  @article{ , abstract = {Complex dynamical systems, from macromolecules to ecosystems, are often modeled by stochastic differential equations. To learn such models from data, a common approach involves sparse selection among a large function library. However, we show that overfitting arises not just from individual model complexity, but also from the combinatorial growth of possible models. To address this, we introduce parsimonious stochastic inference (PASTIS), a principled method combining likelihood-estimation statistics with extreme value theory to suppress superfluous parameters. PASTIS outperforms existing methods and reliably identifies minimal models, even with low sampling rates or measurement error. It extends to stochastic partial differential equations, and applies to ecological networks and reaction-diffusion dynamics.}, archive = {J_PRL}, author = {Andonis Gerardos and Pierre Ronceray}, doi = {10.1103/ltdt-hvh7}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {167401}, shortjournal = {Phys. Rev. Lett.}, title = {Principled model selection for stochastic dynamics}, volume = {135}, year = {2025}, }
• (2025). Invariant measures in time-delay coordinates for unique dynamical system identification. PRL, 135(16), 167202. (www)

  @article{ , abstract = {While invariant measures are widely employed to analyze physical systems when a direct study of pointwise trajectories is intractable, e.g., due to chaos or noise, they cannot uniquely identify the underlying dynamics. Our first result shows that, in contrast to invariant measures in state coordinates, e.g., the invariant measure expressed in time-delay coordinates, e.g., can identify the dynamics up to a topological conjugacy. Our second result resolves the remaining ambiguity: by combining invariant measures constructed from multiple delay frames with distinct observables, the system is uniquely identifiable, provided that a suitable initial condition is satisfied. These guarantees require informative observables and appropriate delay parameters ( , ), which can be limiting in certain settings. We support our theoretical contributions through a series of physical examples demonstrating how invariant measures expressed in delay coordinates can be used to perform robust system identification in practice.}, archive = {J_PRL}, author = {Jonah Botvinick-Greenhouse and Robert Martin and Yunan Yang}, doi = {10.1103/ppys-lx68}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {167202}, shortjournal = {Phys. Rev. Lett.}, title = {Invariant measures in time-delay coordinates for unique dynamical system identification}, volume = {135}, year = {2025}, }
• (2025). Anomalous correlators, negative frequencies, and non-phase-invariant hamiltonians in random waves. PRL, 135(16), 167201. (www)

  @article{ , abstract = {We investigate a generic non-phase-invariant Hamiltonian model that governs the dynamics of nonlinear dispersive waves. We give evidence that initial data characterized by random phases naturally evolve into phase correlations between positive and negative wave numbers, leading to the emergence of nonzero anomalous correlators and negative frequencies. Using analytical techniques, we show that anomalous correlators develop on a timescale of O ( 1 / ε ) , earlier than the kinetic timescale. Our theoretical predictions are validated through direct numerical simulations of the deterministic system.}, archive = {J_PRL}, author = {A. Villois and G. Dematteis and Y. V. Lvov and M. Onorato and J. Shatah}, doi = {10.1103/3brq-j34x}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {167201}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous correlators, negative frequencies, and non-phase-invariant hamiltonians in random waves}, volume = {135}, year = {2025}, }
• (2025). Odd dynamics of passive objects in a chiral active bath. PRL, 135(16), 167102. (www)

  @article{ , abstract = {When submerged in a chiral active bath, a passive object becomes a spinning ratchet imbued with odd transport properties. We present the most general Langevin dynamics for a rigid body in a chiral active bath, in the adiabatic limit of large object mass. For rotationally symmetric objects, odd diffusion and odd mobility are connected by an Einstein relation, that we show numerically to break down outside the adiabatic limit. As the object symmetry decreases, its dynamics becomes increasingly irreversible: A massive disk exhibits an effective equilibrium dynamics, while a rod admits distinct translational and rotational temperatures, and a wedge is fully irreversible. Conversely, this departure from equilibrium can be read in universal far-field currents and density modulations of the bath, which we measure numerically and derive analytically.}, archive = {J_PRL}, author = {Cory Hargus and Federico Ghimenti and Julien Tailleur and Frédéric van Wijland}, doi = {10.1103/pdpf-sd9q}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {167102}, shortjournal = {Phys. Rev. Lett.}, title = {Odd dynamics of passive objects in a chiral active bath}, volume = {135}, year = {2025}, }
• (2025). Nested stochastic resetting: Nonequilibrium steady states and exact correlations. PRL, 135(16), 167101. (www)

  @article{ , abstract = {Stochastic resetting breaks detailed balance and drives the formation of nonequilibrium steady states. Here, we consider a chain of diffusive processes x i ( t ) that interact unilaterally: at random time intervals, the process x n stochastically resets to the instantaneous value of x n − 1 . We derive analytically the steady-state statistics of these nested stochastic resetting processes including the stationary distribution for each process as well as its moments. We are also able to calculate exactly the steady-state two-point correlations ⟨ x n x n + j ⟩ between processes by mapping the problem to one of the ordering statistics of random counting processes. Understanding statistics and correlations in many-particle nonequilibrium systems remains a formidable challenge and our results provide an example of such tractable correlations. We expect this framework will both help build a model-independent framework for random processes with unilateral interactions and find immediate applications, e.g., in the modeling of lossy information propagation.}, archive = {J_PRL}, author = {Henry Alston and Callum Britton and Thibault Bertrand}, doi = {10.1103/ccjj-6ksn}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {167101}, shortjournal = {Phys. Rev. Lett.}, title = {Nested stochastic resetting: Nonequilibrium steady states and exact correlations}, volume = {135}, year = {2025}, }
• (2025). Photomagnetic-chiral anisotropy mediated by chirality-driven asymmetric spin splitting. PRL, 135(16), 166903. (www)

  @article{ , abstract = {Photomagnetic effects (PMEs), intrinsic to transition metals, arise from the interaction between light-induced angular momentum and electronic spin. These effects are suppressed in noble metals with high symmetry and electron density. Introducing chiral structures can induce photomagnetic-chiral anisotropy (PMChA) of metals by linking chirality and spin dynamics. However, a theoretical explanation remains elusive. Here, we investigated the mechanism of PMChA in tetrahelix-stacked chiral nanostructured Au chains (CNACs) using first-principles calculations. Nonequilibrium Green’s function calculations reveal that chiral potentials enhance spin channel asymmetry by amplifying spin-orbit coupling (SOC)-induced spin splitting. Real-time time-dependent density functional theory simulations further identify SOC as the bridge connecting chiral spintronics to PMEs, where chirality-driven spin flips from asymmetric geometries generate opposing photomagnetic fields in materials of different handedness. These findings are consistent with experimental observations in chiral nanostructured gold films and provide theoretical guidance for designing metallic spintronic devices.}, archive = {J_PRL}, author = {Tianwei Ouyang and Hang Su and Wanning Zhang and Yingying Duan and Yuxi Fang and Shunai Che and Yizhou Liu}, doi = {10.1103/llys-8b4p}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166903}, shortjournal = {Phys. Rev. Lett.}, title = {Photomagnetic-chiral anisotropy mediated by chirality-driven asymmetric spin splitting}, volume = {135}, year = {2025}, }
• (2025). Phase matching of high harmonic generation in twisted van der waals crystals. PRL, 135(16), 166902. (www)

  @article{ , abstract = {High harmonic generation (HHG) in crystals could enable attosecond and ultraviolet light sources with high compactness, great controllability, and rich functions. However, the HHG process is accompanied by a quite large wave vector mismatch that is uncompensated by any traditional phase-matching method, directly limiting its energy conversion efficiency. Here, we propose an effective strategy for phase matching of HHG with arbitrary harmonic orders in crystals. Two flakes of twisted van der Waals crystals induce a nonlinear optical phase that depends on the crystal symmetry, twist angle, and harmonic order, which can be accurately designed to compensate for the phase mismatch in HHG. Guided by the twist-phase-matching theory, we achieved a record-high conversion efficiency of ∼ 4 × 10 − 5 for the fifth HHG in twisted hexagonal boron nitride crystals within thickness of ∼ 1 μ m . Moreover, the designed crystal has the polarization controllability that can emit a pure circularly polarized HHG light. Our Letter establishes a foundation for developing ultrashort-wavelength and ultrafast-pulse laser sources in compact solid-state tabletop systems for fundamental and applied sciences.}, archive = {J_PRL}, author = {Chenjun Ma and Chen Huang and Yilong You and Huazhan Liu and Zhitong Ding and Mingchao Ding and Chang Liu and Jin Zhang and Guixin Li and Zhipei Sun and Shiwei Wu and Chaojie Ma and Enge Wang and Hao Hong and Kaihui Liu}, doi = {10.1103/kskc-qlb3}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166902}, shortjournal = {Phys. Rev. Lett.}, title = {Phase matching of high harmonic generation in twisted van der waals crystals}, volume = {135}, year = {2025}, }
• (2025). Topologically tunable polaritons based on a two-dimensional crystal in a photonic lattice. PRL, 135(16), 166901. (www)

  @article{ , abstract = {Structured optical cavities have advanced as a powerful test bed to study lattice Hamiltonians in general, and topological phenomena in particular. The in situ tuning of topological modes, enabled via substantial modifications of emulated lattice potentials, has remained out of experimental reach due to the commonly utilized monolithic cavity samples. Here, we study the Su-Schrieffer-Heeger (SSH) lattice Hamiltonian, which we emulate in a widely tunable open optical cavity strongly coupled to excitons in an integrated monolayer. The potential landscape comprises a topological domain boundary hosting a topological, exponentially localized mode at the interface between two lattices characterized by different Zak phases. The mode is spectrally tunable over 80 meV. Moreover, we use the unique tilt tunability of our implementation to transform the SSH lattice into a Stark ladder. This transformation couples the topologically protected defect mode to propagating lattice modes and effectively changes the symmetry of the system. Furthermore, it allows us to directly quantify the Zak-phase difference between the two topological phases. Our Letter constitutes an important step toward in situ tuning topological lattices to control and guide light on nonlinear chips.}, archive = {J_PRL}, author = {L. Lackner and O. A. Egorov and A. Ernzerhof and C. Bennenhei and V. N. Mitryakhin and G. Leibeling and F. Eilenberger and S. Tongay and U. Peschel and M. Esmann and C. Schneider}, doi = {10.1103/qphl-qd37}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166901}, shortjournal = {Phys. Rev. Lett.}, title = {Topologically tunable polaritons based on a two-dimensional crystal in a photonic lattice}, volume = {135}, year = {2025}, }
• (2025). Magnon-magnon interaction induced by nonlinear spin-wave dynamics. PRL, 135(16), 166703. (www)

  @article{ , abstract = {We experimentally and theoretically demonstrate that nonlinear spin-wave dynamics can induce an effective resonant interaction between nonresonant magnon modes in a yttrium iron garnet disk. Under strong pumping near the ferromagnetic resonance mode, we observe a spectral splitting that emerges with increasing drive amplitude. This phenomenon is well captured by a theoretical framework based on the linearization of a magnon three-wave mixing Hamiltonian, which at high power leads to parametric Suhl instabilities. The access and control of nonlinear magnon-parametric processes enable the development of experimental platforms in an unexplored parameter regime for both classical and quantum computation protocols.}, archive = {J_PRL}, author = {Matteo Arfini and Alvaro Bermejillo-Seco and Artem Bondarenko and Clinton A. Potts and Yaroslav M. Blanter and Herre S. J. van der Zant and Gary A. Steele}, doi = {10.1103/jnpb-2mxx}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166703}, shortjournal = {Phys. Rev. Lett.}, title = {Magnon-magnon interaction induced by nonlinear spin-wave dynamics}, volume = {135}, year = {2025}, }
• (2025). Shot noise of photocurrents in magnetic quantum materials. PRL, 135(16), 166702. (www)

  @article{ , abstract = {Recently, the dc shot noise (DSN) of photocurrents has been proposed as its complementary probe to quantify the nonmagnetic gapped quantum materials. In this Letter, we have discovered two novel DSN terms that are crucial for understanding the properties of magnetically insulating quantum materials: linear magnetic shift DSN and circular magnetic injection DSN. Both magnetic shift and injection DSNs inherit quantum geometric information of Bloch states. Interestingly, these terms can appear only when the system breaks parity-time ( P T ) symmetry. Leveraging this unique symmetry sensitivity, we propose DSN as a noninvasive, symmetry-resolved diagnostic capable of distinguishing magnetic properties. We demonstrate the viability of this approach through both minimal altermagnet models and first-principles calculations of realistic monolayer and bilayer CrI 3 in various magnetic configurations. We show that magnetic DSN not only captures the spin-split band structure of altermagnets, but also differentiates magnetic phases and parity of the number of layers in two-dimensional CrI 3 . This establishes DSN as a powerful tool for probing symmetry, quantum geometry, and spin textures in magnetic quantum materials.}, archive = {J_PRL}, author = {Xinyue Liu and Longjun Xiang and Yaqing Yang and Fuming Xu and Jun Chen and Lei Zhang and Jian Wang}, doi = {10.1103/nsky-zmzp}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166702}, shortjournal = {Phys. Rev. Lett.}, title = {Shot noise of photocurrents in magnetic quantum materials}, volume = {135}, year = {2025}, }
• (2025). Altermagnets with topological order in kitaev bilayers. PRL, 135(16), 166701. (www)

  @article{ , abstract = {Building on recent advancements in altermagnetism, we develop a highly frustrated magnetic model with Kitaev-like interactions that integrates key aspects of both quantum spin liquids and altermagnets. While the ground state is a gapless quantum spin liquid, our analysis indicates that an altermagnetic local order emerges upon the introduction of additional interactions that gap the excitation spectrum and give rise to a Z 2 topological order. This magnetically fragmented topological altermagnet has fractionalized fermionic excitations with momentum-dependent splitting, in stark contrast to both standard altermagnets and Kitaev spin liquids. In addition, we discover two more altermagnetic phases, including a pseudoaltermagnet that exhibits splitting in the absence of a local order and a half-altermagnet that possesses only one type of fractionalized excitation, similar to a half-metal. We discuss experimental approaches for detecting these phases, including layer-dependent spin and heat transport. Our results highlight the rich physics that can arise due to the interplay between altermagnetism and fractionalized excitations in quantum magnets.}, archive = {J_PRL}, author = {Aayush Vijayvargia and Ezra Day-Roberts and Antia S. Botana and Onur Erten}, doi = {10.1103/km2j-3zy2}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166701}, shortjournal = {Phys. Rev. Lett.}, title = {Altermagnets with topological order in kitaev bilayers}, volume = {135}, year = {2025}, }
• (2025). Multiband fractional thouless pumps. PRL, 135(16), 166601. (www)

  @article{ , abstract = {Quantization of particle transport lies at the heart of topological physics. In Thouless pumps—dimensionally reduced versions of the integer quantum Hall effect—quantization is dictated by the integer winding of single-band Wannier states. Here, we show that repulsive interactions can drive a transition from an integer- to a fractional-quantized Thouless pump (at fixed integer filling) by stabilizing a crystal of multiband Wannier states, each with fractional winding. We numerically illustrate the concept in few-particle systems and show that a dynamical Hartree-Fock ansatz can quantitatively reproduce the pumping phase diagram.}, archive = {J_PRL}, author = {Marius Jürgensen and Jacob Steiner and Gil Refael and Mikael C. Rechtsman}, doi = {10.1103/4d5s-n4gn}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166601}, shortjournal = {Phys. Rev. Lett.}, title = {Multiband fractional thouless pumps}, volume = {135}, year = {2025}, }
• (2025). Critical gate distance for wigner crystallization in the two-dimensional electron gas. PRL, 135(16), 166501. (www)

  @article{ , abstract = {In devices based on two-dimensional electron gases (2DEGs), gate electrodes can be used to tune the electronic properties by controlling the electron density. Despite the prevalence of such gated systems, the properties of 2DEGs in these environments remain poorly understood quantitatively. To address this, we have studied the 2DEG in a dual-gate geometry using quantum Monte Carlo simulations alongside simpler approximate methods, and we have mapped out the phase diagram of the gated 2DEG as a function of electron density and gate distance. We find that the Wigner crystal is unstable at all densities when the gates are sufficiently close to the 2DEG, and we identify the critical gate distance at which the Wigner crystal phase appears. For larger gate separations, we determine the phase boundary for the reentrant crystal to liquid transition that occurs with decreasing density. Our Letter is particularly relevant to Wigner crystal phases recently observed in a variety of gated two-dimensional materials.}, archive = {J_PRL}, author = {Agnes Valenti and Vladimir Calvera and Yubo Yang (杨煜波 and Miguel A. Morales and Steven A. Kivelson and Ilya Esterlis and Shiwei Zhang}, doi = {10.1103/2qgp-v27h}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166501}, shortjournal = {Phys. Rev. Lett.}, title = {Critical gate distance for wigner crystallization in the two-dimensional electron gas}, volume = {135}, year = {2025}, }
• (2025). Identifying electronic doorway states in secondary electron emission from layered materials. PRL, 135(16), 166401. (www)

  @article{ , abstract = {We investigate the secondary low-energy electron emission induced by inelastic electron scattering from graphene and layered materials thereof. By applying a coincidence detection of the primary scattered and the emitted secondary electron we unravel pronounced resonance features otherwise overshadowed by the largely structureless secondary electron energy distribution. Supported by density functional theory calculations we show that these structures are the signature of prominent resonances above the vacuum threshold which originate from interlayer states acting as a doorway state for electron emission. Remarkably, some of these doorway states open up only for samples with more than five layers.}, archive = {J_PRL}, author = {A. Niggas and M. Hao and P. Richter and F. Simperl and F. Blödorn and M. Cap and J. Kero and D. Hofmann and A. Bellissimo and J. Burgdörfer and T. Seyller and R. A. Wilhelm and F. Libisch and W. S. M. Werner}, doi = {10.1103/qls7-tr4v}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166401}, shortjournal = {Phys. Rev. Lett.}, title = {Identifying electronic doorway states in secondary electron emission from layered materials}, volume = {135}, year = {2025}, }
• (2025). Unconventional hall effect in gapless superconductors: Transverse supercurrent converted from normal current. PRL, 135(16), 166304. (www)

  @article{ , abstract = {A normal metal proximitized by a superconductor can exhibit a gapless superconducting state characterized by segmented Fermi surfaces, as confirmed experimentally. In this state, quasiparticle states remain gapless along one direction, while a superconducting gap opens in the perpendicular direction. We show that this anisotropic phase enables an unconventional Hall effect in gapless superconductors, termed the superconducting Hall effect (ScHE), in which a longitudinal quasiparticle current is converted into a dissipationless transverse supercurrent without a phase transition. Using both the thermodynamic approach for bulk systems and quantum transport theory for a four-probe setup, we demonstrate the existence of this effect and reveal its intrinsic origin as the quasiparticle Berry curvature. The predicted ScHE can be experimentally verified via angular-dependent Hall measurements performed on gapless superconductors, such as Bi 2 Te 3 proximitized by superconducting NbSe 2 as well as altermagnetic materials coupled to superconductors.}, archive = {J_PRL}, author = {Miaomiao Wei and Longjun Xiang and Fuming Xu and Bin Wang and Jian Wang}, doi = {10.1103/fql8-f3tl}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166304}, shortjournal = {Phys. Rev. Lett.}, title = {Unconventional hall effect in gapless superconductors: Transverse supercurrent converted from normal current}, volume = {135}, year = {2025}, }
• (2025). Superdiffusive transport in chaotic quantum systems with nodal interactions. PRL, 135(16), 166303. (www)

  @article{ , abstract = {We introduce a class of interacting fermionic quantum models in dimensions with nodal interactions that exhibit superdiffusive transport. We establish nonperturbatively that the nodal structure of the interactions gives rise to long-lived quasiparticle excitations that result in a diverging diffusion constant, even though the system is fully chaotic. Using a Boltzmann equation approach, we find that the charge mode acquires an anomalous dispersion relation at long wavelength with dynamical exponent , where is the order of the nodal point in momentum space. We verify our predictions in one-dimensional systems using tensor-network techniques.}, archive = {J_PRL}, author = {Yu-Peng Wang and Jie Ren and Sarang Gopalakrishnan and Romain Vasseur}, doi = {10.1103/xx9z-4j6c}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166303}, shortjournal = {Phys. Rev. Lett.}, title = {Superdiffusive transport in chaotic quantum systems with nodal interactions}, volume = {135}, year = {2025}, }
• (2025). Kinetic uncertainty relations for quantum transport. PRL, 135(16), 166302. (www)

  @article{ , abstract = {We analyze the precision of generic currents in a multiterminal quantum-transport setting. Employing scattering theory, we show that the precision of such currents is limited by a function of the particle-current noise that can be interpreted as the activity in the classical limit. We thereby establish a kinetic uncertainty relation for quantum transport. In the full quantum limit, we find precision bounds with modified activity constraints depending on whether the system is fermionic or bosonic. We expect these bounds to be suitable as guidelines for any transport process aiming at high precision.}, archive = {J_PRL}, author = {Didrik Palmqvist and Ludovico Tesser and Janine Splettstoesser}, doi = {10.1103/kvdn-skn1}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166302}, shortjournal = {Phys. Rev. Lett.}, title = {Kinetic uncertainty relations for quantum transport}, volume = {135}, year = {2025}, }
• (2025). Electrically detected magnetic resonance in ambipolar polymer field-effect transistors. PRL, 135(16), 166301. (www)

  @article{ , abstract = {Electron spin resonance can provide unique insights into charge transport processes in organic semiconductors in a regime in which charge motion determines spin relaxation. In particular, electrically detected magnetic resonance (EDMR) probes directly the changes in charge transport properties that are sensitive to magnetic resonance excitation. Here, we present a systematic study of continuous-wave EDMR on conjugated polymer field-effect transistors (FETs) that can be operated in both unipolar as well as ambipolar regimes. We show that, in addition to a narrow, electron-hole recombination-induced EDMR signal that can only be detected in the ambipolar regime, there is also a broad EDMR signal when devices are operated in both unipolar and ambipolar regions. We attribute this signal to a spin blockade mechanism induced when mobile carriers encounter trapped charges along the charge transport percolation pathways and study its dependence on biasing conditions and temperature. The spin-blockade EDMR signature is also observed in conjugated polymer FETs that exhibit only unipolar operation. Our findings show that EDMR provides a powerful technique to study the role of spin blockade and bipolaron formation on the charge transport properties of a wide range of conjugated polymers.}, archive = {J_PRL}, author = {Zichen Wang and Ilia Kulikov and Tarig Mustafa and Sam Schott and Remington L. Carey and Jan Behrends and Henning Sirringhaus}, doi = {10.1103/7b3m-8zvz}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166301}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically detected magnetic resonance in ambipolar polymer field-effect transistors}, volume = {135}, year = {2025}, }
• (2025). Defect-free growth of decagonal quasicrystals around obstacles. PRL, 135(16), 166203. (www)

  @article{ , abstract = {Quasicrystals are aperiodic solids with exotic physical properties. The mechanisms driving their growth are far from understood, particularly in the presence of rigid obstacles. Using in situ synchrotron x-ray tomography and molecular dynamics simulations, we investigate the interaction between decagonal quasicrystals and obstacles (shrinkage pores) during solidification of an alloy. The results reveal defect-free quasicrystal growth around the pores, independent of pore size and geometry. Our findings point to a universal feature of aperiodic solids: their ability to accommodate structural disruptions due to additional (phasonic) degrees of freedom. This Letter opens new possibilities for synthesizing large-scale, single quasicrystals from a liquid metal precursor.}, archive = {J_PRL}, author = {Kelly L. Wang and Insung Han and Domagoj Fijan and Sharon C. Glotzer and Ashwin J. Shahani}, doi = {10.1103/bsbs-rryl}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166203}, shortjournal = {Phys. Rev. Lett.}, title = {Defect-free growth of decagonal quasicrystals around obstacles}, volume = {135}, year = {2025}, }
• (2025). Transition from near-field to extreme near-field radiative heat transfer. PRL, 135(16), 166202. (www)

  @article{ , abstract = {The radiative heat transfer in the extreme near-field regime, i.e., for distances below 10 nm, remains poorly understood. There are competing experimental results in this regime, with some in good agreement with theoretical predictions, while others report drastically elevated heat fluxes, orders of magnitude larger than what theory suggests. Whether the theory of fluctuational electrodynamics can predict the radiative heat transfer in this extreme near-field regime or not remains a matter of active debate. In this Letter, a radiative heat transfer measurement is presented between a gold-coated sphere and a gold film sample in the transition regime between the near-field and the extreme near-field regime just before contact. The radiative heat flux measurement is made by using a near-field scanning thermal microscope equipped with a temperature sensor at a sharp tip as a heat flux sensor. We find an excellent agreement with the theoretical predictions of fluctuational electrodynamics in the near-field regime. In the extreme near-field regime, however, a highly increased radiative heat flux is observed with values about 100 times larger than the theoretical predictions, indicating that fluctuational electrodynamics fails to capture the radiative heat flux in this regime.}, archive = {J_PRL}, author = {F. Geesmann and P. Thurau and S. Rodehutskors and T. Ziehm and L. Worbes and S.-A. Biehs and A. Kittel}, doi = {10.1103/lcz1-f5v9}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166202}, shortjournal = {Phys. Rev. Lett.}, title = {Transition from near-field to extreme near-field radiative heat transfer}, volume = {135}, year = {2025}, }
• (2025). Imaging sublattice cooper-pair density waves in monolayer 1 T′−MoTe2. PRL, 135(16), 166201. (www)

  @article{ , abstract = {Unconventional superconductors that spontaneously break space-group symmetries of their underlying crystal lattice are distinguished by spatial modulations of superconducting order parameter. These states have recently captured significant attention in various strongly correlated materials, where the translational or intra-unit-cell symmetry breaking results in the emergence of pair density waves with wavelength extending across one or multiple unit cells. Here, we employ a spectroscopic-imaging scanning tunneling microscopy to reveal sublattice modulations of the superconducting gap magnitude, coherence strength, and subgap states in tunable monolayer. These modulations are uniquely oriented perpendicular to the zigzag Mo chains at the scale of half a unit cell and coexist with three-unit-cell pair density wave modulations along the Mo chains, both of which attenuate with increasing temperature and external magnetic fields. Importantly, we find that the superconductivity modulations are strongly linked to unconventional electron pairing mechanisms, which significantly deviate from the Cooper pairing observed in conventional Bardeen-Cooper-Schrieffer superconductors. Our findings advance the knowledge of Cooper-pair density modulations and their intricate interplay with other symmetry-breaking states in strongly correlated superconductors.}, archive = {J_PRL}, author = {Fang-Jun Cheng and Cong-Cong Lou and Ai-Xi Chen and Li-Xuan Wei and Yu Liu and Bo-Yuan Deng and Fangsen Li and Ziqiang Wang and Qi-Kun Xue and Xu-Cun Ma and Can-Li Song}, doi = {10.1103/x6k9-wgk9}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166201}, shortjournal = {Phys. Rev. Lett.}, title = {Imaging sublattice cooper-pair density waves in monolayer 1 T′−MoTe2}, volume = {135}, year = {2025}, }
• (2025). Quantitative role of phonons and elasticity in tuning uniaxial negative thermal expansion of MZr2(M=Fe,Co, and ni). PRL, 135(16), 166101. (www)

  @article{ , abstract = {Elucidating the mechanisms of negative thermal expansion (NTE) not only identifies the determining factors of this phenomenon but also provides guidance for the precise regulation of the coefficient of thermal expansion (CTE). However, accurately quantifying these determining factors during CTE modulation remains a critical challenge. In this Letter, we quantitatively determine the respective contributions of phonon-derived Grüneisen parameters (axial values and their difference) and elastic compliance tensors to the tuning of axial NTE in the M Zr 2 system. Through temperature dependence of the neutron total scattering data (for neutron powder diffraction and neutron pair distribution function analyses), extended x-ray absorption fine structure, synchrotron x-ray diffraction, and first-principles calculations, it provides insight into the quantified roles of phonons and anisotropic elasticity in controlling the broad-range CTE. As the number of M − 3 d electrons grows, phonons, which are the dominant factors, weaken NTE, while elasticity, playing a cross-linking coefficient, enhances NTE. The current study not only provides deep insights into the origins of NTE in the M Zr 2 system, but it also offers a novel perspective on the quantifiable control of NTE in anisotropic materials.}, archive = {J_PRL}, author = {Meng Xu and Qilong Gao and Yongqiang Qiao and Kaiyue Zhao and Andrea Sanson and Qiang Sun and Changtian Wang and Alessandro Venier and Francesco d’Acapito and Matt Tucker and Yuzhu Song and Chang Zhou and Xianran Xing and Jun Chen}, doi = {10.1103/35ff-84fc}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166101}, shortjournal = {Phys. Rev. Lett.}, title = {Quantitative role of phonons and elasticity in tuning uniaxial negative thermal expansion of MZr2(M=Fe,Co, and ni)}, volume = {135}, year = {2025}, }
• (2025). Superconductivity at 28 k in sodium graphite intercalation compound under high pressure. PRL, 135(16), 166003. (www)

  @article{ , abstract = {The discovery of 15.1 K superconductivity in first-stage CaC 6 reignited interest in searching for high-temperature superconductors in graphite intercalation compounds (GICs). However, despite nearly two decades of intensive research, progress in exploring high-temperature superconductivity in GIC materials has remained stagnant. Currently, research on the superconductivity of GICs mainly focuses on first-stage GICs, while the superconductivity of high-stage GICs has been largely overlooked. Here, we report an experimental discovery of superconductivity with maximum critical temperature ( T c ) of approximately 28 K in sodium carbide at about 14 GPa evidenced by a sharp drop of resistance and a characteristic decrease of T c under magnetic fields up to 6 T. The upper critical field μ 0 H c 2 ( 0 ) was estimated to be 8.8 T based on fitting with the Ginzburg-Landau superconducting model while the coherent length is approximately 61.2 Å . X-ray diffraction measurements combined with crystal structure predictions identified the superconducting candidate material as the second-stage GIC NaC 8 , in which sodium atoms occupy the interlayer spaces between AA-stacked bilayer graphene. The current findings not only achieve the long-sought high- T c GICs, but more importantly, open up a new avenue for exploring high-temperature superconductors in light-element compounds.}, archive = {J_PRL}, author = {Guangchen Ma and Yingying Wang and Zefang Wang and Yuki Nakamoto and Katsuya Shimizu and Guangtao Liu and Mi Zhou and Hongbo Wang and Pengyue Gao and Yanming Ma}, doi = {10.1103/2t6l-sqmj}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166003}, shortjournal = {Phys. Rev. Lett.}, title = {Superconductivity at 28 k in sodium graphite intercalation compound under high pressure}, volume = {135}, year = {2025}, }
• (2025). Selective excitation of collective modes in multiband superconductor MgB2. PRL, 135(16), 166002. (www)

  @article{ , abstract = {Recent developments in nonequilibrium and nonlinear terahertz (THz) spectroscopies have significantly advanced the understanding of collective excitations in superconductors. However, there is ongoing debate regarding the identification of Higgs, Leggett modes, and BCS charge fluctuations in the two-band superconductor MgB 2 . To address this issue, we have demonstrated the selective excitation of collective modes in MgB 2 by systematically adjusting THz pump pulse characteristics. Using multicycle THz pump-probe spectroscopy, we distinguish various nonlinear processes through two-dimensional scans. The π -band Higgs mode is identified through its characteristic resonant enhancement at the temperatures where the pump frequency ω p matches the π -band superconductivity gap 2 Δ π ( T ) . In contrast, employing single-cycle THz pulses that satisfy nonadiabatic excitation conditions reveals a heavily damped oscillation corresponding to the Leggett mode. Our observed mode-selective responses in MgB 2 under tailored excitation provide a clear experimental route to discriminate between the modes, helping to reconcile existing controversies while highlighting the critical role of interband coupling in collective mode observation for multiband superconductors.}, archive = {J_PRL}, author = {Jiayu Yuan and Liyu Shi and Tiequan Xu and Yue Wang and Zizhao Gan and Hao Wang and Tianyi Wu and Dong Wu and Tao Dong and Nanlin Wang}, doi = {10.1103/b5h4-ppdf}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166002}, shortjournal = {Phys. Rev. Lett.}, title = {Selective excitation of collective modes in multiband superconductor MgB2}, volume = {135}, year = {2025}, }
• (2025). Dissipative superfluidity in a molecular bose-einstein condensate. PRL, 135(16), 166001. (www)

  @article{ , abstract = {Motivated by recent experimental realization of a Bose-Einstein condensate (BEC) of dipolar molecules, we develop superfluid transport theory for a dissipative BEC to show that a weak uniform two-body loss can induce phase rigidity, leading to superfluid transport of bosons without repulsive interactions. A generalized -sum rule is shown to hold for a dissipative superfluid as a consequence of weak U(1) symmetry. We also demonstrate that dissipation enhances the stability of a molecular BEC with dipolar interactions. Possible experimental signatures of dissipative superfluidity are discussed.}, archive = {J_PRL}, author = {Hongchao Li and Xie-Hang Yu and Masaya Nakagawa and Masahito Ueda}, doi = {10.1103/ww8r-sjhb}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {166001}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipative superfluidity in a molecular bose-einstein condensate}, volume = {135}, year = {2025}, }
• (2025). Femtosecond and attosecond phase-space correlations in few-particle photoelectron pulses. PRL, 135(16), 165002. (www)

  @article{ , abstract = {Temporal correlations in pulsed electron beams reflect the microscopic dynamics of emission and interparticle interaction. In femtosecond electron emission from nanoscale field emitters, Coulomb interactions result in structured few-electron states with strong correlations in energy, time, and transverse momentum. Interactions with external fields may be used to both probe and further manipulate these correlated states. Here, we combine femtosecond-gated, event-based detection with inelastic electron-light scattering to directly map the photoelectron phase-space distribution of two-electron states. Our experiments demonstrate a bimodal structure in longitudinal phase space, with distinct contributions from interparticle interaction and dispersion. Moreover, we imprint a global phase modulation onto two-electron states and theoretically show that coherent shaping of few-electron phase-space distributions enables attosecond temporal correlations. This controlled phasing of few-electron states can be harnessed to produce tailored excitations and superradiance via two-electron energy postselection.}, archive = {J_PRL}, author = {Rudolf Haindl and Valerio Di Giulio and Armin Feist and Claus Ropers}, doi = {10.1103/lylq-m63c}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {165002}, shortjournal = {Phys. Rev. Lett.}, title = {Femtosecond and attosecond phase-space correlations in few-particle photoelectron pulses}, volume = {135}, year = {2025}, }
• (2025). Relativistic oscillating window driven by an intense laguerre-gaussian laser pulse. PRL, 135(16), 165001. (www)

  @article{ , abstract = {High-order harmonic generation by the diffraction of an intense Laguerre-Gaussian (LG) laser beam through a small aperture is studied. It is found that the 2D peripheral electron dynamics at the boundary of the diffraction aperture can facilitate complex interplay between the spin and orbital angular momentum interaction, which leads to distinct selection rules for LG pulses with different polarization states. In particular, when the driver is linearly polarized, each harmonic beam contains multiple LG modes with different topological charges. The number of modes equals to the harmonic order and the total angular momentum is conserved during this process. A theory is derived and validated by simulations, which can predict the harmonic topological charges as well as their relative intensities for LG drivers with different polarization states. Our Letter provides fundamental insight into the behavior of light in nonlinear optics and paves the way toward high-intensity UV or x-ray pulses carrying controllable orbital angular momentum that can serve as versatile tools at frontiers of various scientific fields.}, archive = {J_PRL}, author = {Yao Meng and Runze Li and Longqing Yi}, doi = {10.1103/tww5-w4fk}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {165001}, shortjournal = {Phys. Rev. Lett.}, title = {Relativistic oscillating window driven by an intense laguerre-gaussian laser pulse}, volume = {135}, year = {2025}, }
• (2025). Persistence in physical systems: An application to soil moisture memory. PRL, 135(16), 164201. (www)

  @article{ , abstract = {Several physical variables and fluid systems exhibit memory effects arising from their internal dynamics and interactions with external forcings. Various existing techniques are either complex or face limitations due to the usual nonlinear nature of the time series, typically overestimating memory timescales. We overcome this by considering a nonparametric, model-free framework grounded in information theory, with methodological modifications to estimate memory timescales. We show that there is a good agreement between the estimated memory and the known Markov order of some synthetic time series. Leveraging this method, we analyzed observational and reanalysis datasets of soil moisture (SM) time series over India’s core monsoon zone and quantified SM memory. Results indicate that SM behaves as a finitary, higher order Markov process, revealing a memory timescale of on core monsoon zone. The proposed treatment offers methodological simplicity and generalization beyond conventional linear approaches for analyzing stationary time series.}, archive = {J_PRL}, author = {Madhusudan Ingale and Bhupendra Bahadur Singh and Milind Mujumdar and Mangesh Goswami and Naresh Ganeshi and C. D. Aju and R. Krishnan and M. Ravichandran}, doi = {10.1103/djz5-2lsn}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {164201}, shortjournal = {Phys. Rev. Lett.}, title = {Persistence in physical systems: An application to soil moisture memory}, volume = {135}, year = {2025}, }
• (2025). Two-dimensional topological edge states in periodic space-time interfaces. PRL, 135(16), 163801. (www)

  @article{ , abstract = {Topological edge states in systems of two (or more) dimensions offer scattering-free transport, exhibiting robustness to inhomogeneities and disorder. In a different domain, time-modulated systems, such as photonic time crystals, offer nonresonant amplification drawing energy from the modulation. Combining these concepts, we explore topological systems that vary periodically in both time and space, manifesting the best of both worlds. We present topological phases and topological edge states in photonic space-time crystals—materials in which the refractive index varies periodically in both space and time, displaying band gaps in both frequency and momentum. The topological nature of this system leads to topological invariants that govern the phase between refracted and reflected waves generated from both the spatial and the temporal interfaces. The 2D (1D space + 1D time) nature of this system leads to propagating edge states, and a unique edge state that grows exponentially in amplitude while following the space-time edge.}, archive = {J_PRL}, author = {Ohad Segal and Yonatan Plotnik and Eran Lustig and Yonatan Sharabi and Moshe-Ishay Cohen and Alexander Dikopoltsev and Mordechai Segev}, doi = {10.1103/5hf5-pg3t}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163801}, shortjournal = {Phys. Rev. Lett.}, title = {Two-dimensional topological edge states in periodic space-time interfaces}, volume = {135}, year = {2025}, }
• (2025). Photoionization-induced floquet driving of a discrete time crystal in a thermal rydberg ensemble. PRL, 135(16), 163603. (www)

  @article{ , abstract = {Nonequilibrium, strongly interacting systems exhibit rich dynamics even in the presence of strong dissipation. For example, periodic dynamics, such as discrete time crystalline (DTC) phases, can appear. The DTC phase structure can be further enriched using external periodic driving—Floquet driving. In this Letter, we study a photoionization-induced Floquet driving of a DTC phase in a thermal Rydberg gas. We add an additional laser to induce photoelectrons from the cell wall. These electrons are rotated around the magnetic-field vector and collide with the Rydberg atoms, generating a plasma with large electric fields that perturb further Rydberg excitation. This results in a photoionization-induced Floquet driving of the DTC phase. Importantly, we demonstrate experimentally how the DTC phase relies on the emergence of bistability. Simulations of the mean-field Floquet-driven system reproduce the experimental observations. Our Letter fills an experimental gap in our understanding of the relation of multistability and dissipative discrete time crystals, and in this regard, it constitutes a highly controlled platform for exploring exotic nonequilibrium physics in dissipative interacting systems.}, archive = {J_PRL}, author = {Yuechun Jiao and Yu Zhang and Jingxu Bai and Suotang Jia and C. Stuart Adams and Zhengyang Bai and Heng Shen and Jianming Zhao}, doi = {10.1103/1c1k-bv7z}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163603}, shortjournal = {Phys. Rev. Lett.}, title = {Photoionization-induced floquet driving of a discrete time crystal in a thermal rydberg ensemble}, volume = {135}, year = {2025}, }
• (2025). Addressing the correlation of stokes-shifted photons emitted from two quantum emitters. PRL, 135(16), 163602. (www)

  @article{ , abstract = {In resonance fluorescence excitation experiments, light emitted from solid-state quantum emitters is typically filtered to eliminate the laser photons, ensuring that only red-shifted Stokes photons are detected. However, theoretical analyses of the fluorescence intensity correlation often model emitters as two-level systems, focusing on light emitted exclusively from the purely electronic transition (the zero-phonon line), or they rely on statistical approaches based on conditional probabilities that neglect the quantum coherence between the emitters and the coherence between the electric fields they generate. Here, we propose a model to characterize the correlation of either zero-phonon line photons or Stokes-shifted photons. This model successfully reproduces the experimental correlation of Stokes-shifted photons emitted from two interacting molecules and predicts that this correlation is affected by quantum coherence. Besides, we analyze the role of quantum coherence in the Stokes-shifted emission from two distant emitters, showing a sharp peak at zero time delay due to the Hanbury Brown–Twiss effect.}, archive = {J_PRL}, author = {Adrián Juan-Delgado and Jean-Baptiste Trebbia and Ruben Esteban and Quentin Deplano and Philippe Tamarat and Rémi Avriller and Brahim Lounis and Javier Aizpurua}, doi = {10.1103/1z52-p73t}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163602}, shortjournal = {Phys. Rev. Lett.}, title = {Addressing the correlation of stokes-shifted photons emitted from two quantum emitters}, volume = {135}, year = {2025}, }
• (2025). Meissner-like currents of photons in anomalous superradiant phases. PRL, 135(16), 163601. (www)

  @article{ , abstract = {We present Meissner-like photon currents in a quantum Rabi zigzag chain under staggered synthetic magnetic fields. The ground state of the Meissner superradiant phase hosts persistent chiral edge currents in a sequence of cancellation of antiparallel vortex pairs, akin to surface currents of the Meissner effect in superconductors. The Meissner phase displays distinct vortex structures and anomalous scaling exponents, arising from geometric frustration effects. Modifying the staggered flux triggers transitions to even- or odd-vortex superradiant phases, where the chiral edge currents flow exclusively in even or odd cavities with localized vortices, respectively. Enhanced interspecies interactions induce the vanishing of currents in a ferromagnetic superradiant phase. Our results enable observation of stabilized photon vortices and edge currents with analogy to quantum Hall-like robustness in light-matter coupling systems.}, archive = {J_PRL}, author = {Linjun Li and Pengfei Huang and Zi-Xiang Hu and Yu-Yu Zhang}, doi = {10.1103/qj5x-t71k}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163601}, shortjournal = {Phys. Rev. Lett.}, title = {Meissner-like currents of photons in anomalous superradiant phases}, volume = {135}, year = {2025}, }
• (2025). Attosecond optical orientation. PRL, 135(16), 163201. (www)

  @article{ , abstract = {Circularly polarized light offers opportunities to probe symmetry-dependent properties of matter such as chirality and spin. Circular-dichroic measurements typically require further intrinsic or extrinsic breaking of symmetry by, e.g., enantiomeric excess, orientation, magnetic fields, or direction-sensitive detectors. Here we introduce circular-dichroic attosecond transient absorption spectroscopy by leveraging the angular momentum of two circularly polarized pulses, both pump and probe, in an isotropic medium, optically orienting the angular momentum of excited states on an attosecond timescale. We investigate a circular-dichroic measurement of the attosecond transient absorption of He Rydberg states. By limiting the allowed pathways via dipole selection rules for co- and counterrotating circularly polarized near-infrared and extreme ultraviolet (XUV) pulses, different spectral reshapings of the XUV transient absorption due to the AC Stark effect are observed. Paired with time-dependent Schrödinger equation calculations, the results show the role of selection and propensity rules and open up new opportunities to study coupling pathways of excited states as well as spin-dependent dynamics in atoms and beyond via attosecond optical orientation.}, archive = {J_PRL}, author = {Lauren B. Drescher and Nicola Mayer and Kylie Gannan and Jonah R. Adelman and Stephen R. Leone}, doi = {10.1103/kfjh-zc96}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163201}, shortjournal = {Phys. Rev. Lett.}, title = {Attosecond optical orientation}, volume = {135}, year = {2025}, }
• (2025). Pb208 nuclear charge radius revisited: Closing the fine-structure-anomaly gap. PRL, 135(16), 163002. (www)

  @article{ , abstract = {A comprehensive reevaluation of the root-mean-square nuclear charge radius is presented for the doubly magic Pb 208 extracted from muonic spectroscopy measurements. By integrating rigorous theoretical quantum electrodynamics calculations, state-of-the-art numerical methods, and a systematic reanalysis of the uncertainties, we reduced the long-standing muonic fine-structure anomaly and improved the goodness of fit by a factor of 20. The resulting value of 5.5062(5) fm for a Fermi distribution is fairly consistent with the previously reported muonic spectroscopy value, and 3 standard deviations larger than the commonly used compilation data, which indicates that the current value and its uncertainty could be significantly underestimated. Attributing the remaining discrepancy to theory errors which cannot be rigorously calculated, we suggest the rms charge radius with reduced model dependence to be 5.5062(17) fm. This Letter sets an improved benchmark for charge radius extraction in heavy nuclei and paves a path for systematic reevaluations across the nuclear chart.}, archive = {J_PRL}, author = {Zewen Sun and Konstantin A. Beyer and Zoia A. Mandrykina and Igor A. Valuev and Christoph H. Keitel and Natalia S. Oreshkina}, doi = {10.1103/h3xz-xdxr}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163002}, shortjournal = {Phys. Rev. Lett.}, title = {Pb208 nuclear charge radius revisited: Closing the fine-structure-anomaly gap}, volume = {135}, year = {2025}, }
• (2025). Spontaneous emission from electronic metastable resonance states. PRL, 135(16), 163001. (www)

  @article{ , abstract = {We demonstrate that calculating the spontaneous emission decay rate from metastable resonance states (states with finite lifetimes embedded in the continuum) requires considering transitions to all continuum states, not just to lower states. This holds even when the lifetimes of the metastable states are very long and might be effectively considered as bound states in the continuum. However, employing complex-scaling transformations, this computationally prohibitive task becomes feasible by utilizing methods originally designed for excited bound states for calculation of complex poles of the scattering matrix. As an illustrative example, these methods are applied to calculate the spontaneous emission decay rates of metastable resonance states in a double-barrier potential. The rapid numerical convergence of this approach highlights a new avenue for studying spontaneous emission from metastable states in real-life systems, particularly in many-electron systems, where calculation of the spontaneous emission decay rate from metastable resonances (e.g., autoionization states) is computationally difficult, if not impossible, using the standard (Hermitian) formalism of quantum mechanics.}, archive = {J_PRL}, author = {Amir Sivan and Milan Šindelka and Meir Orenstein and Nimrod Moiseyev}, doi = {10.1103/jm4m-rpyc}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {163001}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous emission from electronic metastable resonance states}, volume = {135}, year = {2025}, }
• (2025). Crust composition and the shallow heat source in KS 1731–260. PRL, 135(16), 162701. (www)

  @article{ , abstract = {The presence of a strong shallow heat source of unknown origin in accreting neutron star crusts has been inferred by analyzing x-ray observations of their cooling in quiescence. We model the cooling of KS 1731–260 using realistic crust compositions and nuclear heating and cooling sources from detailed nuclear reaction network calculations. We find that the required strength of the shallow heat source in KS 1731–260 is reduced by more than a factor of 3 compared to previous analysis, a 5 σ difference that alleviates the need for exotic solutions. Our analysis also suggests the existence of an impure nuclear pasta layer in the inner crust of KS 1731–260, though future observations will provide more stringent constraints. In addition, we obtain constraints on the dominant surface burning modes of KS 1731–260 over its history.}, archive = {J_PRL}, author = {R. Jain and E. F. Brown and H. Schatz and A. V. Afanasjev and M. Beard and L. R. Gasques and J. Grace and A. Heger and G. W. Hitt and W. R. Hix and R. Lau and W.-J. Ong and M. Wiescher and Y. Xu}, doi = {10.1103/jwc8-xfhv}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {162701}, shortjournal = {Phys. Rev. Lett.}, title = {Crust composition and the shallow heat source in KS 1731–260}, volume = {135}, year = {2025}, }
• (2025). Extracting the speed of sound in heavy-ion collisions: A study of quantum-initiated fluctuations and thermalization. PRL, 135(16), 162301. (www)

  @article{ , abstract = {The thermalization of quark-gluon plasma created in heavy-ion collisions is crucial for understanding its behavior as a relativistic fluid and the thermodynamic properties of the quantum chromodynamics (QCD). This study investigates the role of fluctuations in the relationship between transverse momentum and particle multiplicity, with a particular focus on their impact on extracting the QCD speed of sound. In a thermalized quark-gluon plasma, these fluctuations mostly originate from quantum fluctuations in the colliding nuclei, and exhibit a Gaussian distribution as a consequence of their independence from thermodynamic response. In contrast, nonthermalized systems display non-Gaussian fluctuations, reflecting the breakdown of thermalization. By leveraging the Gaussianity condition of quantum-initiated fluctuations, the physical value of the speed of sound can be extracted statistically, even in the presence of significant event-by-event fluctuations. This framework provides a robust diagnostic tool for probing thermalization and extracting thermodynamic properties in both large and small collision systems.}, archive = {J_PRL}, author = {Yu-Shan Mu and Jing-An Sun and Li Yan and Xu-Guang Huang}, doi = {10.1103/skhj-cj9p}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {162301}, shortjournal = {Phys. Rev. Lett.}, title = {Extracting the speed of sound in heavy-ion collisions: A study of quantum-initiated fluctuations and thermalization}, volume = {135}, year = {2025}, }
• (2025). η and η′ production in j/ψ radiative decays from quantum chromodynamics. PRL, 135(16), 161904. (www)

  @article{ , abstract = {We present a first principles calculation within quantum chromodynamics (QCD) of the radiative decays of the into the light pseudoscalar mesons and . Within a lattice computation we obtain the transition form factors as a function of photon virtuality from the timelike region, accessible experimentally via the “Dalitz” decay , through to the real photon point corresponding to . This is the first calculation in lattice QCD with two (heavier than physical) degenerate flavors of light quark and a heavier strange quark, in which the appears as the first excited state with pseudoscalar isoscalar quantum numbers. We access it reliably by using variationally optimized operators , the use of which also improves the purity of the and signals, reducing systematic uncertainties. High quality results at a large number of kinematic points are obtained in a typically noisy disconnected process by using a novel correlator averaging procedure. Our results show the expected enhanced production of the over the in this process, and suggest that the demonstrated lattice technology is suitable for future calculations considering processes in which light meson resonances are produced.}, archive = {J_PRL}, author = {for the Hadron Spectrum Collaboration and Mischa Batelaan and Jozef J. Dudek and Robert G. Edwards}, doi = {10.1103/tdk2-bk8w}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161904}, shortjournal = {Phys. Rev. Lett.}, title = {η and η′ production in j/ψ radiative decays from quantum chromodynamics}, volume = {135}, year = {2025}, }
• (2025). Open B-hadron production at hadron colliders in QCD at next-to-next-to-leading-order and next-to-next-to-leading-logarithmic accuracy. PRL, 135(16), 161903. (www)

  @article{ , abstract = {We report on a calculation of open heavy-flavor production at hadron colliders which extends to next-to-next-to-leading order (NNLO) accuracy the classic NLO-accurate formalism developed almost 30 years ago under the acronym FONLL. The approach retains the exact heavy-flavor mass dependence at low transverse momentum, p T , and resums collinear logarithms through next-to-next-to-leading log (NNLL) at high p T . Provided are predictions for B hadrons as well as B -decay products like J / Ψ and muons. The main features of the NNLO + NNLL results are reduced scale dependence and moderate NNLO correction, consistent with perturbative convergence in a wide range of kinematic scales from few GeV up to asymptotically large values of p T . The new calculation significantly improves the agreement with data for B hadrons and muons. We uncover an intriguing discrepancy in J / Ψ final states which may point to a lower value of the B → J / Ψ decay rate.}, archive = {J_PRL}, author = {Michał Czakon and Terry Generet and Alexander Mitov and Rene Poncelet}, doi = {10.1103/b6pf-rj4h}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161903}, shortjournal = {Phys. Rev. Lett.}, title = {Open B-hadron production at hadron colliders in QCD at next-to-next-to-leading-order and next-to-next-to-leading-logarithmic accuracy}, volume = {135}, year = {2025}, }
• (2025). Study of ϕ→KK¯ and KS0−KL0 asymmetry in the amplitude analysis of Ds+→KS0KL0π+ decays. PRL, 135(16), 161902. (www)

  @article{ , abstract = {Using e + e − annihilation data corresponding to a total integrated luminosity of 7.33 fb − 1 collected at center-of-mass energies between 4.128 and 4.226 GeV with the BESIII detector, we provide the first amplitude analysis and absolute branching fraction measurement of the hadronic decay D s + → K S 0 K L 0 π + . The branching fraction of D s + → K S 0 K L 0 π + is determined to be ( 1.86 ± 0.0 6 stat ± 0.0 3 syst ) % . Combining the B [ D s + → ϕ ( → K S 0 K L 0 ) π + ] obtained in this Letter and the world average of B [ D s + → ϕ ( → K + K − ) π + ] , we measure the relative branching fraction B ( ϕ → K S 0 K L 0 ) / B ( ϕ → K + K − ) = ( 0.593 ± 0.02 3 stat ± 0.01 4 syst ± 0.01 6 ϕ π ) , where the third error is due to the uncertainty of the B ( D s + → ϕ π + , ϕ → K + K − ) . Our result deviates from the Particle Data Group value by more than 3 σ . Furthermore, the asymmetry of the branching fractions of D s + → K S 0 K * ( 892 ) + and D s + → K L 0 K * ( 892 ) + , ( { B [ D s + → K S 0 K * ( 892 ) + ] − B [ D s + → K L 0 K * ( 892 ) + ] } / { B [ D s + → K S 0 K * ( 892 ) + ] + B [ D s + → K L 0 K * ( 892 ) + ] } ) , is determined to be ( − 14.5 ± 5.1 stat ± 1.8 syst ) % .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Y. Y. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/6py9-h8qv}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161902}, shortjournal = {Phys. Rev. Lett.}, title = {Study of ϕ→KK¯ and KS0−KL0 asymmetry in the amplitude analysis of Ds+→KS0KL0π+ decays}, volume = {135}, year = {2025}, }
• (2025). Observation of a new charmed baryon decaying to Ξc+π−π+. PRL, 135(16), 161901. (www)

  @article{ , abstract = {The Ξ c + π − π + spectrum is investigated using proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4 fb − 1 , collected by the LHCb experiment during 2016–2018. Four states are observed with high significance, and their masses and widths are measured to be m [ Ξ c ( 2815 ) + ] = 2816.65 ± 0.03 ± 0.03 ± 0.23 MeV , Γ [ Ξ c ( 2815 ) + ] = 2.07 ± 0.08 ± 0.12 MeV , m [ Ξ c ( 2923 ) + ] = 2922.8 ± 0.3 ± 0.5 ± 0.2 MeV , Γ [ Ξ c ( 2923 ) + ] = 5.3 ± 0.9 ± 1.4 MeV , m [ Ξ c ( 2970 ) + ] = 2968.6 ± 0.5 ± 0.5 ± 0.2 MeV , Γ [ Ξ c ( 2970 ) + ] = 31.7 ± 1.7 ± 1.9 MeV , [ Ξ c ( 3080 ) + ] = 3076.8 ± 0.7 ± 1.3 ± 0.2 MeV , Γ [ Ξ c ( 3080 ) + ] = 6.8 ± 2.3 ± 0.9 MeV , where the uncertainties are statistical, systematic, and due to the limited precision on the Ξ c + mass, respectively. The Ξ c ( 2923 ) + baryon is observed for the first time, and is consistent with being the isospin partner of the previously observed Ξ c ( 2923 ) 0 state. Most of the measured parameters are more precise than existing world averages.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and J. Bartz and J. M. Basels and S. Bashir and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and O. Bezshyyko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and E. Bottalico and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and J. D. Brandenburg and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and L. Buonincontri and M. Burgos Marcos and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and S. Cesare and A. J. Chadwick and I. Chahrour and H. Chang and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and C. Coronel and I. Corredoira and A. Correia and G. Corti and J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and S. Faghih and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and A. Gavrikov and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and C. Giugliano and M. A. Giza and F. C. Glaser and V. V. Gligorov and C. Göbel and L. Golinka-Bezshyyko and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and E. Govorkova and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and A. Korchin and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and V. Kushnir and B. K. Kutsenko and I. Kyryllin and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and J. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and D. Liu and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and G. Loachamin Ordonez and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and L. Moeser and R. A. Mohammed and R. D. Moise and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and V. Mytrochenko and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and E. Nekrasova and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and R. N. Pilato and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and M. Ribalda Galvez and R. Ribatti and G. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and M. Singha and N. Skidmore and T. Skwarnicki and M. W. Slater and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and M. Stefaniak and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and T. Tork and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and A. Upadhyay and B. Urbach and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and J. van Eldik and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and B. Vivacqua and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and A. Wang and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and T. X. Xing and A. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Z. Zhang and Y. Zhao and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and Y. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/gghl-m6fm}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of a new charmed baryon decaying to Ξc+π−π+}, volume = {135}, year = {2025}, }
• (2025). Measurement of the Z-boson mass. PRL, 135(16), 161802. (www)

  @article{ , abstract = {The first dedicated -boson mass measurement at the LHC with decays is reported. The dataset uses proton-proton collisions at a center-of-mass energy of 13 TeV, recorded in 2016 by the LHCb experiment, and corresponds to an integrated luminosity of . A template fit to the mass distribution yields the following result for the -boson mass: , where the first uncertainty is statistical and the second systematic. This result is consistent with previous measurements and predictions from global electroweak fits.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and P. Andreola and M. Andreotti and A. Anelli and D. Ao and F. Archilli and Z Areg and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and J. Bartz and S. Bashir and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and O. Bezshyyko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and E. Bottalico and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and J. D. Brandenburg and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and L. Buonincontri and M. Burgos Marcos and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and S. Cesare and A. J. Chadwick and I. Chahrour and H. Chang and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and C. Coronel and I. Corredoira and A. Correia and G. Corti and J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and Y. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and S. Faghih and L. N. Falcao and B. Fang and R. Fantechi and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and A. Fomin and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and A. Gavrikov and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and M. A. Giza and F. C. Glaser and V. V. Gligorov and C. Göbel and L. Golinka-Bezshyyko and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and E. Govorkova and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and G. Hallett and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Iniukhin and A. Ishteev and K. Ivshin and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and A. Korchin and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and E. Kowalczyk and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and V. Kushnir and B. Kutsenko and I. Kyryllin and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and J. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and R. Litvinov and D. Liu and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and G. Loachamin Ordonez and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and D. Magdalinski and D. Maisuzenko and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and L. Moeser and R. A. Mohammed and R. D. Moise and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and V. Mytrochenko and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and E. Nekrasova and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and T. Pajero and A. Palano and M. Palutan and X. Pan and S. Panebianco and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and R. N. Pilato and D. Pinci and F. Pisani and M. Pizzichemi and V. M. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and M. Ribalda Galvez and R. Ribatti and G. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and B. Sevilla Sanjuan and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and M. Singha and N. Skidmore and T. Skwarnicki and M. W. Slater and E. Smith and K. Smith and M. Smith and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and M. Stefaniak and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and Y. T. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and U. Thoma and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and T. Tork and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and A. Upadhyay and B. Urbach and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and J. van Eldik and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and B. Vivacqua and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and A. Wang and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and T. X. Xing and A. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and R. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Z. Zhang and Y. Zhao and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and Y. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/ydn7-qx1d}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161802}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of the Z-boson mass}, volume = {135}, year = {2025}, }
• (2025). New chiral structures for baryon number violating nucleon decays. PRL, 135(16), 161801. (www)

  @article{ , abstract = {We examine the most general nucleon decay interactions that involve three light quarks without being acted upon by a derivative. We identify four generic operator structures that correspond to the irreducible representations in the chiral group SU ( 3 ) L ⊗ SU ( 3 ) R of QCD, { 8 L ⊗ 1 R , 3 ¯ L ⊗ 3 R , 6 L ⊗ 3 R , 10 L ⊗ 1 R } , plus their chirality partners under the interchange of chiralities L ↔ R . While half of them have been extensively discussed in the literature, the other half, 6 L ( R ) ⊗ 3 R ( L ) and 10 ¯ L ( R ) ⊗ 1 R ( L ) , are identified for the first time. We perform chiral matching for these interactions at the leading chiral order and find that each has a unique chiral realization in terms of the octet baryons and pseudoscalars. Notably, the chiral interaction in the 6 L ( R ) ⊗ 3 R ( L ) representation appears at the same chiral order as those of the known ones, while the one in the 10 L ( R ) ⊗ 1 R ( L ) representation appears at a higher chiral order. These new structures are prevalent in effective field theories and ultraviolet models, and they offer novel experimental avenues to search for baryon number violating nucleon decays.}, archive = {J_PRL}, author = {Yi Liao and Xiao-Dong Ma and Hao-Lin Wang}, doi = {10.1103/d8m7-5xxx}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161801}, shortjournal = {Phys. Rev. Lett.}, title = {New chiral structures for baryon number violating nucleon decays}, volume = {135}, year = {2025}, }
• (2025). Semiclassical wormholes toward typical entangled states. PRL, 135(16), 161601. (www)

  @article{ , abstract = {What do the typical entangled states of two black holes look like? Do they contain semiclassical interiors? We approach these questions constructively, providing ensembles of states that densely explore the black hole Hilbert space. The states contain very long Einstein-Rosen caterpillars : semiclassical wormholes with large numbers of matter inhomogeneities. Distinguishing these ensembles from the typical entangled states of the black holes is hard. We quantify this by deriving the correspondence between a microscopic notion of quantum randomness and the geometric length of the wormhole. This formalizes a “complexity = geometry” relation.}, archive = {J_PRL}, author = {Javier M. Magán and Martin Sasieta and Brian Swingle}, doi = {10.1103/btw6-44ry}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161601}, shortjournal = {Phys. Rev. Lett.}, title = {Semiclassical wormholes toward typical entangled states}, volume = {135}, year = {2025}, }
• (2025). Hawking evaporation and the fate of black holes in loop quantum gravity. PRL, 135(16), 161501. (www)

  @article{ , abstract = {A recent covariant formulation, that includes nonperturbative effects from loop quantum gravity (LQG) as self-consistent effective models, has revealed the possibility of nonsingular black hole solutions. The new framework makes it possible to couple scalar matter to such LQG black holes and derive Hawking radiation in the presence of quantum spacetime effects while respecting general covariance. Standard methods to derive particle production both within the geometric optics approximation and the Parikh–Wilczek tunnelling approach are therefore available and confirm the thermal nature of Hawking radiation. The covariant description of scale-dependent decreasing holonomy corrections maintains Hawking temperature as well as universality of the low-energy transmission coefficients, stating that the absorption rates are proportional to the horizon area at leading order. Quantum-geometry effects enter the thermal distribution only through subleading corrections in the graybody factors. Nevertheless, they do impact energy emission of the black hole and its final state in a crucial way regarding one of the main questions of black-hole evaporation: whether a black-to-white-hole transition, or a stable remnant, is preferred. For the first time, a first-principles derivation, based on a discussion of backreaction, finds evidence that points to the former outcome.}, archive = {J_PRL}, author = {Idrus Husin Belfaqih and Martin Bojowald and Suddhasattwa Brahma and Erick I. Duque}, doi = {10.1103/t6q4-4l77}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161501}, shortjournal = {Phys. Rev. Lett.}, title = {Hawking evaporation and the fate of black holes in loop quantum gravity}, volume = {135}, year = {2025}, }
• (2025). Fermi-LAT galactic center excess morphology of dark matter in simulations of the milky way galaxy. PRL, 135(16), 161005. (www)

  @article{ , abstract = {The strongest experimental evidence for dark matter is the Galactic Center gamma-ray excess observed by the Fermi telescope and even predicted prior to discovery as a potential dark matter signature via weakly interacting massive particle dark matter self-annihilations. However, an equally compelling explanation of the excess gamma-ray flux refers to a population of old millisecond pulsars that also accounts for the observed boxy morphology inferred from the bulge old star population. We employ a set of Milky Way-like galaxies found in the hestia constrained simulations of the local universe to explore the rich morphology of the central dark matter distribution, motivated by the GAIA discovery of a vigorous early merging history of the Milky Way galaxy. We predict a significantly nonspherical gamma-ray morphology from the weakly interacting massive particle interpretation. Future experiments, such as the Cherenkov Telescope Array, that extend to higher energies, should distinguish between the competing interpretations.}, archive = {J_PRL}, author = {Moorits Mihkel Muru and Joseph Silk and Noam I. Libeskind and Stefan Gottlöber and Yehuda Hoffman}, doi = {10.1103/g9qz-h8wd}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161005}, shortjournal = {Phys. Rev. Lett.}, title = {Fermi-LAT galactic center excess morphology of dark matter in simulations of the milky way galaxy}, volume = {135}, year = {2025}, }
• (2025). Resolving the negative effective neutrino mass parameter with cosmic birefringence. PRL, 135(16), 161004. (www)

  @article{ , abstract = {The recent measurement of baryonic acoustic oscillations by the Dark Energy Spectroscopic Instrument reveals a mild tension with observations of the cosmic microwave background (CMB) within the standard Λ cold dark matter ( Λ CDM ) cosmological model. This discrepancy leads to a preference for a total neutrino mass that is lower than the minimum value inferred from neutrino oscillation experiments. Alternatively, this tension can be eased within Λ CDM by assuming a higher optical depth ( τ ≃ 0.09 ), but such a value conflicts with large-scale CMB polarization data. We point out that cosmic birefringence, as suggested by recent Planck reanalyses, resolves this discrepancy if the birefringence angle varies significantly during reionization. Specifically, we consider the fact that the measured cosmic birefringence angle β 0 = 0.34 ± 0.09 ( 1 σ ) deg has the phase ambiguity, i.e., the measured rotation angle is described by β = β 0 + 180 n deg ( n ∈ Z ). We show that cosmic birefringence induced by axionlike particles with nonzero n suppresses the reionization bump, allowing a higher τ consistent with data. We provide a viable parameter space where the birefringence effect simultaneously accounts for the low- ℓ polarization spectra, the Planck E B correlations, and the elevated value of τ , suggesting a key role for cosmic birefringence in current cosmological tensions.}, archive = {J_PRL}, author = {Toshiya Namikawa}, doi = {10.1103/qgnn-6hsf}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161004}, shortjournal = {Phys. Rev. Lett.}, title = {Resolving the negative effective neutrino mass parameter with cosmic birefringence}, volume = {135}, year = {2025}, }
• (2025). Fermion-boson stars as attractors in fuzzy dark matter and ideal gas dynamics. PRL, 135(16), 161003. (www)

  @article{ , abstract = {In the context of fuzzy dark matter (FDM) we study the core formation in the presence of an ideal gas (IG). Our analysis is based on the solution of the Schrödinger-Poisson-Euler system of equations that drives the evolution of FDM together with a compressible IG, both coupled through the gravitational potential they produce. Starting from random initial conditions for both FDM and IG, we study the evolution of the system until it forms a nearly relaxed, virialized, and close to hydrostatic equilibrium core, surrounded by an envelope of the two components. We find that the core corresponds to Newtonian fermion-boson stars (FBS). If the IG is used to model luminous matter, our results indicate that FBS behave as attractor core solutions of structure formation of FDM along with visible matter.}, archive = {J_PRL}, author = {Iván Alvarez-Rios and Francisco S. Guzmán and Jens Niemeyer}, doi = {10.1103/4tkh-7hjs}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161003}, shortjournal = {Phys. Rev. Lett.}, title = {Fermion-boson stars as attractors in fuzzy dark matter and ideal gas dynamics}, volume = {135}, year = {2025}, }
• (2025). First limits on light dark matter interactions in a low threshold two-channel athermal phonon detector from the TESSERACT collaboration. PRL, 135(16), 161002. (www)

  @article{ , abstract = {We present results of a search for spin-independent dark matter-nucleus interactions in a 1 cm 2 by 1 mm thick (0.233 g) high-resolution silicon athermal phonon detector operated above ground. For interactions in the substrate, this detector achieves an rms baseline energy resolution of 361.5 ( 4 ) m eV (statistical error), the best for any athermal phonon detector to date. With an exposure of 0.233 g × 12 hours, we place the most stringent constraints on dark matter masses between 44 and 87 M eV / c 2 , with the lowest unexplored cross section of 4 × 10 − 32 c m 2 at 87 M eV / c 2 . We employ a conservative salting technique to reach the lowest dark matter mass ever probed via direct detection experiment. This constraint is enabled by two-channel rejection of low energy backgrounds that are coupled to individual sensors.}, archive = {J_PRL}, author = {TESSERACT Collaboration and T. K. Bui and C. L. Chang and Y.-Y. Chang and L. Chaplinsky and C. W. Fink and M. Garcia-Sciveres and W. Guo and S. A. Hertel and L. Juigne and A. R. L. Kavner and X. Li and J. Lin and M. Lisovenko and R. Mahapatra and W. Matava and D. N. McKinsey and V. Novati and P. K. Patel and B. Penning and H. D. Pinckney and M. Platt and M. Pyle and Y. Qi and M. Reed and G. R. C. Rischbieter and R. K. Romani and B. Sadoulet and B. Serfass and P. Sorensen and B. Suerfu and A. Suzuki and V. Velan and G. Wang and Y. Wang and S. L. Watkins and M. R. Williams and J. K. Wuko and T. Aramaki and P. Cushman and N. N. Gite and A. Gupta and M. E. Huber and N. A. Kurinsky and B. von Krosigk and J. S. Mammo and A. J. Mayer and J. Nelson and S. M. Oser and L. Pandey and A. Pradeep and W. Rau and T. Saab}, doi = {10.1103/hsrl-crvf}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161002}, shortjournal = {Phys. Rev. Lett.}, title = {First limits on light dark matter interactions in a low threshold two-channel athermal phonon detector from the TESSERACT collaboration}, volume = {135}, year = {2025}, }
• (2025). Atacama cosmology telescope, south pole telescope, and chaotic inflation. PRL, 135(16), 161001. (www)

  @article{ , abstract = {We show that the simplest generalization of the chaotic inflation model 1 2 m 2 ϕ 2 with nonminimal coupling to gravity ( 1 + ϕ ) R provides a good match to the results of the latest data release of the Atacama Cosmology Telescope and South Pole Telescope, with r ≈ 10 − 2 .}, archive = {J_PRL}, author = {Renata Kallosh and Andrei Linde and Diederik Roest}, doi = {10.1103/d6gn-78hn}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {161001}, shortjournal = {Phys. Rev. Lett.}, title = {Atacama cosmology telescope, south pole telescope, and chaotic inflation}, volume = {135}, year = {2025}, }
• (2025). Suppressing spurious transitions using spectrally balanced pulse. PRL, 135(16), 160804. (www)

  @article{ , abstract = {Achieving precise control over quantum systems presents a significant challenge, especially in many-body setups, where residual couplings and unintended transitions undermine the accuracy of quantum operations. In superconducting qubits, parasitic interactions—both between distant qubits and with spurious two-level systems—can severely limit the performance of quantum gates. In this Letter, we introduce a pulse-shaping technique that uses spectrally balanced microwave pulses to suppress undesired transitions. Experimental results demonstrate an order-of-magnitude reduction in spurious excitations between weakly detuned qubits as well as a substantial decrease in single-qubit gate errors caused by a strongly coupled two-level defect over a broad frequency range. Our method provides a simple yet powerful solution for mitigating adverse effects from parasitic couplings, enhancing quantum gate fidelity. The pulse-shaping technique can be readily adapted to various physical systems.}, archive = {J_PRL}, author = {Ruixia Wang and Yaqing Feng and Yujia Zhang and Jiayu Ding and Boxi Li and Felix Motzoi and Yang Gao and Huikai Xu and Zhen Yang and Wuerkaixi Nuerbolati and Haifeng Yu and Weijie Sun and Fei Yan}, doi = {10.1103/h4xf-vq2l}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160804}, shortjournal = {Phys. Rev. Lett.}, title = {Suppressing spurious transitions using spectrally balanced pulse}, volume = {135}, year = {2025}, }
• (2025). Closing the detection loophole in the triangle network with high-dimensional photonic states. PRL, 135(16), 160803. (www)

  @article{ , abstract = {Bell nonlocality without input settings, .g., in the triangle network, has been perceived to be particularly fragile, with low robustness to noise in physical implementations. Here, we show to the contrary that nonlocality based on N00N states already for N = 2 has an exceptionally high robustness to photon loss. For the dominant noise factor, single photon loss in the transmission channels, we can certify noise robustness up to 10% loss, while for a realistic noise model we use neural network-based heuristics to observe ∼ 50 % robustness. Moreover we show that the robustness holds even for imperfect sources based on spontaneous parametric down-conversion sources, where the heralding information of the sources can be used to avoid any global postprocessing of the outcomes, such as discarding rounds when photons fail to arrive, and thus demonstrate how the detection loophole in the triangle network can be closed.}, archive = {J_PRL}, author = {Tamás Kriváchy and Martin Kerschbaumer}, doi = {10.1103/nwzw-tqzp}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160803}, shortjournal = {Phys. Rev. Lett.}, title = {Closing the detection loophole in the triangle network with high-dimensional photonic states}, volume = {135}, year = {2025}, }
• (2025). Bell nonlocality in quantum networks with unreliable sources: Loophole-free postelection via self-testing. PRL, 135(16), 160802. (www)

  @article{ , abstract = {We discuss Bell nonlocality in quantum networks with unreliable sources. Our main result is a condition on the observed data that ensures that inconclusive events can be safely discarded, without introducing any loophole. More formally, we characterize the fair-sampling property for measurements in a network. When all measurements are fair-sampling, we show that the postselection of conclusive outcomes does not compromise the assumption of source independence, hence avoiding the detection loophole. Furthermore, we show that in some cases, the fair-sampling property can in fact be certified directly from observed data. To show this, we prove that saturation of the Finner inequality provides a self-test of the underlying quantum model. We illustrate the relevance of our results by demonstrating an improvement in device-independent randomness generation for a photonic Bell test with a probabilistic source and for the triangle network.}, archive = {J_PRL}, author = {Sadra Boreiri and Nicolas Brunner and Pavel Sekatski}, doi = {10.1103/bqwm-ll5y}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160802}, shortjournal = {Phys. Rev. Lett.}, title = {Bell nonlocality in quantum networks with unreliable sources: Loophole-free postelection via self-testing}, volume = {135}, year = {2025}, }
• (2025). On-chip verified quantum computation with an ion-trap quantum processing unit. PRL, 135(16), 160801. (www)

  @article{ , abstract = {We present a novel approach to cryptographically secure verification and benchmarking of quantum computing, demonstrating our approach on an ion-trap quantum computer. Unlike previous cryptographically secure verification protocols, which typically require quantum communication between client and server, our approach is implemented entirely on chip. This eliminates the need for a quantum capable client, and significantly enhances practicality. We perform tomography to justify the additionally required assumption that the noise is independent of the secret used to prepare the server’s single-qubit states. We quantify the soundness error that may be caused by residual secret dependencies. We demonstrate our protocol on the 20-qubit Quantinuum H1-1 ion-trap quantum processing unit, using qubit measurements and resets to construct measurement patterns with up to 52 vertices. To our knowledge, these are the largest verified measurement-based quantum computations performed to date.}, archive = {J_PRL}, author = {Cica Gustiani and Dominik Leichtle and Jonathan Miller and Ross Grassie and Daniel Mills and Elham Kashefi}, doi = {10.1103/jpms-v3kw}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160801}, shortjournal = {Phys. Rev. Lett.}, title = {On-chip verified quantum computation with an ion-trap quantum processing unit}, volume = {135}, year = {2025}, }
• (2025). Roughening transition in quantum circuits. PRL, 135(16), 160603. (www)

  @article{ , abstract = {We explore a roughening phase transition that occurs in the entanglement dynamics of certain quantum circuits. Viewing entanglement as the free energy of a membrane in a circuit-defined random environment, there is a competition between membrane smoothing due to lattice pinning and roughening due to disorder in the circuit. In particular, we investigate the randomness-induced roughening transition of the entanglement membrane in a ( )-dimensional Clifford circuit model by calculating the entanglement entropy for various bipartitions. We further construct a scaling theory for membranes tilted away from lattice planes, uncovering new scaling forms and a crossover to a previously unexplored critical “tilted regime.”}, archive = {J_PRL}, author = {Hyunsoo Ha and David A. Huse and Grace M. Sommers}, doi = {10.1103/gkwd-8477}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160603}, shortjournal = {Phys. Rev. Lett.}, title = {Roughening transition in quantum circuits}, volume = {135}, year = {2025}, }
• (2025). Lindbladian simulation with logarithmic precision scaling via two ancillas. PRL, 135(16), 160602. (www)

  @article{ , abstract = {Quantum computers promise efficient simulation of Lindbladian dynamics in open quantum systems, with broad applications in quantum chemistry, quantum error correction, and quantum state preparation. However, simulating open systems is more challenging than simulating closed systems, inherently requiring nonunitary operations. Existing approaches face unique challenges: methods with higher theoretical efficiency demand numerous ancillae and multiqubit operations that are experimentally challenging, while more experimentally feasible methods incur deep quantum circuits to control simulation errors. Here, we introduce a powerful framework, the linear combinations of superoperators, to systematically compensate for simulation errors and overcome these challenges. Utilizing simple gates and experimentally accessible Trotter decompositions, our approach achieves an exponential reduction in circuit depth with respect to the simulation precision, if only two ancillas are allowed to be used. We further extend the approach to time-dependent Lindbladians, achieving for the first time logarithmic depth in precision. Numerical simulations demonstrate significant performance advantages, establishing our method as a practical and scalable solution for simulating open quantum systems on near-term quantum hardware.}, archive = {J_PRL}, author = {Wenjun Yu and Xiaogang Li and Qi Zhao and Xiao Yuan}, doi = {10.1103/2cx4-b82c}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160602}, shortjournal = {Phys. Rev. Lett.}, title = {Lindbladian simulation with logarithmic precision scaling via two ancillas}, volume = {135}, year = {2025}, }
• (2025). Measuring full counting statistics in a trapped-ion quantum simulator. PRL, 135(16), 160601. (www)

  @article{ , abstract = {In quantum mechanics, the probability distribution function and full counting statistics play a fundamental role in characterizing the fluctuations of quantum observables, as they encode the complete information about these fluctuations. In this Letter, we measure these two quantities in a trapped-ion quantum simulator for the transverse and longitudinal magnetization within a subsystem. We utilize the toolbox of classical shadows to postprocess the measurements performed in random bases. The measurement scheme efficiently allows access to the full counting statistics and probability distribution function of all possible operators on desired choices of subsystems of an extended quantum system.}, archive = {J_PRL}, author = {Lata Kh Joshi and Filiberto Ares and Manoj K. Joshi and Christian F. Roos and Pasquale Calabrese}, doi = {10.1103/gyvf-s5bd}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160601}, shortjournal = {Phys. Rev. Lett.}, title = {Measuring full counting statistics in a trapped-ion quantum simulator}, volume = {135}, year = {2025}, }
• (2025). Thermodynamics and state preparation in a two-state system of light. PRL, 135(16), 160406. (www)

  @article{ , abstract = {The coupling of two-level quantum systems to the thermal environment is a fundamental problem with applications of such usually single-particle or fermionic systems ranging from qubit state preparation to spin models. The present Letter studies the elementary problem of the thermodynamics of an ensemble of bosons populating a two-level system. Using an optical dye microcavity platform, we thermalize photons in a two-mode system at conditions of tunable chemical potential, demonstrating the statistical mechanical problem of bosons populating a two-level system, coupled to a heat bath. Under pulsed excitation, we observe Josephson oscillations between the two quantum states, which verifies the possibility for coherent manipulation. In contrast, under stationary conditions, the thermalization of the two-mode system is observed, arising from radiative coupling of photons to the dye. As the energetic splitting between eigenstates is 2 orders of magnitude smaller than thermal energy, at low occupations, an almost equal distribution of the occupation of the modes is observed, as expected from Boltzmann statistics. For larger occupation, we observe efficient population of the ground state and saturation of the upper level at high filling, expected from quantum statistics. Our experiment holds promise for state preparation in quantum technologies as well as for quantum thermodynamics studies.}, archive = {J_PRL}, author = {Christian Kurtscheid and Andreas Redmann and Frank Vewinger and Julian Schmitt and Martin Weitz}, doi = {10.1103/kynj-l87s}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160406}, shortjournal = {Phys. Rev. Lett.}, title = {Thermodynamics and state preparation in a two-state system of light}, volume = {135}, year = {2025}, }
• (2025). Macroscopic suppression of supersonic quantum transport. PRL, 135(16), 160405. (www)

  @article{ , abstract = {We consider a broad class of strongly interacting quantum lattice gases, including the Fermi-Hubbard and Bose-Hubbard models. We focus on macroscopic particle clusters of size , with and the total particle number, and we study the quantum probability that such a cluster is transported across a distance within time . Conventional effective light cone arguments yield a bound of the form . We report a substantially stronger bound , which provides exponential suppression that scales with system size. Our result establishes a universal dynamical large deviation principle: macroscopic suppression of supersonic macroscopic transport (MASSMAT).}, archive = {J_PRL}, author = {Jérémy Faupin and Marius Lemm and Israel Michael Sigal and Jingxuan Zhang (张景宣}, doi = {10.1103/27qs-vlrn}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160405}, shortjournal = {Phys. Rev. Lett.}, title = {Macroscopic suppression of supersonic quantum transport}, volume = {135}, year = {2025}, }
• (2025). Long-range nonstabilizerness and phases of matter. PRL, 135(16), 160404. (www)

  @article{ , abstract = {Long-range nonstabilizerness can be defined as the amount of nonstabilizerness that cannot be removed by shallow local quantum circuits. We study long-range nonstabilizerness in the context of many-body quantum physics, a task with possible implications for quantum-state preparation protocols and implementation of quantum-error correcting codes. After presenting a simple argument showing that long-range nonstabilizerness is a generic property of many-body states, we restrict to the class of ground states of gapped local Hamiltonians. We focus on one-dimensional (1D) systems and present rigorous results in the context of translation-invariant matrix product states (MPSs), with our analysis extending to all gapped 1D phases under widely accepted physical assumptions. By analyzing the fixed points of the MPS renormalization-group flow, we provide a sufficient condition for long-range nonstabilizerness, which depends entirely on the local MPS tensors. Physically, our condition captures the fact that the mutual information between distant regions of stabilizer fixed points is quantized and remains so after applying shallow quantum circuits.}, archive = {J_PRL}, author = {David Aram Korbany and Michael J. Gullans and Lorenzo Piroli}, doi = {10.1103/1hlj-h6t9}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160404}, shortjournal = {Phys. Rev. Lett.}, title = {Long-range nonstabilizerness and phases of matter}, volume = {135}, year = {2025}, }
• (2025). Multimode cavity QED ising spin glass. PRL, 135(16), 160403. (www)

  @article{ , abstract = {We realize a driven-dissipative Ising spin glass using cavity QED in a novel “4/7” multimode geometry. Gases of ultracold atoms trapped within the cavity by optical tweezers serve as effective spins. They are coupled via randomly signed, all-to-all Ising cavity-mediated interactions. Networks of up to spins are holographically imaged via cavity emission. The system is driven through a frustrated transverse-field Ising transition, and we show that the entropy of the spin glass states depends on the rate at which the transition is crossed. Despite being intrinsically nonequilibrium, the system exhibits phenomena associated with Parisi’s theory of equilibrium spin glasses, namely, replica symmetry breaking (RSB) and ultrametric structure. For system sizes up to , we measure the Parisi function , Edwards-Anderson overlap , and ultrametricity correlator; all indicate a deeply ordered spin glass under RSB. The system can serve as an associative memory and enable aging and rejuvenation studies in driven-dissipative spin glasses at the microscopic level.}, archive = {J_PRL}, author = {Brendan P. Marsh and David Atri Schuller and Yunpeng Ji and Henry S. Hunt and Giulia Z. Socolof and Deven P. Bowman and Jonathan Keeling and Benjamin L. Lev}, doi = {10.1103/x19r-pzyb}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160403}, shortjournal = {Phys. Rev. Lett.}, title = {Multimode cavity QED ising spin glass}, volume = {135}, year = {2025}, }
• (2025). Energetic advantages for quantum agents in online execution of complex strategies. PRL, 135(16), 160402. (www)

  @article{ , abstract = {Agents often execute complex strategies, adapting their response to each input stimulus depending on past observations and actions. Here, we derive the minimal energetic cost for classical agents to execute a given strategy, highlighting that they must dissipate a certain amount of heat with each decision beyond Landauer’s limit. We then prove that quantum agents can reduce this dissipation below classical limits. We establish the necessary and sufficient conditions for a strategy to guarantee quantum agents have energetic advantage, and illustrate settings where this advantage grows without bound. Our results establish a fundamental energetic advantage for agents utilizing quantum processing to enact complex adaptive behavior.}, archive = {J_PRL}, author = {Jayne Thompson and Paul M. Riechers and Andrew J. P. Garner and Thomas J. Elliott and Mile Gu}, doi = {10.1103/dryx-l5rt}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160402}, shortjournal = {Phys. Rev. Lett.}, title = {Energetic advantages for quantum agents in online execution of complex strategies}, volume = {135}, year = {2025}, }
• (2025). Conditional mutual information and information-theoretic phases of decohered gibbs states. PRL, 135(16), 160401. (www)

  @article{ , abstract = {Conditional mutual information (CMI) is a widely studied multipartite correlation measure with a connection to the Markov property. Intriguingly, CMI can be generated by local dissipation, a phenomenon closely related to teleportation. The onset of long-range CMI corresponds to an information-theoretic mixed-state phase transition, with far-ranging implications for phase transitions, decoding, and state compressions. Little is known, however, about the conditions under which dissipation can generate long-range CMI. In this Letter, we provide the first rigorous results in this direction. We establish that CMI in high-temperature commuting Gibbs states subject to local dissipation decays exponentially under certain mild restrictions. Conversely, we show that the same setup can sustain long-range CMI at low temperatures. Our results establish the existence of finite-temperature information-theoretic phase transitions even in models that have no finite-temperature thermodynamic phase transitions.}, archive = {J_PRL}, author = {Yifan F. Zhang and Sarang Gopalakrishnan}, doi = {10.1103/cjkh-1z6c}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160401}, shortjournal = {Phys. Rev. Lett.}, title = {Conditional mutual information and information-theoretic phases of decohered gibbs states}, volume = {135}, year = {2025}, }
• (2025). Invested and potential magic resources in measurement-based quantum computation. PRL, 135(16), 160203. (www)

  @article{ , abstract = {Magic states and magic gates are crucial for achieving universal quantum computation, but important questions about how magic resources should be implemented to attain maximal quantum advantage have remained unexplored, especially in the context of measurement-based quantum computation (MQC). This Letter bridges the gap between MQC and the resource theory of magic by introducing the key concepts of “ invested ” and “ potential ” magic resources. The former quantifies the magic cost associated with MQC, serving as both a resource witness and a feasible upper bound for the practical realization, and is gate-order independent; the latter represents the maximal achievable magic resource in a given graph structure defining MQC. We utilize both concepts to analyze the quantum Fourier transform (QFT) and provide a fresh perspective on the universality of MQC, highlighting the crucial role of non-Pauli measurements in injecting magic. In particular, we theoretically prove that high-dimensional graphs can generate an exponential advantage of MQC compared to classical computing. We demonstrate experimentally our theoretical findings in a high-fidelity four-photon setup, surpassing conventional magic state injection methods in both qubit efficiency and resource utilization. Our findings pave the way for future research exploring magic resource optimization and novel distillation schemes within the MQC framework, advancing fault-tolerant universal quantum computation.}, archive = {J_PRL}, author = {Gong-Chu Li and Lei Chen and Si-Qi Zhang and Xu-Song Hong and Huaqing Xu and Yuancheng Liu and You Zhou and Geng Chen and Chuan-Feng Li and Guang-Can Guo and Alioscia Hamma}, doi = {10.1103/4yyv-hggz}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160203}, shortjournal = {Phys. Rev. Lett.}, title = {Invested and potential magic resources in measurement-based quantum computation}, volume = {135}, year = {2025}, }
• (2025). Generalized indefinite causal orders in an integrated quantum switch. PRL, 135(16), 160202. (www)

  @article{ , abstract = {Indefinite causal order (ICO), a striking feature of quantum mechanics, has attracted broad theoretical and experimental interest. While ICO holds promise for quantum information processing, akin to quantum entanglement, its experimental realization and rigorous verification remain fundamental challenges. Here, we demonstrate and certify generalized multidimensional multipartite ICOs using a programmable integrated-photonic quantum chip implementing a generalized quantum switch. By violating definite causal order bounds with high statistical significance, we experimentally characterize and verify these generalized ICOs. Furthermore, we explore a resource theory of causal nonseparability by implementing a single-copy distillation protocol. Our Letter constitutes a major step toward a generalized framework for quantum causality.}, archive = {J_PRL}, author = {Yaohao Deng and Shuheng Liu and Xiaojiong Chen and Zhaorong Fu and Jueming Bao and Yun Zheng and Qihuang Gong and Qiongyi He and Jianwei Wang}, doi = {10.1103/39vh-84n1}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160202}, shortjournal = {Phys. Rev. Lett.}, title = {Generalized indefinite causal orders in an integrated quantum switch}, volume = {135}, year = {2025}, }
• (2025). Bridging entanglement and magic resources within operator space. PRL, 135(16), 160201. (www)

  @article{ , abstract = {Local-operator entanglement (LOE) dictates the complexity of simulating Heisenberg evolution using tensor network methods, and it bears witness to many-body chaos for local dynamics. We show that LOE is also sensitive to how non-Clifford a unitary is—its magic resources. In particular, we prove that LOE is always upper-bound by three distinct magic monotones: T -count, unitary nullity, and operator-stabilizer Rényi entropy. Moreover, in the average case for large, random circuits, LOE and magic monotones approximately coincide. Our results imply that an operator evolution that is expensive to simulate using tensor network methods must also be inefficient using both stabilizer and Pauli truncation methods. In terms of a previous conjecture on the characteristic scaling of LOE, our results imply that nonintegrable spin chains cannot be simulated classically. Entanglement in operator space therefore measures a unified picture of nonclassical resources, in stark contrast to the Schrödinger picture.}, archive = {J_PRL}, author = {Neil Dowling and Kavan Modi and Gregory A. L. White}, doi = {10.1103/c7k1-xcwy}, journal = {Physical Review Letters}, month = {10}, number = {16}, pages = {160201}, shortjournal = {Phys. Rev. Lett.}, title = {Bridging entanglement and magic resources within operator space}, volume = {135}, year = {2025}, }
• (2025). Erratum: Thermally bianisotropic metamaterials induced by spatial asymmetry [Phys. rev. lett. 135, 116303 (2025)]. PRL, 135(15), 159902. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 159902 (2025)}, archive = {J_PRL}, author = {Gal Shmuel and John R. Willis}, doi = {10.1103/rkyy-m7hc}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {159902}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Thermally bianisotropic metamaterials induced by spatial asymmetry [Phys. rev. lett. 135, 116303 (2025)]}, volume = {135}, year = {2025}, }
• (2025). Erratum: New method for the astrometric direct detection of ultralight dark matter [Phys. rev. lett. 134, 111003 (2025)]. PRL, 135(15), 159901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 159901 (2025)}, archive = {J_PRL}, author = {Jeff A. Dror and Sarunas Verner}, doi = {10.1103/qcz6-g71m}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {159901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: New method for the astrometric direct detection of ultralight dark matter [Phys. rev. lett. 134, 111003 (2025)]}, volume = {135}, year = {2025}, }
• (2025). Comment on “Shell-shaped quantum droplet in a three-component ultracold bose gas”. PRL, 135(15), 159301. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 159301 (2025)}, archive = {J_PRL}, author = {Francesco Ancilotto}, doi = {10.1103/ycst-x8d5}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {159301}, shortjournal = {Phys. Rev. Lett.}, title = {Comment on “Shell-shaped quantum droplet in a three-component ultracold bose gas”}, volume = {135}, year = {2025}, }
• (2025). Bridging-induced phase separation and loop extrusion drive noise in chromatin transcription. PRL, 135(15), 158401. (www)

  @article{ , abstract = {Cell-to-cell heterogeneity in transcription, or transcriptional noise, is important in cellular development and in disease. The molecular mechanisms driving it are, however, elusive and ill-understood. Here, we use computer simulations to explore the role of 3D chromatin structure in driving transcriptional noise. We study a simple polymer model where proteins—modeling complexes of transcription factors and polymerases—bind multivalently to transcription units—modeling regulatory elements such as promoters and enhancers. We also include cohesinlike factors that extrude chromatin loops that are important for the physiological folding of chromosomes. We find that transcription factor binding creates spatiotemporal patterning and a highly variable correlation time in transcriptional dynamics, which is linked to the cell-to-cell variation in gene expression. Loop extrusion also contributes to noise, as the stochastic nature of this process leads to different networks of cohesin loops in different cells in our model. Our results could be tested with single-cell experiments and provide a pathway to understanding the principles underlying transcriptional plasticity in vivo .}, archive = {J_PRL}, author = {Michael Chiang and Cleis Battaglia and Giada Forte and Chris A. Brackley and Nick Gilbert and Davide Marenduzzo}, doi = {10.1103/bjq4-xnsy}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {158401}, shortjournal = {Phys. Rev. Lett.}, title = {Bridging-induced phase separation and loop extrusion drive noise in chromatin transcription}, volume = {135}, year = {2025}, }
• (2025). Motility-induced crystallization and rotating crystallites. PRL, 135(15), 158301. (www)

  @article{ , abstract = {Active soft matter frequently shows motility-induced phase separation, where self-propelled particles condensate into clusters with an inner liquidlike structure. Such activity may also result in motility-induced crystallization into clusters with an inner crystalline structure. We derive a higher-order active phase-field-crystal model and employ it to study the interplay of passive (i.e., thermodynamic) and active (i.e., motility-induced) condensation or evaporation and crystallization or melting. Stability and morphological phase diagrams indicate the various occurring phase coexistences and transitions, e.g., the destruction of passive clusters in the case of a density-independent effective velocity and the possible creation of active clusters in the case of a density-dependent effective velocity. Finally, simple and complex rotating crystallites are discussed, including states of time-periodic chirality.}, archive = {J_PRL}, author = {Max Philipp Holl and Alina Barbara Steinberg and Michael te Vrugt and Uwe Thiele}, doi = {10.1103/m3dy-53yc}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {158301}, shortjournal = {Phys. Rev. Lett.}, title = {Motility-induced crystallization and rotating crystallites}, volume = {135}, year = {2025}, }
• (2025). Time is length in self-similar logarithmic aging of physically cross-linked semiflexible polymer networks. PRL, 135(15), 158101. (www)

  @article{ , abstract = {Physical aging in polymers is a fundamental yet poorly understood phenomenon, as diverse macromolecular systems exhibit remarkably similar slow dynamics. Through molecular dynamics simulations of physically cross-linked networks composed of semiflexible polymers, we identify a previously unexplored class of self-similar aging. The network undergoes ultraslow coarsening characterized by a logarithmically growing mesh size, which governs the spatial organization, cohesive and bending energies, and the aging dynamics of the system. This single time-dependent length scale defines an internal clock, giving rise to spatiotemporal self-similarity of both structure and dynamics—offering a perspective on aging in soft and disordered materials.}, archive = {J_PRL}, author = {Patrick Ilg and Clarisse Luap and Martin Kröger}, doi = {10.1103/1slf-41nm}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {158101}, shortjournal = {Phys. Rev. Lett.}, title = {Time is length in self-similar logarithmic aging of physically cross-linked semiflexible polymer networks}, volume = {135}, year = {2025}, }
• (2025). Perturbed nonlinear evolution of optical soliton gases: Growth and decay in integrable turbulence. PRL, 135(15), 157201. (www)

  @article{ , abstract = {We present optical fiber experiments investigating the perturbed, nonintegrable evolution of soliton gases (SGs) under weak linear damping and gain. By measuring the amplitude and phase of the optical field in a recirculating loop, we determine the spectral distribution of SGs at various propagation distances. We demonstrate that a SG, initially prepared as a soliton condensate with a Weyl distribution, undergoes significant changes in its spectral distribution due to dissipation. Specifically, weak gain leads to the emergence of a bichromatic SG, while weak damping results in a SG with a semicircular spectral distribution at long propagation distances. These observed dissipation-driven changes in the SG’s spectral characteristics are not explained by existing hydrodynamic or kinetic theories.}, archive = {J_PRL}, author = {Loic Fache and François Copie and Pierre Suret and Stéphane Randoux}, doi = {10.1103/hwpr-628r}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {157201}, shortjournal = {Phys. Rev. Lett.}, title = {Perturbed nonlinear evolution of optical soliton gases: Growth and decay in integrable turbulence}, volume = {135}, year = {2025}, }
• (2025). Measuring chemical shifts with energy-dispersive X-ray spectroscopy. PRL, 135(15), 157002. (www)

  @article{ , abstract = {Electron microscopy uses energy-dispersive x-ray spectroscopy (EDS) and electron energy loss spectroscopy (EELS) for elemental analysis. EDS and EELS energy resolutions are commonly between 30 and 100 eV or 0.01 and 1 eV, respectively. Large solid angle EDS detector technology has increased collection efficiency to enable precision spectroscopy via averaging of 0.02–0.1 eV. This improved precision gives access to chemical shifts; examples are shown in compounds of Al, Ti, and W. EDS can now detect chemical information in a complementary parameter space (accelerating voltage, thickness, atomic number) to that covered by EELS.}, archive = {J_PRL}, author = {Yueyun Chen and Rebekah Jin and Yarin Heffes and Brian Zutter and Tristan P. O’Neill and Jared J. Lodico and B. C. Regan and Matthew Mecklenburg}, doi = {10.1103/t1rs-7kr2}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {157002}, shortjournal = {Phys. Rev. Lett.}, title = {Measuring chemical shifts with energy-dispersive X-ray spectroscopy}, volume = {135}, year = {2025}, }
• (2025). Nearly temperature-independent gate-electric-field-driven lateral migration of electrons in Si3N4 charge trap layer of flash memory devices. PRL, 135(15), 157001. (www)

  @article{ , abstract = {Through experiments and a proposed model, we revealed for the first time why electrons laterally migrate within the charge trap layer during the programming of flash memory devices. The proposed thermally assisted trap-to-band tunneling emission model well explained the measured electric field and temperature effects on the lateral migration of electrons. The proposed model was emulated in a commercial technology computer-aided design tool through a user interface, enabling accurate physical analysis. This model can be used to design devices utilizing lateral migration of electrons or to analyze various phenomena in vertical NAND flash memory, such as space program and Z interference.}, archive = {J_PRL}, author = {Joon Hwang and Min-Kyu Park and Joonhyung Cho and Yeongheon Yang and Jong-Ho Bae and Jong-Ho Lee}, doi = {10.1103/lj4r-dcb7}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {157001}, shortjournal = {Phys. Rev. Lett.}, title = {Nearly temperature-independent gate-electric-field-driven lateral migration of electrons in Si3N4 charge trap layer of flash memory devices}, volume = {135}, year = {2025}, }
• (2025). Formulation of dispersive and dissipative time-varying media as a floquet matrix eigenproblem. PRL, 135(15), 156903. (www)

  @article{ , abstract = {Dispersion is ubiquitous in nature as a result of causality, and dispersive time-varying materials have been widely used in the experimental realization of photonic time-varying media. Here, we derive the Floquet Hamiltonian and formulate Maxwell’s equations of dispersive time-varying media as a Floquet matrix eigenproblem. The derived Floquet Hamiltonian allows us to investigate the band structures and eigenmodes of the system. Using the eigenmodes, we identify the Floquet π exceptional points by tracking the variation of Aharonov-Anandan phase. Our theory rigorously reformulates existing models and facilitates the development of Floquet Green’s function and resonant mode expansion in open photonic time-varying systems.}, archive = {J_PRL}, author = {Yuchen Sun and Shanhui Fan and Guangwei Hu}, doi = {10.1103/lcmw-qrrp}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156903}, shortjournal = {Phys. Rev. Lett.}, title = {Formulation of dispersive and dissipative time-varying media as a floquet matrix eigenproblem}, volume = {135}, year = {2025}, }
• (2025). Surface-mediated ultrastrong cavity coupling of two-dimensional itinerant electrons. PRL, 135(15), 156902. (www)

  @article{ , abstract = {Engineering phases of matter in cavities requires effective light-matter coupling strengths that are on the same order of magnitude as the bare system energetics, coined the ultrastrong coupling regime. For models of itinerant electron systems, which do not have discrete energy levels, a clear definition of this regime has been lacking to date. Here, we argue that a change of the electronic mass exceeding 10% of its bare value may serve as such a definition. We propose a quantitative computational scheme for obtaining the electronic mass in relation to its bare vacuum value and show that coupling to surface polariton modes can induce such mass changes. Our results have important implications for cavity design principles that enable the engineering of electronic properties with quantum light.}, archive = {J_PRL}, author = {Christian J. Eckhardt and Andrey Grankin and Dante M. Kennes and Michael Ruggenthaler and Angel Rubio and Michael A. Sentef and Mohammad Hafezi and Marios H. Michael}, doi = {10.1103/2fw2-lbhy}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156902}, shortjournal = {Phys. Rev. Lett.}, title = {Surface-mediated ultrastrong cavity coupling of two-dimensional itinerant electrons}, volume = {135}, year = {2025}, }
• (2025). Twist engineering of anisotropic excitonic and optical properties of a two-dimensional magnetic semiconductor. PRL, 135(15), 156901. (www)

  @article{ , abstract = {Two-dimensional (2D) van der Waals (vdW) magnetic semiconductors are a new class of quantum materials for studying the emergent physics of excitons and spins in the 2D limit. Twist engineering provides a powerful tool to manipulate the fundamental properties of 2D vdW materials. Here, we show that twist engineering of the anisotropic ferromagnetic monolayer semiconductor CrSBr leads to bilayer magnetic semiconductors with continuously tunable magnetic moment, dielectric anisotropy, exciton energy, and linear dichroism. We furthermore provide a model for exciton energy in the media with tunable anisotropy. These results advance fundamental studies of 2D vdW materials and open doors to applications to nano-optics, twistronics, and spintronics.}, archive = {J_PRL}, author = {Qiuyang Li and Xiaohan Wan and Senlei Li and Adam Alfrey and Wenhao Liu and Zixin Zhai and Wyatt Alpers and Yujie Yang and Irmina Wladyszewska and Christiano W. Beach and Liuyan Zhao and Bing Lv and Chunhui Rita Du and Kai Sun and Hui Deng}, doi = {10.1103/zbbr-5mgv}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156901}, shortjournal = {Phys. Rev. Lett.}, title = {Twist engineering of anisotropic excitonic and optical properties of a two-dimensional magnetic semiconductor}, volume = {135}, year = {2025}, }
• (2025). Prediction of room temperature ferroelectricity in subnano silicon thin films with an antiferroelectric ground state. PRL, 135(15), 156801. (www)

  @article{ , abstract = {Recent advancements highlight the critical need for ferroelectric (FE) materials compatible with silicon, particularly pure silicon phases exhibiting FE behavior above room temperature that can be readily integrated onto silicon substrates. Here, we systematically predict potential FE silicon films using first-principles structure searching. Furthermore, we develop an advanced machine learning model that simultaneously predicts interatomic potentials and Born effective charges to investigate their FE behavior. In particular, we discover a low-energy FE silicon film merely above its antiferroelectric (AFE) ground state. Both phases are confirmed to be dynamically and mechanically stable semiconductors with indirect band gaps of approximately 1.3 eV. Although the ground state exhibits AFE ordering, our simulations with the machine learning model remarkably reveal a robust FE hysteresis loop above room temperature, characterized by a low coercive field of about . An effective Hamiltonian model analysis indicates that this anomalous FE behavior arises from weak AFE coupling between the top and bottom surfaces of the silicon film. These findings of a switchable FE state in pure silicon phases suggest their potential use in memory devices, sensors, and energy converters.}, archive = {J_PRL}, author = {Hongyu Yu and Shihan Deng and Haiyan Zhu and Muting Xie and Yuwen Zhang and Xizhi Shi and Jianxin Zhong and Chaoyu He and Hongjun Xiang}, doi = {10.1103/xlkt-4wk5}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156801}, shortjournal = {Phys. Rev. Lett.}, title = {Prediction of room temperature ferroelectricity in subnano silicon thin films with an antiferroelectric ground state}, volume = {135}, year = {2025}, }
• (2025). Possible observation of quadrupole waves in spin nematics. PRL, 135(15), 156704. (www)

  @article{ , abstract = {Discovery of new states of matter is a key objective in modern condensed matter physics, which often leads to revolutionary technological advancements such as superconductivity. Quantum spin nematic, a “hidden order” that evades conventional magnetic probes, is one such state. is a potential spin nematic material, suggested by the observation of a two-magnon Bose-Einstein condensation from above the saturation field. However, direct confirmation of the spin nematicity remains elusive. This Letter presents inelastic neutron scattering spectra from the putative spin nematic phases of , revealing low-energy quadrupole waves that are absent in the neighboring conventional magnetic phases. A spin-one model quantitatively captures the full details of the spin excitation spectra across all low-temperature phases, providing direct evidence of the spin nematic orders. Additionally, we show evidence of the three-magnon continuum and two-magnon bound states in the -magnetization plateau, revealing condensation of the two-magnon bound state as the origin of the low-field spin nematic supersolid phase.}, archive = {J_PRL}, author = {Jieming Sheng and Jiahang Hu and Lei Xu and Le Wang and Xiaojian Shi and Runze Chi and Dehong Yu and Andrey Podlesnyak and Pharit Piyawongwatthana and Naoki Murai and Seiko Ohira-Kawamura and Huiqiu Yuan and Ling Wang and Jia-Wei Mei and Hai-Jun Liao and Tao Xiang and Liusuo Wu and Zhentao Wang}, doi = {10.1103/pywx-vxfh}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156704}, shortjournal = {Phys. Rev. Lett.}, title = {Possible observation of quadrupole waves in spin nematics}, volume = {135}, year = {2025}, }
• (2025). Probing nonlinear spin dynamics in canted easy-plane antiferromagnets using spin-rectification effects. PRL, 135(15), 156703. (www)

  @article{ , abstract = {We investigate spin-rectification phenomena in canted antiferromagnets, closely connected to the family of altermagnetic materials. Our results show that excitation efficiency is significantly enhanced by the Dzyaloshinskii-Moriya interaction. Antiferromagnetic dynamics can be detected through spin-Hall magnetoresistance and bolometric effects, with an efficiency reaching up to mV / W . The rectified voltage is influenced by the symmetry of the exciting torques, detection mechanisms (continuous spin-pumping and spin-Hall magnetoresistance), and the antiferromagnetic crystalline axis. Under high pumping power, we observe a saturation effect related to Suhl-like spin-wave instabilities and a nonlinear redshift of the antiferromagnetic resonance. These findings open new avenues for studying nonlinear dynamics in antiferromagnetic and altermagnetic spintronic devices.}, archive = {J_PRL}, author = {A. El Kanj and S. Mantion and I. Boventer and P. Bortolotti and V. Cros and A. Anane and O. Gomonay and R. Lebrun}, doi = {10.1103/vwd1-7r11}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156703}, shortjournal = {Phys. Rev. Lett.}, title = {Probing nonlinear spin dynamics in canted easy-plane antiferromagnets using spin-rectification effects}, volume = {135}, year = {2025}, }
• (2025). Large orbital torque from interfacial spin-vorticity coupling in PtCo/Cu heterostructures. PRL, 135(15), 156702. (www)

  @article{ , abstract = {The use of orbital torques to efficiently modulate magnetization is currently a central topic in orbitronics. In this Letter, we report the discovery of an unexpectedly large dampinglike torque efficiency per unit electric field in metallic heterostructures, with its maximum value being 2 (1) orders of magnitude higher than that in typical heavy-metal Ta (Pt) systems. Current-induced magnetization reversal experiments confirm the enhanced dampinglike torque efficiency, which increases significantly with the thickness of the Cu layer. We attribute this ultraefficient orbital torque to the interfacial vorticity of the drift velocity of conduction electrons, arising from the substantial resistivity difference between the Cu and PtCo layers. The remarkable dampinglike torque efficiency demonstrated in our Letter highlights the potential of interfacial vorticity in spin orbitronics, suggesting a promising new direction for future research in the field.}, archive = {J_PRL}, author = {Longwen Yi and Tianxiang Yang and Cheng Tan and Ronghuan Xie and Senmiao Liu and Li Cai and Qiang Cao and Yan Wang and Weiming Lü and Yufeng Tian and QiKun Huang and Shishen Yan}, doi = {10.1103/qgdy-k39l}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156702}, shortjournal = {Phys. Rev. Lett.}, title = {Large orbital torque from interfacial spin-vorticity coupling in PtCo/Cu heterostructures}, volume = {135}, year = {2025}, }
• (2025). Strongly inhomogeneous spin dynamics induced by ultrashort laser pulses with a gradient intensity profile. PRL, 135(15), 156701. (www)

  @article{ , abstract = {The optical pump-probe technique is a common tool for the investigation of ultrafast spin dynamics, which usually utilizes single-diode detection averaging the dynamics over the pumped area. Using an ultrafast imaging technique, we show experimentally that a femtosecond laser pulse with a gradient distribution of intensity efficiently excites strongly inhomogeneous spin dynamics on spatial scales much smaller than the pump spot size. The mechanism responsible for the inhomogeneous distribution is based on temperature gradients and corresponds to a sign change of the torque derivative in different areas of the pump. We argue that the observed phenomenon is general for the systems with competitive magnetic anisotropies. Overlooking this effect in the majority of pump-probe experiments can result in a dramatic underestimate of the lifetime and amplitude of the laser-induced spin dynamics.}, archive = {J_PRL}, author = {T. T. Gareev and N. E. Khokhlov and L. Körber and A. V. Kimel}, doi = {10.1103/gspf-b9n2}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156701}, shortjournal = {Phys. Rev. Lett.}, title = {Strongly inhomogeneous spin dynamics induced by ultrashort laser pulses with a gradient intensity profile}, volume = {135}, year = {2025}, }
• (2025). Artificial gauge field engineered excited-state topology: Control of dynamical evolution of localized spinons. PRL, 135(15), 156601. (www)

  @article{ , abstract = {Spinons are elementary excitations at the core of frustrated quantum magnets. Although it is well established that a pair of spinons can emerge from a magnon via deconfinement, controlled manipulation of individual spinons and direct observation of their deconfinement remain elusive. We propose an artificial gauge field scenario that enables the engineering of specific excited states in quantum spin models. This generates spatially localized individual spinons with high controllability. By applying time-dependent gauge fields, we realize adiabatic braiding of these spinons, as well as their dynamical evolution in a controllable manner. These results not only provide the first direct visualization of individual spinons localized in the bulk, but also point to new possibilities to simulate their confinement process. Finally, we demonstrate the feasibility of our scenario in Rydberg atoms, which suggests an experimentally viable direction-gauge-field engineering of correlated phenomena in excited states.}, archive = {J_PRL}, author = {Jie Ren and Yi-Ran Xue and Run-Jia Luo and Rui Wang and Baigeng Wang}, doi = {10.1103/ll8w-g9q1}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156601}, shortjournal = {Phys. Rev. Lett.}, title = {Artificial gauge field engineered excited-state topology: Control of dynamical evolution of localized spinons}, volume = {135}, year = {2025}, }
• (2025). Uniaxial-pressure control of excitonic fluctuations and monoclinic distortions in Ta2NiSe5. PRL, 135(15), 156503. (www)

  @article{ , abstract = {Ta 2 NiSe 5 undergoes a phase transition characterized by the opening of an energy gap and a reduction in its crystal symmetry below T c = 326 K . The primary cause of this transition is debated to be either electron-hole correlations, in line with the excitonic insulator hypothesis, or structural instability. The chain structure of Ta 2 NiSe 5 enables effective control over its electronic and lattice properties by applying uniaxial strain. In this study, we utilize polarization-resolved Raman spectroscopy to demonstrate that the electronic and structural order parameters respond differently to uniaxial pressure applied along the Ta-Ni chains. Compressive strain reduces monoclinic distortions while enhancing excitonic fluctuations. Such disparate behavior suggests that many-body effects may significantly amplify exciton fluctuations even when monoclinic distortions are minimized, thereby supporting the excitonic nature of the phase transition.}, archive = {J_PRL}, author = {X. Shi and Y.-S. Zhang and D. Huang and M. Isobe and H. Takagi and B. Keimer and A. V. Boris}, doi = {10.1103/jysr-2dk1}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156503}, shortjournal = {Phys. Rev. Lett.}, title = {Uniaxial-pressure control of excitonic fluctuations and monoclinic distortions in Ta2NiSe5}, volume = {135}, year = {2025}, }
• (2025). Altermagnetism in modified lieb lattice hubbard model. PRL, 135(15), 156502. (www)

  @article{ , abstract = {We study the emergence of altermagnetism from repulsive interactions for electrons on the Lieb lattice as a model of quasi-2D oxychalcogenides with the so-called “ ” lattice structure. A comprehensive study of the Lieb lattice Hubbard model, using unrestricted Hartree-Fock and exact diagonalization techniques, establishes the presence of a spin- altermagnetic Mott insulating ground state for average electron densities of 2 and 4 per unit cell. Both phases show the characteristic spin splitting in the electron bands as well as in the magnon bands, as indicated by solutions of an effective spin- Heisenberg model that we construct. We also provide evidence for altermagnetic metal formation in the electron- and hole-doped Mott state, giving rise to Fermi surfaces with -wave spin splitting and quasi-one-dimensional characteristics.}, archive = {J_PRL}, author = {Nitin Kaushal and Marcel Franz}, doi = {10.1103/s31h-hk2v}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156502}, shortjournal = {Phys. Rev. Lett.}, title = {Altermagnetism in modified lieb lattice hubbard model}, volume = {135}, year = {2025}, }
• (2025). Quantum oscillations in the heat capacity of kondo insulator YbB12. PRL, 135(15), 156501. (www)

  @article{ , abstract = {We observe magnetic quantum oscillations in the heat capacity of the Kondo insulator . The frequency of these oscillations, agrees with that from magnetoresistance and torque magnetometry experiments for in the Kondo insulating phase. Remarkably, the quantum-oscillation amplitudes in the heat capacity are substantial, with at 0.8 K, accounting for 13% of the known linear heat-capacity coefficient . Double-peak structures of quantum-oscillation amplitudes due to the distribution function of fermions were identified and used to determine the value of the effective mass from the heat capacity, which agrees well with that from torque magnetometry. These observations support bulk charge-neutral fermions contributing to the quantum oscillations in .}, archive = {J_PRL}, author = {Kuan-Wen Chen and Yuan Zhu and Danilo Ratkovski and Guoxin Zheng and Dechen Zhang and Aaron Chan and Kaila Jenkins and Joanna Blawat and Tomoya Asaba and Fumitoshi Iga and Chandra M. Varma and Yuji Matsuda and John Singleton and Alimamy F. Bangura and Lu Li}, doi = {10.1103/ms3x-pjsk}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156501}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum oscillations in the heat capacity of kondo insulator YbB12}, volume = {135}, year = {2025}, }
• (2025). Electronic correlations in rhombohedral graphene at atomic scale. PRL, 135(15), 156401. (www)

  @article{ , abstract = {Rhombohedral graphene (RG) has emerged as a promising platform for exploring exotic quantum phenomena, such as quantum magnetism, unconventional superconductivity, and fractional quantum anomalous Hall effects. Despite its potential, atomic-scale investigations of RG remain limited, hindering a detailed microscopic understanding of the origins of these correlated states. In this Letter, we employ scanning probe microscopy and spectroscopy to probe the intrinsic electronic states in trilayer and tetralayer RG. We identify a correlated insulating state with a gap up to 19 meV at the charge neutrality point in tetralayer RG, which is absent in the trilayer RG and Bernal stacking tetralayer. This gap is suppressed by applying a perpendicular magnetic field or doping the charge carrier density and does not exhibit intervalley coherence patterns. We attribute this phenomenon to a symmetry-broken layer antiferromagnetic state, characterized by ferrimagnetic ordering in the outermost layers and antiferromagnetic coupling between them. To further investigate this magnetic correlated state, we conduct local scattering experiments. Within the correlated regime, a threefold symmetric pattern emerges around a possible nonmagnetic impurity, suggesting that nonmagnetic doping may induce a spin texture in the ferrimagnetic surface layers. Outside the correlated regime, Friedel oscillations are observed, allowing precise determination of the band dispersion in tetralayer RG. These findings provide atomic-scale evidences of zero-field correlations in RG and may be extended to study other exotic phases in RG.}, archive = {J_PRL}, author = {Yufeng Liu and Zonglin Li and Shudan Jiang and Min Li and Yu Gu and Kai Liu and Qia Shen and Liang Liu and Xiaoxue Liu and Dandan Guan and Yaoyi Li and Hao Zheng and Canhua Liu and Kenji Watanabe and Takashi Taniguchi and Jinfeng Jia and Tingxin Li and Guorui Chen and Jianpeng Liu and Can Li and Zhiwen Shi and Shiyong Wang}, doi = {10.1103/fv52-pd3h}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156401}, shortjournal = {Phys. Rev. Lett.}, title = {Electronic correlations in rhombohedral graphene at atomic scale}, volume = {135}, year = {2025}, }
• (2025). Quantum response theory and momentum-space gravity. PRL, 135(15), 156302. (www)

  @article{ , abstract = {We present a quantum response approach to momentum-space gravity in dissipative multiband systems, which dresses both the quantum geometry—through an interband Weyl transformation—and the equations of motion. In addition to clarifying the roles of the contorsion and symplectic terms, we introduce the three-state quantum geometric tensor as a necessary element in the geometric classification of nonlinear responses and discuss the significance of the emergent terms from a gravitational point of view. We also identify a dual quantum geometric drag force in momentum space that provides an entropic source term for the multiband matrix of Einstein field equations.}, archive = {J_PRL}, author = {M. Mehraeen}, doi = {10.1103/t6nt-qzws}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156302}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum response theory and momentum-space gravity}, volume = {135}, year = {2025}, }
• (2025). Voltage-tuned anomalous-metal to metal transition in hybrid josephson junction arrays. PRL, 135(15), 156301. (www)

  @article{ , abstract = {We report on voltage-tuned phase transitions in arrays of hybrid semiconductor-superconductor islands arranged in a square lattice. A double-layer electrostatic gate geometry enables independent tuning of interisland coupling and proximity-induced superconductivity. This design enables access to the superconductor-insulator, superconductor-metal, and metal-insulator transitions in a single device, revealing critical points and emergent intermediate phases. We find that the superconductor-insulator transition is interrupted by an anomalous metallic phase with saturating low-temperature resistivity. Across gate voltages, this regime extends over 3 orders of magnitude in resistivity and can be continuously tuned into the conventional metallic phase. The signature of the anomalous metallic phase is suppressed by magnetic frustration.}, archive = {J_PRL}, author = {S. Sasmal and M. Efthymiou-Tsironi and G. Nagda and E. Fugl and L. L. Olsen and F. Krizek and C. M. Marcus and S. Vaitiekėnas}, doi = {10.1103/xbm4-37cf}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156301}, shortjournal = {Phys. Rev. Lett.}, title = {Voltage-tuned anomalous-metal to metal transition in hybrid josephson junction arrays}, volume = {135}, year = {2025}, }
• (2025). Transparency of graphene to solid-solid van der waals interactions. PRL, 135(15), 156202. (www)

  @article{ , abstract = {Understanding the transparency of two-dimensional (2D) materials to intermolecular interactions—particularly their ability to transmit van der Waals (vdW) forces—is crucial for applications such as the design of 2D material-based nanofluidic and microelectromechanical systems. However, experimental studies have produced inconsistent and even contradictory conclusions regarding the vdW transparency of 2D materials. Here, we employ colloidal atomic force microscopy with a geometrically well-defined probe to measure pull-off and pull-in forces in a model system: graphene on silicon dioxide ( SiO 2 ). Our results reveal that the total vdW force deviates significantly from the naive sum of contributions from graphene and its substrate. Intriguingly, the measured pull-off forces indicate that the effective surface energy of a suspended graphene monolayer can exceed that of its substrate-supported counterpart. Furthermore, our measurements of pull-in forces in substrate-supported systems suggest that graphene of 1–5 layers screens 15%–50% of the intrinsic solid-solid vdW interaction, consistent with Lifshitz theory calculations.}, archive = {J_PRL}, author = {Chuanli Yu and Weijia Zeng and Zepu Kou and Wenxiang Wang and Ling Wang and Qunyang Li and Xiaofei Liu and Zhaohe Dai}, doi = {10.1103/jgqz-gwlc}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156202}, shortjournal = {Phys. Rev. Lett.}, title = {Transparency of graphene to solid-solid van der waals interactions}, volume = {135}, year = {2025}, }
• (2025). Resolving elementary steps of vapor-phase dealloying via in situ transmission electron microscopy. PRL, 135(15), 156201. (www)

  @article{ , abstract = {Nanopores evolve in dealloying to dictate alloy corrosion while enabling the creation of functional metallic nanomaterials. Yet, the nanoscale dynamics of the porosity evolution have long eluded experimental characterizations. With aberration-corrected transmission electron microscopy, we reveal the evolution of nanoporous Co from the vapor phase dealloying (VPD) of -CoZn across scales. The in situ characterization confirms key aspects of the dealloying mechanism based on macroscopic characterizations and simulations, including dissolution by repeated step flow and vacancy-cluster nucleation as well as ligament and pore bifurcation. It also separates the step flow kinetics from that of VPD, revealing that a bond energy difference between the alloy constituents can determine the dealloying kinetics and affect the morphology. The findings refine the classic dealloying theory for potentially new fabrications.}, archive = {J_PRL}, author = {Xinyao Wang and Yanying Li and Yuqiao Zeng and Yanyue Wang and Mingwei Chen and Qing Chen and Pan Liu}, doi = {10.1103/22l6-jmw7}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156201}, shortjournal = {Phys. Rev. Lett.}, title = {Resolving elementary steps of vapor-phase dealloying via in situ transmission electron microscopy}, volume = {135}, year = {2025}, }
• (2025). Multipoint correlations in poisson media. PRL, 135(15), 156101. (www)

  @article{ , abstract = {Multipoint correlations in randomly heterogeneous composite media are determined by the probability that a set of points belong to specific phases. They determine a wide range of macroscopic transport properties such as conductivity, dielectric constant, diffusion coefficient, and transmittance. The Poisson model—a random tesselation of space by hyperplanes—provides realistic descriptions of heterogeneous media in, e.g., radiation-transport applications; yet, until now, it has lacked closed-form expressions for its multipoint correlations. We resolve this problem by presenting an exact solution for the multipoint correlations in the Poisson model. By comparing it to Monte Carlo simulations of four-point correlations in three dimensions, we demonstrate the accuracy of our solution. We visualize the multipoint correlations and discuss their features.}, archive = {J_PRL}, author = {Alec Shelley and Aaron Olson and Gianluca Geraci and Daniel M. Tartakovsky}, doi = {10.1103/325k-g4dr}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156101}, shortjournal = {Phys. Rev. Lett.}, title = {Multipoint correlations in poisson media}, volume = {135}, year = {2025}, }
• (2025). Frustrated frustration of arrays with four-terminal nb-pt-nb josephson junctions. PRL, 135(15), 156002. (www)

  @article{ , abstract = {We study the frustration pattern of a square lattice with in situ fabricated Nb-Pt-Nb four-terminal Josephson junctions. The four-terminal geometry gives rise to a checkerboard pattern of alternating fluxes , piercing the plaquettes, which stabilizes the Berezinskii-Kosterlitz-Thouless transition even at irrational flux quanta per plaquette, due to an unequal repartition of integer flux sum into alternating plaquettes. This type of frustrated frustration manifests as a beating pattern of the dc resistance, with state configurations at the resistance dips gradually changing between the conventional zero- and half-flux states. Hence, the four-terminal Josephson junction array offers a promising platform to study previously unexplored flux and vortex configurations and provides an estimate on the spatial expansion of the four-terminal Josephson junction central weak link area.}, archive = {J_PRL}, author = {Justus Teller and Christian Schäfer and Kristof Moors and Benjamin Bennemann and Matvey Lyatti and Florian Lentz and Detlev Grützmacher and Roman-Pascal Riwar and Thomas Schäpers}, doi = {10.1103/gxdc-py56}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156002}, shortjournal = {Phys. Rev. Lett.}, title = {Frustrated frustration of arrays with four-terminal nb-pt-nb josephson junctions}, volume = {135}, year = {2025}, }
• (2025). Intra-unit-cell singlet pairing mediated by altermagnetic fluctuations. PRL, 135(15), 156001. (www)

  @article{ , abstract = {We investigate the superconducting instabilities induced by altermagnetic fluctuations. Because of the nontrivial sublattice structure of the altermagnetic order, shorter-range and longer-range fluctuations favor qualitatively different types of pairing states. Specifically, while the latter stabilize a standard spin-triplet p -wave state, just like ferromagnetic fluctuations, the former leads to intra-unit-cell pairing, in which the Cooper pairs are formed by electrons from different sublattices. The symmetry of the intra-unit-cell gap function can be not only p -wave, but also spin-singlet s -wave and d -wave, depending on the shape of the Fermi surface. We also show that coexistence with altermagnetic order promotes intrinsic nontrivial topology, such as protected Bogoliubov Fermi surfaces and higher-order topological superconductivity. Our Letter establishes the key role played by sublattice degrees of freedom in altermagnetic-fluctuation mediated interactions.}, archive = {J_PRL}, author = {Yi-Ming Wu and Yuxuan Wang and Rafael M. Fernandes}, doi = {10.1103/dlpb-gfct}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {156001}, shortjournal = {Phys. Rev. Lett.}, title = {Intra-unit-cell singlet pairing mediated by altermagnetic fluctuations}, volume = {135}, year = {2025}, }
• (2025). Enhancement to fusion reactivity in sheared flows. PRL, 135(15), 155101. (www)

  @article{ , abstract = {Sheared flow increases the reactivity of fusion plasma. In unmagnetized plasma with flow gradients comparable to the mean free path of reacting ions, fusion reactivity can be more than doubled. The effect is of particular relevance to inertial confinement fusion (ICF), where it allows implosion kinetic energy to contribute to the fusion burn even before thermalizing. Because colder fuel stops alpha particles more quickly, ignition is possible in a smaller volume, substantially reducing energy requirements in fast-ignition designs.}, archive = {J_PRL}, author = {Henry Fetsch and Nathaniel J. Fisch}, doi = {10.1103/5nll-y8rx}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {155101}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancement to fusion reactivity in sheared flows}, volume = {135}, year = {2025}, }
• (2025). Terahertz surface wave compression for low-energy electron diffraction and imaging. PRL, 135(15), 155002. (www)

  @article{ , abstract = {Low-energy electrons, with their large scattering cross sections and exceptional sensitivity to electric fields, have attracted considerable attention for probing ultrafast surface structural and electronic dynamics, particularly through techniques such as low-energy electron diffraction and imaging. However, the significant dispersion of low-energy electron pulses during transport poses a critical challenge to achieving high temporal resolution in time-resolved experiments. In this Letter, we present an at-the-source compression method for low-energy electron pulses using terahertz surface waves on a micrometer-sized tip cathode. Simultaneous electron acceleration and compression have been achieved directly at the emitter surface within a few tens of micrometers. A low-energy (1.5 keV) electron beam with near femtocoulomb charge is temporally compressed by a factor of 3.5, producing 74-femtosecond (FWHM) electron bunches. The quality of the compressed electron bunches is validated through high-quality diffraction patterns of few-layer graphene and projection imaging of a copper mesh. Furthermore, the compressed electrons are applied to investigate the transient electric field propagation generated by photoexcited charged particles on metal surfaces, demonstrating the enhanced temporal resolution. This advancement presents the most compact solution for an electron gun that integrates electron generation, acceleration, and compression into a unified system, paving the way for investigating surface dynamics and complex material phenomena with unprecedented precision.}, archive = {J_PRL}, author = {Dace Su and Jiaqi Zheng and Lingbin Zheng and Xie He and Jianwei Ying and Peng Yuan and Günther H. Kassier and Dongfang Zhang and Liejia Qian}, doi = {10.1103/ys1r-nns3}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {155002}, shortjournal = {Phys. Rev. Lett.}, title = {Terahertz surface wave compression for low-energy electron diffraction and imaging}, volume = {135}, year = {2025}, }
• (2025). High-efficiency plasma-based compressor for ultrafast soft X-ray free-electron lasers. PRL, 135(15), 155001. (www)

  @article{ , abstract = {The generation of intense, femtosecond-scale x-ray pulses is crucial for probing matter under extreme temporal and field conditions. Current chirped-pulse amplification (CPA) techniques in free-electron lasers (FELs), however, face efficiency limitations in the soft x-ray regime due to the inherent constraints of conventional optical compressors. To address this challenge, we propose a high-efficiency plasma-based compressor utilizing highly ionized noble gas plasma. Exploiting strong refractive index dispersion near ionic resonances, this scheme achieves over 70% transmission efficiency around 5.2 nm and is extendable to other highly charged ions for operation across the soft x-ray to vacuum ultraviolet range. Simulations demonstrate that a 25 fs FEL pulse can be compressed to 1.4 fs with peak power boosted to over 100 GW, while maintaining high-energy throughput. This transformative approach bridges the soft x-ray CPA gap and opens a scalable path toward compact, high-brightness attosecond FEL sources.}, archive = {J_PRL}, author = {Mingchang Wang and Li Zeng and Bingbing Zhang and Qinghao Zhu and Xiaozhe Shen and Xiaofan Wang and Qinming Li and Weiqing Zhang}, doi = {10.1103/d7r7-46ld}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {155001}, shortjournal = {Phys. Rev. Lett.}, title = {High-efficiency plasma-based compressor for ultrafast soft X-ray free-electron lasers}, volume = {135}, year = {2025}, }
• (2025). Droplets wicking in thin materials exhibit universal drying dynamics. PRL, 135(15), 154002. (www)

  @article{ , abstract = {When a drop contacts and absorbs in a thin porous surface, it can wick radially outward. This phenomenon is exploited in cooling textiles, but also complicates forensic stain analysis. The distance that the liquid spreads and the time it takes to evaporate are coupled, yet the consequence of this coupling on the wicking dynamics is not well understood. Here we measure and model how evaporation can reverse the direction of the liquid front so that the wetted patch shrinks after reaching a maximum diameter. We show that both this maximum diameter and the time to fully evaporate can be predicted with a single dimensionless parameter based on the substrate and liquid properties. Yet regardless of the system properties, we uncover a universal dynamic in which drops expand for approximately 1 / 4 of their lifetime and shrink for the rest. Counterintuitively, we find that neither the evaporative cooling nor the stain area scales linearly with the initial droplet volume.}, archive = {J_PRL}, author = {Garam Lee and Samira Shiri and James C. Bird}, doi = {10.1103/rx8p-st39}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {154002}, shortjournal = {Phys. Rev. Lett.}, title = {Droplets wicking in thin materials exhibit universal drying dynamics}, volume = {135}, year = {2025}, }
• (2025). Maximum dissipation reduction in bulk polymeric turbulence. PRL, 135(15), 154001. (www)

  @article{ , abstract = {We present an experimental study of the flow regime and vortex structure in bulk polymeric turbulence through three-dimensional velocity measurements with unprecedented high spatial resolution. We demonstrate that, as the polymer concentration increases, the effect of polymers on the fluid energy dissipation rate can be categorized into two distinct regimes: the dissipation reduction regime and the maximum dissipation reduction (MDR) regime, and in the latter the effect of the polymers saturates. We reveal that the MDR regime occurs when the scale range affected by the polymer additives extends up to the integral length scale, rather than the generally accepted Lumley scale. This finding enables us to map out the phase diagram of the flow regimes of polymeric turbulence on the Reynolds number and Weissenberg number. Furthermore, we demonstrate that in the MDR regime, sheetlike vortex and strain structures dominate, which is traced to the fact that polymer stress stabilizes shear layers and reduces perturbation to shear instability. These results suggest that the MDR regime is a universal flow state in bulk polymeric turbulence and is the counterpart of the maximum drag reduction regime in wall-bounded flows. Our findings emphasize the significance of sheetlike vortex structures and offer new insights into predicting the critical conditions for the emergence of various flow regimes in viscoelastic fluids.}, archive = {J_PRL}, author = {Yi-Bao Zhang and Feng Wang and Sheng-Hong Peng and Heng-Dong Xi}, doi = {10.1103/vxvs-zdbt}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {154001}, shortjournal = {Phys. Rev. Lett.}, title = {Maximum dissipation reduction in bulk polymeric turbulence}, volume = {135}, year = {2025}, }
• (2025). Multiplexed scanning microscopy with dual-qubit spin sensors. PRL, 135(15), 153801. (www)

  @article{ , abstract = {Scanning probe microscopy with multiqubit sensors offers the potential to improve imaging speed and measure previously inaccessible quantities, such as two-point correlations. We develop a multiplexed quantum sensing approach with scanning probes containing two nitrogen-vacancy (NV) centers at the tip apex. A shared optical channel is used for simultaneous qubit initialization and readout, while phase- and frequency-dependent microwave spin manipulations are leveraged for demultiplexing the optical readout signal. Scanning dual-NV magnetometry is first demonstrated by simultaneously imaging multiple field projections of a ferrimagnetic racetrack device. Then, we record the two-point covariance of spatially correlated field fluctuations across a current-carrying wire. Our multiplex framework establishes a method to investigate a variety of spatiotemporal correlations, including phase transitions and electronic noise, with nanoscale resolution.}, archive = {J_PRL}, author = {William S. Huxter and Federico Dalmagioni and Christian L. Degen}, doi = {10.1103/y14n-44h3}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153801}, shortjournal = {Phys. Rev. Lett.}, title = {Multiplexed scanning microscopy with dual-qubit spin sensors}, volume = {135}, year = {2025}, }
• (2025). Disorder-induced strongly correlated photons in waveguide QED. PRL, 135(15), 153604. (www)

  @article{ , abstract = {Strongly correlated photons play a crucial role in modern quantum technologies. Here, we investigate the probability of generating strongly correlated photons in a chain of N qubits coupled to a one-dimensional waveguide. We found that disorder in the transition frequencies can induce photon antibunching and especially nearly perfect photon blockade events in the transmission and reflection outputs. As a comparison, in ordered chains, strongly correlated photons cannot be generated in the transmission output, and only weakly antibunched photons are found in the reflection output. The occurrence of nearly perfect photon blockade events stems from the disorder-induced nearly completely destructive interference of photon scattering paths. Our Letter highlights the impact of disorder on photon correlation generation and suggests that disorder can enhance the potential for achieving strongly correlated photons.}, archive = {J_PRL}, author = {Guoqing Tian and Li-Li Zheng and Zhi-Ming Zhan and Franco Nori and Xin-You Lü}, doi = {10.1103/mldt-d59t}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153604}, shortjournal = {Phys. Rev. Lett.}, title = {Disorder-induced strongly correlated photons in waveguide QED}, volume = {135}, year = {2025}, }
• (2025). Parametric drive of a double quantum dot in a cavity. PRL, 135(15), 153603. (www)

  @article{ , abstract = {We demonstrate the parametric modulation of a double quantum dot charge dipole coupled to a cavity, at the cavity frequency, achieving an amplified readout signal compared to conventional dispersive protocols. Our findings show that the observed cavity field displacement originates from dipole radiation within the cavity, rather than from a longitudinal coupling mechanism, yet exhibits the same signatures while relying on a transverse coupling. By carefully tuning the phase and amplitude of the intracavity field, we achieve a π -phase shift between two dipole states, resulting in a substantial enhancement of the signal-to-noise ratio. In addition to its applications in quantum dot based qubits in circuit QED architectures, this protocol could serve as a new promising tool for probing exotic electronic states in mesoscopic circuits embedded in cavities.}, archive = {J_PRL}, author = {L. Jarjat and B. Hue and T. Philippe-Kagan and B. Neukelmance and J. Craquelin and A. Théry and C. Fruy and G. Abulizi and J. Becdelievre and M. M. Desjardins and T. Kontos and M. R. Delbecq}, doi = {10.1103/d8z6-x7pv}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153603}, shortjournal = {Phys. Rev. Lett.}, title = {Parametric drive of a double quantum dot in a cavity}, volume = {135}, year = {2025}, }
• (2025). Terahertz electrooptic modulation of single-photon level pulses. PRL, 135(15), 153602. (www)

  @article{ , abstract = {The manipulation of visible and near-infrared light at the single-photon level plays a key role in quantum communication systems where information is encoded into photonic degrees of freedom. In practical implementations, it is important to achieve this manipulation with high speeds, low loss, and low noise. In this Letter, we propose the use of terahertz electric fields as a pump source for electro-optic modulation of single photons in bulk media. We demonstrate spectral modulations of single photons in the form of frequency translation and bandwidth manipulations as the terahertz field imparts linear and quadratic phases on the photons at various time delays within 1 ps. Our results show frequency translations exceeding 500 GHz at multi-THz modulation speeds and loss levels of ≈ 1 dB , complementing the current state-of-the-art electro-optic modulation techniques limited to speeds up to 100 GHz. The proposed approach leverages recent developments in terahertz generation techniques, introducing new avenues to manipulate nonclassical light in an unexplored regime for quantum photonics.}, archive = {J_PRL}, author = {Nicolas Couture and Frédéric Bouchard and Alicia Sit and Guillaume Thekkadath and Duncan England and Philip J. Bustard and Benjamin J. Sussman}, doi = {10.1103/2hq3-t534}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153602}, shortjournal = {Phys. Rev. Lett.}, title = {Terahertz electrooptic modulation of single-photon level pulses}, volume = {135}, year = {2025}, }
• (2025). Universality of stationary entanglement in an optomechanical system driven by non-markovian noise and squeezed light. PRL, 135(15), 153601. (www)

  @article{ , abstract = {Optomechanical systems subjected to environmental noise give rise to rich physical phenomena. We investigate entanglement between a mechanical oscillator and the reflected coherent optical field in a general, not necessarily Markovian environment. For the input optical field, we consider stationary Gaussian states and frequency-dependent squeezing. We demonstrate that for a coherent laser drive, either unsqueezed or squeezed in a frequency-independent manner, optomechanical entanglement is destroyed after a threshold that depends only on the environmental noises—independent of the coherent coupling between the oscillator and the optical field, or the squeeze factor. In this way, we have found a universal entangling-disentangling transition. We also show that for a configuration in which the oscillator and the reflected field are separable, entanglement cannot be generated by incorporating frequency-dependent squeezing in the optical field.}, archive = {J_PRL}, author = {Su Direkci and Klemens Winkler and Corentin Gut and Markus Aspelmeyer and Yanbei Chen}, doi = {10.1103/vzhk-cdc3}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153601}, shortjournal = {Phys. Rev. Lett.}, title = {Universality of stationary entanglement in an optomechanical system driven by non-markovian noise and squeezed light}, volume = {135}, year = {2025}, }
• (2025). Emergence of a landau level structure in dark optical lattices. PRL, 135(15), 153402. (www)

  @article{ , abstract = {An optical flux lattice is a set of light beams that couple different internal states of an atom, thereby producing topological energy bands. Here we present a configuration in which the atoms exhibit a dark state, i.e., an internal state that is not coupled to the light. At large light intensity, the low-energy dynamics is restricted to the dark state, leading to an effective continuum model with a Landau-level-like structure. This structure is dramatically different from that of usual topological optical lattices, which lead to discrete models in the tight-binding limit. For well-chosen atomic species, the proposed system is essentially immune to heating due to photon scattering, making it a highly promising way to emulate the integer or fractional quantum Hall effect.}, archive = {J_PRL}, author = {Sylvain Nascimbene and Jean Dalibard}, doi = {10.1103/rmw9-8cft}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153402}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of a landau level structure in dark optical lattices}, volume = {135}, year = {2025}, }
• (2025). Self-bound superfluid membranes and monolayer crystals of ultracold polar molecules. PRL, 135(15), 153401. (www)

  @article{ , abstract = {We investigate the physics of ultracold dipolar molecules using path-integral quantum Monte Carlo simulations, and construct the complete phase diagram extending from weak to strong interactions and from small to mesoscopic particle numbers. Our calculations predict the formation of self-bound quantum droplets at interaction strengths lower than previous estimates for molecular condensates. Strikingly, we observe that, for stronger interactions, the oblate quantum droplet transitions to a two-dimensional sheet or superfluid membrane with a thickness of a single molecule. As interactions are increased further the system continually loses superfluidity while correlations develop, and is eventually found to undergo a transition to a crystalline monolayer that remains self-bound without external confinement. The spontaneous formation of such two-dimensional phases from a three-dimensional quantum gas is traced back to the peculiar anisotropic form of the dipole-dipole interaction generated by microwave dressing of rotational molecular states. For sufficiently large particle numbers, crystallization takes place for comparably low interaction strengths that do not promote two-body bound states and should thus be observable in ongoing experiments without limitations from three-body recombination.}, archive = {J_PRL}, author = {Matteo Ciardi and Kasper Rønning Pedersen and Tim Langen and Thomas Pohl}, doi = {10.1103/v7gw-xy36}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153401}, shortjournal = {Phys. Rev. Lett.}, title = {Self-bound superfluid membranes and monolayer crystals of ultracold polar molecules}, volume = {135}, year = {2025}, }
• (2025). Hydrogen molecular dissociation driven by quantum light. PRL, 135(15), 153201. (www)

  @article{ , abstract = {We investigate the dissociation dynamics of hydrogen molecular ions driven by nonclassical light by solving the time-dependent Schrödinger equation. The driving field is composed of horizontally polarized 400 nm coherent light and vertically polarized 800 nm quantum squeezed light. Our results reveal that the photon quantum fluctuations encoded in the squeezing parameter influence the kinetic energy release spectra and modulate the relative yields of competing dissociation channels. In particular, the photon-number statistics and phase uncertainty introduced by the quadrature-squeezed light can selectively enhance or suppress specific dissociation pathways. These findings highlight the potential of quantum light as a tunable resource for manipulating and probing the molecular dynamics. This Letter has implications on ultrafast chemistry with quantum light.}, archive = {J_PRL}, author = {Xiaoxiao Long and Peizeng Li and Yunquan Liu}, doi = {10.1103/4g87-d9j3}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153201}, shortjournal = {Phys. Rev. Lett.}, title = {Hydrogen molecular dissociation driven by quantum light}, volume = {135}, year = {2025}, }
• (2025). Series of molecularlike doubly excited states of a quasi-three-body coulomb system. PRL, 135(15), 153002. (www)

  @article{ , abstract = {We investigated resonant multiphoton excitation of high-angular-momentum doubly excited states of the strontium atom, a quasi-three-body Coulomb system, both experimentally and theoretically. A series of highly doubly excited states converging to the double ionization threshold was identified and reproduced by first-principles calculations, which provided access to the two-electron wave functions of the resonances. In these states, the outer electron is dynamically localized at large distances by pendulumlike oscillations of the inner electron across the nucleus. A complementary simple molecularlike adiabatic model offers a clear interpretation of the correlated two-electron motion and suggests that the series is a general feature of highly doubly excited states of atoms and molecules.}, archive = {J_PRL}, author = {M. Génévriez and M. Jungers and C. Rosen and U. Eichmann}, doi = {10.1103/svsd-9mj3}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153002}, shortjournal = {Phys. Rev. Lett.}, title = {Series of molecularlike doubly excited states of a quasi-three-body coulomb system}, volume = {135}, year = {2025}, }
• (2025). Probing dipolar interactions between rydberg atoms and ultracold polar molecules. PRL, 135(15), 153001. (www)

  @article{ , abstract = {We probe resonant dipolar interactions between ultracold molecules and Rydberg atoms in an optically trapped ensemble. Through state-selective ionization detection of the KRb molecules, we observe resonant energy transfer at 2.227 GHz from Rydberg atoms to molecules under a tunable external electric field. We measure a broadening up to 3.5 MHz, for the Rb Rydberg excitation spectrum, which matches a Monte Carlo simulation that describes a Rydberg atom and neighboring molecules evolving under a dipole-dipole interacting Hamiltonian. The demonstrated interspecies dipolar interaction is a key ingredient for hybrid Rydberg-polar molecule systems, where the advantages of each system can be leveraged and combined.}, archive = {J_PRL}, author = {Lingbang Zhu and Jeshurun Luke and Roy Shaham and Yi-Xiang Liu and Kang-Kuen Ni}, doi = {10.1103/48rk-sxfs}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {153001}, shortjournal = {Phys. Rev. Lett.}, title = {Probing dipolar interactions between rydberg atoms and ultracold polar molecules}, volume = {135}, year = {2025}, }
• (2025). Parity-doubled nucleons can rapidly cool neutron stars. PRL, 135(15), 152702. (www)

  @article{ , abstract = {In confined hadronic matter, the spontaneous breaking and restoration of chiral symmetry can be described by considering nucleons, and excited states of opposite parity, . In a cold, dense hadronic phase where chiral symmetry remains spontaneously broken, direct Urca decay processes involving the are possible, e.g., . We show that at low temperature and moderate densities, because the are much heavier than the , such cooling dominates over standard direct Urca processes. This provides a strong astrophysical signature of the pattern of chiral symmetry restoration in neutron stars.}, archive = {J_PRL}, author = {Liam Brodie and Robert D. Pisarski}, doi = {10.1103/bf66-1hr5}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {152702}, shortjournal = {Phys. Rev. Lett.}, title = {Parity-doubled nucleons can rapidly cool neutron stars}, volume = {135}, year = {2025}, }
• (2025). Precision mass measurements around mo84 rule out ZrNb cycle formation in the rapid proton-capture process at type i X-ray bursts. PRL, 135(15), 152701. (www)

  @article{ , abstract = {The rapid proton-capture process is one of the primary, explosive thermonuclear burning processes that drive type I x-ray bursts. A possible termination of the rapid proton-capture process at around Mo 84 was previously suggested by the formation of a ZrNb cycle. We report here precision mass measurements at around Mo 84 that conclude the issue regarding the possibility of the cycle. The experiment was conducted using the multireflection time-of-flight spectrograph at RIKEN Radioactive Isotope Beam Factory, and the masses of Y 79 , Nb 83 , Mo 84 , Ru 88 , and an isomer in Y 78 were measured. For Mo 84 , Ru 88 , and the isomeric state of Y 78 , their masses were experimentally determined for the first time with uncertainties of δ m ≈ 20 keV / c 2 . The mass precisions of Y 79 and Nb 83 were improved to 13 and 9.6 keV / c 2 , respectively. The new α -separation energy of Mo 84 , 1.434(83) MeV, unambiguously rules out the possibility of forming the ZrNb cycle. The x-ray burst simulation with the new masses shows that our measurements effectively remove the large final abundance uncertainties in the A = 80 – 90 mass region. The new mass values improve the prediction power for the composition of the nuclear ashes in x-ray bursts.}, archive = {J_PRL}, author = {S. Kimura and M. Wada and C. Y. Fu and N. Fukuda and Y. Hirayama and D. S. Hou and S. Iimura and H. Ishiyama and Y. Ito and S. Kubono and K. Kusaka and S. Michimasa and H. Miyatake and S. Nishimura and T. Niwase and V. Phong and M. Rosenbusch and H. Schatz and P. Schury and Y. Shimizu and H. Suzuki and A. Takamine and H. Takeda and Y. Togano and Y. X. Watanabe and W. D. Xian and Y. Yanagisawa and T. T. Yeung and M. Yoshimoto and S. Zha}, doi = {10.1103/2dyn-q7wp}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {152701}, shortjournal = {Phys. Rev. Lett.}, title = {Precision mass measurements around mo84 rule out ZrNb cycle formation in the rapid proton-capture process at type i X-ray bursts}, volume = {135}, year = {2025}, }
• (2025). Ab initio study of the radii of oxygen isotopes. PRL, 135(15), 152502. (www)

  @article{ , abstract = {We present an ab initio study of the charge and matter radii of oxygen isotopes from O 16 to O 20 using nuclear lattice effective field theory (NLEFT) with high-fidelity N 3 LO chiral interactions. To efficiently address the Monte Carlo sign problem encountered in nuclear radius calculations, we introduce the partial pinhole algorithm , significantly reducing statistical uncertainties and extending the reach to more neutron-rich and proton-rich isotopes. Our computed charge radii for O 16 , O 17 , and O 18 closely match experimental data, and we predict a charge radius of 2.810(32) fm for O 20 . The calculated matter radii show excellent agreement with values extracted from low-energy proton and electron elastic scattering data, but are inconsistent with those derived from interaction cross sections and charge-changing cross section measurements. These discrepancies highlight model-dependent ambiguities in the experimental extraction methods of matter radii and underscore the value of precise theoretical benchmarks from NLEFT calculations.}, archive = {J_PRL}, author = {Zhengxue Ren and Serdar Elhatisari and Ulf-G. Meißner}, doi = {10.1103/y6s2-43ym}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {152502}, shortjournal = {Phys. Rev. Lett.}, title = {Ab initio study of the radii of oxygen isotopes}, volume = {135}, year = {2025}, }
• (2025). First β-delayed two-neutron spectroscopy of the r-process nucleus in134 and observation of the i13/2 single-particle neutron state in sn133. PRL, 135(15), 152501. (www)

  @article{ , abstract = {This manuscript reports on the direct observation of a β -delayed two-neutron emission in a study of In 134 at the ISOLDE Decay Station using neutron spectroscopy. We also report on the first measurement in β − decay of the long-sought 13 / 2 + excited state in Sn 133 , attributed to be the neutron single-particle i 13 / 2 orbital. The observation of sequential neutron emission is used to extract the relative population of the i 13 / 2 state, which was found to be much smaller than the predictions of the statistical model. The experiment was possible because of the innovative use of a neutron array with neutron discrimination and interaction tracking capabilities. This is the first study of the details of the two-neutron emission for a nucleus, which belongs to the r -process path. Understanding β -delayed two-neutron emission probabilities is essential to validate models used in astrophysical r -process nucleosynthesis calculations. Observing two-neutron emissions in β − decay paves the way for new experiments to study energy and angular correlations for β -delayed multineutron emitters.}, archive = {J_PRL}, author = {IDS Collaboration and P. Dyszel and R. Grzywacz and Z. Y. Xu and N. Kitamura and M. Karny and A. Korgul and M. Madurga and S. Neupane and A. Algora and A. N. Andreyev and M. Araszkiewicz and R. A. Bark and J. Benito and N. Bernier and M. J. G. Borge and M. Caballero and P. Chuchala and T. E. Cocolios and C. Costache and J. G. Cubiss and H. DeWitte and J. E. Escher and D. Fernandez-Ruiz and A. Fijalkowska and L. M. Fraile and H. O. U. Fynbo and J. Gouge and J. L. Herraiz and A. Illana and P. M. Jones and D. S. Judson and P. Kamińska and T. Kawano and K. Kolos and M. Labiche and R. Lică and M. Llanos-Expósito and G. G. DeLorenzo and N. Marginean and I. Michelon and C. Mihai and E. Nácher and C. Neacsu and J. S. Nielsen and B. Olaizola and J. N. Orce and C. A. A. Page and R. D. Page and J. Pakarinen and A. Perea and M. Piersa-Siłkowska and Zs. Podolyák and J. S. Prieto and M. Rajabali and J. Shaw and A. I. Sison and K. Solak and M. Stryjczyk and O. Tengblad and P. G. T. Vicente and N. Warr and J. Wilson and Z. Yue and S. Zajda}, doi = {10.1103/l24v-5m31}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {152501}, shortjournal = {Phys. Rev. Lett.}, title = {First β-delayed two-neutron spectroscopy of the r-process nucleus in134 and observation of the i13/2 single-particle neutron state in sn133}, volume = {135}, year = {2025}, }
• (2025). New measurements of the deuteron-to-proton f2 structure-function ratio. PRL, 135(15), 151902. (www)

  @article{ , abstract = {Nucleon structure functions, as measured in lepton-nucleon scattering, have historically provided a critical observable in the study of partonic dynamics within the nucleon. However, at very large parton momenta, it is both experimentally and theoretically challenging to extract parton distributions due to the probable onset of nonperturbative contributions and the unavailability of high-precision data at critical kinematics. Extraction of the neutron structure and the d quark distribution have been further challenging because of the necessity of applying nuclear corrections when utilizing scattering data from a deuteron target to extract the free neutron structure. However, a program of experiments has been carried out recently at the energy-upgraded Jefferson Lab electron accelerator aimed at significantly reducing the nuclear correction uncertainties on the d quark distribution function at large partonic momentum. This allows leveraging the vast body of deuterium data covering a large kinematic range to be utilized for d quark parton distribution function extraction. In this Letter, we present new data from experiment E12-10-002, carried out in Jefferson Lab Experimental Hall C, on the deuteron to proton cross section ratio at large Bjorken x . These results significantly improve the precision of existing data and provide a first look at the expected impact on quark distributions extracted from parton distribution function fits.}, archive = {J_PRL}, author = {Hall C Collaboration and D. Biswas and F. A. Gonzalez and W. Henry and A. Karki and C. Morean and A. Nadeeshani and A. Sun and Z. Ahmed and S. Alsalmi and W. Armstrong and A. Asaturyan and C. Ayerbe Gayoso and V. Berdnikov and H. Bhatt and D. Bhetuwal and P. Bosted and E. Brash and M. H. S. Bukhari and J. P. Chen and M. Chen and M. E. Christy and S. Covrig Dusa and K. Craycraft and S. Danagoulian and D. Day and M. Diefenthaler and M. Dlamini and J. Dunne and B. Duran and D. Dutta and R. Ent and H. Fenker and N. Fomin and E. Fuchey and D. Gaskell and T. N. Gautam and J. O. Hansen and F. Hauenstein and A. V. Hernandez and T. Horn and G. M. Huber and M. K. Jones and S. Joosten and M. L. Kabir and C. Keppel and A. Khanal and P. M. King and E. Kinney and M. Kohl and N. Lashley-Colthirst and S. Li and W. B. Li and A. H. Liyanage and D. Mack and S. Malace and P. Markowitz and J. Matter and D. Meekins and R. Michaels and A. Mkrtchyan and H. Mkrtchyan and Z. Moore and S. J. Nazeer and S. Nanda and G. Niculescu and I. Niculescu and D. Nguyen and Nuruzzaman and B. Pandey and S. Park and E. Pooser and A. J. R. Puckett and M. Rehfuss and J. Reinhold and B. Sawatzky and G. R. Smith and H. Szumila-Vance and A. S. Tadepalli and V. Tadevosyan and R. Trotta and S. A. Wood and C. Yero and J. Zhang}, doi = {10.1103/1xx8-rxlv}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151902}, shortjournal = {Phys. Rev. Lett.}, title = {New measurements of the deuteron-to-proton f2 structure-function ratio}, volume = {135}, year = {2025}, }
• (2025). Single inclusive π± and k± production in e+e− annihilation at center-of-mass energies from 2.000 to 3.671 GeV. PRL, 135(15), 151901. (www)

  @article{ , abstract = {Using data samples with a total integrated luminosity of collected by the BESIII detector operating at the BEPCII collider, the differential cross sections of inclusive and production, as a function of the momentum and normalized by the total hadronic cross section, are measured at center-of-mass energies from 2.000 to 3.671 GeV. The measured cross sections are consistent with the previously reported cross sections by BESIII, while the cross sections are systematically higher than the cross sections by a factor of approximately 1.4. These new results are in agreement with state-of-the-art QCD analyses at next-to-next-to-leading-order accuracy, particularly in the large hadron momentum region at energy scales down to 3 GeV. These findings support the validity of isospin symmetry in parton fragmentation processes.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and J. Gao and X. B. Gao and Y. Gao and Y. N. Gao and Y. Y. Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Q. A. Malik and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. M. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. J. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and H. X. Xing and T. Y Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and L. Q. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Y. P. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/5kxw-3mbw}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151901}, shortjournal = {Phys. Rev. Lett.}, title = {Single inclusive π± and k± production in e+e− annihilation at center-of-mass energies from 2.000 to 3.671 GeV}, volume = {135}, year = {2025}, }
• (2025). Search for sub-GeV invisible particles in inclusive decays of j/ψ to ϕ. PRL, 135(15), 151804. (www)

  @article{ , abstract = {A search for an invisible particle, with a mass between 0 and , is performed in the process using events collected with the BESIII detector from 2017 to 2019. The meson is fully reconstructed and an efficient veto of photons and neutral and charged hadrons up to twice the mass is applied to the rest of the event and the recoil mass against the is obtained precisely from the kinematic constraint in the event. No significant signal over the expected background is observed in the investigated region and the upper limit on the inclusive branch fraction of is determined to be at 90% confidence level. Upper limits at a 90% confidence level are also given for this branch fraction as a function of the invisible particle mass, varying from to over the investigated mass range. Additionally, a 90% confidence level upper limit on the branch fraction of is determined to , which improves the previous best results by more than 4 times. The analysis technique in this Letter offers a clean window to search for sub-GeV invisible particles, which can be adapted for other decays and direct annihilation experiments in future studies, and improve the sensitivity by orders of magnitude.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. Gao and Y. N. Gao and Y. Y. Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Q. A. Malik and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. J. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and L. Q. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Y. P. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/qx34-yy4b}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151804}, shortjournal = {Phys. Rev. Lett.}, title = {Search for sub-GeV invisible particles in inclusive decays of j/ψ to ϕ}, volume = {135}, year = {2025}, }
• (2025). Search for the rare decay d0→μ+μ− in proton-proton collisions at s=13.6 TeV. PRL, 135(15), 151803. (www)

  @article{ , abstract = {A search for the rare decay is reported using proton-proton collision events at collected by the CMS detector in 2022–2023, corresponding to an integrated luminosity of . This is the first analysis to use a newly developed inclusive dimuon trigger, expanding the scope of the CMS flavor physics program. The search uses mesons obtained from decays. No significant excess is observed. A limit on the branching fraction of at 95% confidence level is set. This is the most stringent upper limit set on any flavor changing neutral current decay in the charm sector.}, archive = {J_PRL}, author = {CMS Collaboration and V. Chekhovsky and A. Hayrapetyan and V. Makarenko and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and H. Kwon and T. Van Laer and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and Y. Hong and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and A. Khalilzadeh and F. A. Khan and A. Malara and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and J. Knolle and L. Lambrecht and D. Marckx and K. Skovpen and N. Van Den Bossche and J. van der Linden and J. Vandenbroeck and L. Wezenbeek and S. Bein and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and S. Turkcapar and G. A. Alves and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and E. J. Tonelli Manganote and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and T. Laux Kuhn and M. Macedo and K. Mota Amarilo and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and V. Scheurer and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and D. Laroze and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and H. Wang and K. Yi and J. Zhang and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and J. Jaramillo and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and B. El-mahdy and S. Khalil and E. Salama and M. Abdullah Al-Mashad and M. A. Mahmoud and K. Ehataht and M. Kadastik and T. Lange and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and K. Osterberg and M. Voutilainen and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Myllymäki and M. m. Rantanen and J. Tuominiemi and H. Kirschenmann and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and A. Cappati and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Manoni and M. Nguyen and S. Obraztsov and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and G. Sokmen and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and D. Chokheli and I. Lomidze and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and N. Kumar and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and A. Cardini and F. Colombina and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and S. Zakharov and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and Y. M. Chen and T. Chwalek and A. Dierlamm and G. G. Dincer and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and O. Lavoryk and J. M. Lawhorn and M. Link and A. Lintuluoto and S. Maier and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and R. Schmieder and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and B. Topko and N. Trevisani and T. Voigtländer and R. F. Von Cube and J. Von Den Driesch and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and G. Melachroinos and Z. Painesis and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Mukherjee and S. Baradia and S. Barman and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and T. Mishra and B. Parida and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and S. Bhowmik and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and B. M. Joshi and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and K. Naskar and A. Nayak and S. Nayak and K. Pal and R. Raturi and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and P. Assiouras and G. Barbagli and G. Bardelli and M. Bartolini and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and L. Damenti and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and G. Lavizzari and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and P. Bortignon and G. Bortolato and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and S. Fantinel and F. Gasparini and U. Gasparini and S. Giorgetti and E. Lusiani and M. Margoni and A. T. Meneguzzo and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and M. Pelliccioni and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and F. Cattafesta and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and V. K. Muraleedharan Nair Bindhu and M. Musich and S. Nandan and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and F. Tenchini and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and P. Barria and C. Basile and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and R. Gargiulo and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and G. Mazza and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Ruspa and F. Siviero and V. Sola and A. Solano and C. Tarricone and D. Trocino and G. Umoret and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. Lee and K. S. Lee and S. Lee and J. Yoo and J. Goh and Y. Kang and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and K. Hwang and B. Kim and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and F. E. Neri Huerta and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and A. Bellora and L. Forthomme and L. Grzanka and M. Malawski and K. Piotrzkowski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and M. Stojanovic and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and C. Martin Perez and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and E. Palencia Cortezon and J. Prado Pico and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and A. A. Bin Anuar and A. Bocci and L. Borgonovi and C. Botta and A. Bragagnolo and E. Brondolin and C. E. Brown and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and M. Glowacki and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and G. Karathanasis and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and M. Magherini and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and M. Migliorini and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and M. Pitt and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and W. H. Huang and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and Y. Maghrbi and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and Y. Komurcu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and E. Uslan and I. S. Zorbakir and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and V. J. Smith and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and O. Buchmuller and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and L. Russell and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and V. Hegde and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and S. Ellis and L. Gouskos and M. Hadley and U. Heintz and K. W. Ho and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and J. Luo and S. Mondal and T. Russell and S. Sagir and X. Shen and M. Stamenkovic and N. Venkatasubramanian and S. Abbott and B. Barton and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and S. Yoo and F. Zhang and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and D. Primosch and M. Quinnan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and M. M. Hussain and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and X. Yan and D. Zhang and A. Albert and A. Bornheim and O. Cerri and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and M. Kanemura and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and N. Manganelli and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and X. Chen and D. J. Cranshaw and J. Dickinson and J. Fan and X. Fan and J. Grassi and S. Hogan and P. Kotamnives and J. Monroy and G. Niendorf and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and C. Cosby and G. Cummings and I. Dutta and V. D. Elvira and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and K. Maeshima and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and H. Gupta and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and P. Roy and T. Roy and S. Rudrabhatla and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and S. Popescu and C. Rogan and C. Royon and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and S. Lascio and P. Major and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Wang and L. Zhang and C. Baldenegro Barrera and J. Bendavid and S. Bright-Thonney and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and A. Rohilla and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and P. Levchenko and J. Li and M. Lu and R. Mccarthy and D. M. Morse and T. Orimoto and A. Parker and L. Skinnari and E. Tsai and D. Wood and S. Dittmer and K. A. Hahn and D. Li and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and P. Fackeldey and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and Y. Lai and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and F. Simpson and D. Stickland and C. Tully and L. H. Vage and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and J. F. Schulte and A. K. Virdi and F. Wang and A. Wildridge and W. Xie and Y. Yao and J. Dolen and N. Parashar and A. Pathak and D. Acosta and A. Agrawal and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and I. Krommydas and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and J. Martins and R. Montalvo and K. Nash and J. Reichert and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and A. Safonov and N. Akchurin and J. Damgov and Y. Feng and N. Gogate and Y. Kazhykarim and K. Lamichhane and C. Madrid and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and D. Rathjens and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Mantilla and C. Neu and C. Ramón Álvarez and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and Yu. Andreev and T. Aushev and D. Budkouski and A. Ershov and I. Golutvin and I. Gorbunov and V. Karjavine and V. Klyukhin and O. Kodolova and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and A. Nikitenko and V. Palichik and V. Perelygin and S. Petrushanko and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and Y. Skovpen and V. Smirnov and O. Teryaev and I. Tlisova and A. Toropin and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and K. Ivanov and V. Gavrilov and N. Lychkovskaya and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and V. Bunichev and M. Dubinin and L. Dudko and A. Gribushin and V. Savrin and A. Snigirev and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and V. Kachanov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin}, doi = {10.1103/zc76-rgcp}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151803}, shortjournal = {Phys. Rev. Lett.}, title = {Search for the rare decay d0→μ+μ− in proton-proton collisions at s=13.6 TeV}, volume = {135}, year = {2025}, }
• (2025). First measurement of the electron-neutrino charged-current pion production cross section on carbon with the T2K near detector. PRL, 135(15), 151802. (www)

  @article{ , abstract = {The T2K Collaboration presents the first measurement of electron neutrino-induced charged-current pion production on a predominantly carbon target in a restricted kinematical phase space. This is performed using data from the 2.5° off-axis near detector, ND280. The differential cross sections with respect to the outgoing electron and pion kinematics, in addition to the total flux-integrated cross section, are obtained. Comparisons between the measured and predicted cross-section results using the n eut, g enie, and n u w ro Monte Carlo event generators are presented. The measured total flux-integrated cross section is [ 2.52 ± 0.52 ( stat ) ± 0.30 ( syst ) ] × 10 − 39 cm 2 nucleon − 1 , which is lower than the event generator predictions.}, archive = {J_PRL}, author = {T2K Collaboration and K. Abe and S. Abe and R. Akutsu and H. Alarakia-Charles and Y. I. Alj Hakim and S. Alonso Monsalve and L. Anthony and S. Aoki and K. A. Apte and T. Arai and T. Arihara and S. Arimoto and Y. Ashida and E. T. Atkin and N. Babu and V. Baranov and G. J. Barker and G. Barr and D. Barrow and P. Bates and L. Bathe-Peters and M. Batkiewicz-Kwasniak and N. Baudis and V. Berardi and L. Berns and S. Bhattacharjee and A. Blanchet and A. Blondel and P. M. M. Boistier and S. Bolognesi and S. Bordoni and S. B. Boyd and C. Bronner and A. Bubak and M. Buizza Avanzini and J. A. Caballero and F. Cadoux and N. F. Calabria and S. Cao and S. Cap and D. Carabadjac and S. L. Cartwright and M. P. Casado and M. G. Catanesi and J. Chakrani and A. Chalumeau and D. Cherdack and A. Chvirova and J. Coleman and G. Collazuol and F. Cormier and A. A. L. Craplet and A. Cudd and D. D’ago and C. Dalmazzone and T. Daret and P. Dasgupta and C. Davis and Yu. I. Davydov and P. de Perio and G. De Rosa and T. Dealtry and C. Densham and A. Dergacheva and R. Dharmapal Banerjee and F. Di Lodovico and G. Diaz Lopez and S. Dolan and D. Douqa and T. A. Doyle and O. Drapier and K. E. Duffy and J. Dumarchez and P. Dunne and K. Dygnarowicz and A. Eguchi and J. Elias and S. Emery-Schrenk and G. Erofeev and A. Ershova and G. Eurin and D. Fedorova and S. Fedotov and M. Feltre and L. Feng and D. Ferlewicz and A. J. Finch and M. D. Fitton and C. Forza and M. Friend and Y. Fujii and Y. Fukuda and Y. Furui and J. García-Marcos and A. C. Germer and L. Giannessi and C. Giganti and M. Girgus and V. Glagolev and M. Gonin and R. González Jiménez and J. González Rosa and E. A. G. Goodman and K. Gorshanov and P. Govindaraj and M. Grassi and M. Guigue and F. Y. Guo and D. R. Hadley and S. Han and D. A. Harris and R. J. Harris and T. Hasegawa and C. M. Hasnip and S. Hassani and N. C. Hastings and Y. Hayato and I. Heitkamp and D. Henaff and Y. Hino and J. Holeczek and A. Holin and T. Holvey and N. T. Hong Van and T. Honjo and M. C. F. Hooft and K. Hosokawa and J. Hu and A. K. Ichikawa and K. Ieki and M. Ikeda and T. Ishida and M. Ishitsuka and H. Ito and S. Ito and A. Izmaylov and N. Jachowicz and S. J. Jenkins and C. Jesús-Valls and M. Jia and J. J. Jiang and J. Y. Ji and T. P. Jones and P. Jonsson and S. Joshi and M. Kabirnezhad and A. C. Kaboth and H. Kakuno and J. Kameda and S. Karpova and V. S. Kasturi and Y. Kataoka and T. Katori and A. Kawabata and Y. Kawamura and M. Kawaue and E. Kearns and M. Khabibullin and A. Khotjantsev and T. Kikawa and S. King and V. Kiseeva and J. Kisiel and A. Klustová and L. Kneale and H. Kobayashi and L. Koch and S. Kodama and M. Kolupanova and A. Konaka and L. L. Kormos and Y. Koshio and K. Kowalik and Y. Kudenko and Y. Kudo and A. Kumar Jha and R. Kurjata and V. Kurochka and T. Kutter and L. Labarga and M. Lachat and K. Lachner and J. Lagoda and S. M. Lakshmi and M. Lamers James and A. Langella and D. H. Langridge and J.-F. Laporte and D. Last and N. Latham and M. Laveder and L. Lavitola and M. Lawe and D. Leon Silverio and S. Levorato and S. V. Lewis and B. Li and C. Lin and R. P. Litchfield and S. L. Liu and W. Li and A. Longhin and A. Lopez Moreno and L. Ludovici and X. Lu and T. Lux and L. N. Machado and L. Magaletti and K. Mahn and K. K. Mahtani and S. Manly and A. D. Marino and D. G. R. Martin and D. A. Martinez Caicedo and L. Martinez and M. Martini and T. Matsubara and R. Matsumoto and V. Matveev and C. Mauger and K. Mavrokoridis and N. McCauley and K. S. McFarland and C. McGrew and J. McKean and A. Mefodiev and G. D. Megias and L. Mellet and C. Metelko and M. Mezzetto and S. Miki and V. Mikola and E. W. Miller and A. Minamino and O. Mineev and S. Mine and J. Mirabito and M. Miura and S. Moriyama and P. Morrison and Th. A. Mueller and D. Munford and A. Muñoz and L. Munteanu and Y. Nagai and T. Nakadaira and K. Nakagiri and M. Nakahata and Y. Nakajima and K. D. Nakamura and A. Nakano and Y. Nakano and S. Nakayama and T. Nakaya and K. Nakayoshi and C. E. R. Naseby and D. T. Nguyen and V. Q. Nguyen and K. Niewczas and S. Nishimori and Y. Nishimura and Y. Noguchi and T. Nosek and F. Nova and J. C. Nugent and H. M. O’Keeffe and L. O’Sullivan and R. Okazaki and W. Okinaga and K. Okumura and T. Okusawa and N. Onda and N. Ospina and L. Osu and N. Otani and Y. Oyama and V. Paolone and J. Pasternak and D. Payne and M. Pfaff and L. Pickering and B. Popov and A. J. Portocarrero Yrey and M. Posiadala-Zezula and Y. S. Prabhu and H. Prasad and F. Pupilli and B. Quilain and P. T. Quyen and E. Radicioni and B. Radics and M. A. Ramirez and R. Ramsden and P. N. Ratoff and M. Reh and G. Reina and C. Riccio and D. W. Riley and E. Rondio and S. Roth and N. Roy and A. Rubbia and L. Russo and A. Rychter and W. Saenz and K. Sakashita and S. Samani and F. Sánchez and E. M. Sandford and Y. Sato and T. Schefke and K. Scholberg and M. Scott and Y. Seiya and T. Sekiguchi and H. Sekiya and T. Sekiya and D. Seppala and D. Sgalaberna and A. Shaikhiev and M. Shiozawa and Y. Shiraishi and A. Shvartsman and N. Skrobova and K. Skwarczynski and D. Smyczek and M. Smy and J. T. Sobczyk and H. Sobel and F. J. P. Soler and A. J. Speers and R. Spina and A. Srivastava and P. Stowell and Y. Stroke and I. A. Suslov and A. Suzuki and S. Y. Suzuki and M. Tada and S. Tairafune and A. Takeda and Y. Takeuchi and K. Takeya and H. K. Tanaka and H. Tanigawa and V. V. Tereshchenko and N. Thamm and C. Touramanis and N. Tran and T. Tsukamoto and M. Tzanov and Y. Uchida and M. Vagins and S. Valder and M. Varghese and I. Vasilyev and G. Vasseur and E. Villa and U. Virginet and T. Vladisavljevic and T. Wachala and S.-i. Wada and D. Wakabayashi and H. T. Wallace and J. G. Walsh and D. Wark and M. O. Wascko and A. Weber and R. Wendell and M. J. Wilking and C. Wilkinson and J. R. Wilson and K. Wood and C. Wret and J. Xia and K. Yamamoto and T. Yamamoto and C. Yanagisawa and Y. Yang and T. Yano and N. Yershov and U. Yevarouskaya and M. Yokoyama and Y. Yoshimoto and N. Yoshimura and R. Zaki and A. Zalewska and J. Zalipska and G. Zarnecki and J. Zhang and X. Y. Zhao and H. Zheng and H. Zhong and T. Zhu and M. Ziembicki and E. D. Zimmerman and M. Zito and S. Zsoldos}, doi = {10.1103/klhv-7t6h}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151802}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of the electron-neutrino charged-current pion production cross section on carbon with the T2K near detector}, volume = {135}, year = {2025}, }
• (2025). Search for B0→K*0τ+τ− decays at the belle II experiment. PRL, 135(15), 151801. (www)

  @article{ , abstract = {We present a search for the rare flavor-changing neutral-current decay with data collected by the Belle II experiment at the SuperKEKB electron-positron collider. The analysis uses a data sample recorded at the center-of-mass energy of the resonance. One of the mesons produced in the process is fully reconstructed in a hadronic decay mode, while its companion meson is required to decay into a and two leptons of opposite charge. The leptons are reconstructed in final states with a single electron, muon, charged pion or charged meson, and additional neutrinos. We set an upper limit on the branching fraction of at the 90% confidence level, which is the most stringent constraint reported to date.}, archive = {J_PRL}, author = {Belle II Collaboration and I. Adachi and K. Adamczyk and L. Aggarwal and H. Ahmed and H. Aihara and N. Akopov and M. Alhakami and A. Aloisio and N. Althubiti and M. Angelsmark and N. Anh Ky and D. M. Asner and H. Atmacan and V. Aushev and M. Aversano and R. Ayad and V. Babu and H. Bae and N. K. Baghel and S. Bahinipati and P. Bambade and Sw. Banerjee and S. Bansal and M. Barrett and M. Bartl and J. Baudot and A. Baur and A. Beaubien and F. Becherer and J. Becker and J. V. Bennett and F. U. Bernlochner and V. Bertacchi and M. Bertemes and E. Bertholet and M. Bessner and S. Bettarini and V. Bhardwaj and B. Bhuyan and F. Bianchi and T. Bilka and D. Biswas and A. Bobrov and D. Bodrov and A. Bolz and A. Bondar and A. Boschetti and A. Bozek and M. Bračko and P. Branchini and N. Brenny and R. A. Briere and T. E. Browder and A. Budano and S. Bussino and Q. Campagna and M. Campajola and L. Cao and G. Casarosa and C. Cecchi and J. Cerasoli and M.-C. Chang and P. Chang and R. Cheaib and P. Cheema and B. G. Cheon and K. Chilikin and J. Chin and K. Chirapatpimol and H.-E. Cho and K. Cho and S.-J. Cho and S.-K. Choi and S. Choudhury and J. Cochran and I. Consigny and L. Corona and J. X. Cui and E. De La Cruz-Burelo and S. A. De La Motte and G. de Marino and G. De Nardo and G. De Pietro and R. de Sangro and M. Destefanis and S. Dey and R. Dhamija and A. Di Canto and F. Di Capua and J. Dingfelder and Z. Doležal and I. Domínguez Jiménez and T. V. Dong and M. Dorigo and D. Dossett and S. Dubey and K. Dugic and G. Dujany and P. Ecker and D. Epifanov and J. Eppelt and P. Feichtinger and T. Ferber and T. Fillinger and C. Finck and G. Finocchiaro and A. Fodor and F. Forti and B. G. Fulsom and A. Gabrielli and E. Ganiev and M. Garcia-Hernandez and R. Garg and G. Gaudino and V. Gaur and V. Gautam and A. Gaz and A. Gellrich and G. Ghevondyan and D. Ghosh and H. Ghumaryan and G. Giakoustidis and R. Giordano and A. Giri and P. Gironella Gironell and A. Glazov and B. Gobbo and R. Godang and O. Gogota and P. Goldenzweig and W. Gradl and S. Granderath and E. Graziani and D. Greenwald and Z. Gruberová and Y. Guan and K. Gudkova and I. Haide and Y. Han and T. Hara and C. Harris and K. Hayasaka and H. Hayashii and S. Hazra and C. Hearty and M. T. Hedges and A. Heidelbach and I. Heredia de la Cruz and M. Hernández Villanueva and T. Higuchi and M. Hoek and M. Hohmann and R. Hoppe and P. Horak and C.-L. Hsu and T. Humair and T. Iijima and K. Inami and G. Inguglia and N. Ipsita and A. Ishikawa and R. Itoh and M. Iwasaki and P. Jackson and D. Jacobi and W. W. Jacobs and D. E. Jaffe and E.-J. Jang and Q. P. Ji and S. Jia and Y. Jin and A. Johnson and K. K. Joo and H. Junkerkalefeld and D. Kalita and A. B. Kaliyar and J. Kandra and K. H. Kang and S. Kang and G. Karyan and T. Kawasaki and F. Keil and C. Ketter and C. Kiesling and C.-H. Kim and D. Y. Kim and J.-Y. Kim and K.-H. Kim and Y.-K. Kim and H. Kindo and K. Kinoshita and P. Kodyš and T. Koga and S. Kohani and K. Kojima and A. Korobov and S. Korpar and E. Kovalenko and R. Kowalewski and P. Križan and P. Krokovny and T. Kuhr and Y. Kulii and D. Kumar and J. Kumar and R. Kumar and K. Kumara and T. Kunigo and A. Kuzmin and Y.-J. Kwon and S. Lacaprara and Y.-T. Lai and K. Lalwani and T. Lam and J. S. Lange and T. S. Lau and M. Laurenza and R. Leboucher and F. R. Le Diberder and M. J. Lee and C. Lemettais and P. Leo and P. M. Lewis and C. Li and L. K. Li and Q. M. Li and W. Z. Li and Y. Li and Y. B. Li and Y. P. Liao and J. Libby and J. Lin and S. Lin and M. H. Liu and Q. Y. Liu and Y. Liu and Z. Q. Liu and D. Liventsev and S. Longo and T. Lueck and C. Lyu and Y. Ma and C. Madaan and M. Maggiora and S. P. Maharana and R. Maiti and G. Mancinelli and R. Manfredi and E. Manoni and M. Mantovano and D. Marcantonio and S. Marcello and C. Marinas and C. Martellini and A. Martens and A. Martini and T. Martinov and L. Massaccesi and M. Masuda and K. Matsuoka and D. Matvienko and S. K. Maurya and M. Maushart and J. A. McKenna and R. Mehta and F. Meier and D. Meleshko and M. Merola and C. Miller and M. Mirra and S. Mitra and K. Miyabayashi and H. Miyake and R. Mizuk and G. B. Mohanty and S. Mondal and S. Moneta and H.-G. Moser and I. Nakamura and K. R. Nakamura and M. Nakao and H. Nakazawa and Y. Nakazawa and M. Naruki and Z. Natkaniec and A. Natochii and M. Nayak and G. Nazaryan and M. Neu and S. Nishida and S. Ogawa and R. Okubo and H. Ono and Y. Onuki and F. Otani and P. Pakhlov and G. Pakhlova and E. Paoloni and S. Pardi and K. Parham and H. Park and J. Park and K. Park and S.-H. Park and B. Paschen and A. Passeri and S. Patra and T. K. Pedlar and I. Peruzzi and R. Peschke and R. Pestotnik and M. Piccolo and L. E. Piilonen and P. L. M. Podesta-Lerma and T. Podobnik and S. Pokharel and A. Prakash and C. Praz and S. Prell and E. Prencipe and M. T. Prim and S. Privalov and I. Prudiiev and H. Purwar and P. Rados and G. Raeuber and S. Raiz and N. Rauls and K. Ravindran and J. U. Rehman and M. Reif and S. Reiter and M. Remnev and L. Reuter and D. Ricalde Herrmann and I. Ripp-Baudot and G. Rizzo and S. H. Robertson and M. Roehrken and J. M. Roney and A. Rostomyan and N. Rout and D. A. Sanders and S. Sandilya and L. Santelj and V. Savinov and B. Scavino and J. Schmitz and S. Schneider and M. Schnepf and C. Schwanda and Y. Seino and A. Selce and K. Senyo and J. Serrano and M. E. Sevior and C. Sfienti and W. Shan and C. Sharma and G. Sharma and X. D. Shi and T. Shillington and T. Shimasaki and J.-G. Shiu and D. Shtol and B. Shwartz and A. Sibidanov and F. Simon and J. B. Singh and J. Skorupa and R. J. Sobie and M. Sobotzik and A. Soffer and A. Sokolov and E. Solovieva and W. Song and S. Spataro and B. Spruck and M. Starič and P. Stavroulakis and S. Stefkova and R. Stroili and J. Strube and Y. Sue and M. Sumihama and K. Sumisawa and W. Sutcliffe and N. Suwonjandee and H. Svidras and M. Takahashi and M. Takizawa and U. Tamponi and K. Tanida and F. Tenchini and A. Thaller and O. Tittel and R. Tiwary and E. Torassa and K. Trabelsi and I. Tsaklidis and I. Ueda and T. Uglov and K. Unger and Y. Unno and K. Uno and S. Uno and P. Urquijo and Y. Ushiroda and S. E. Vahsen and R. van Tonder and K. E. Varvell and M. Veronesi and A. Vinokurova and V. S. Vismaya and L. Vitale and V. Vobbilisetti and R. Volpe and A. Vossen and M. Wakai and S. Wallner and M.-Z. Wang and X. L. Wang and Z. Wang and A. Warburton and M. Watanabe and S. Watanuki and C. Wessel and E. Won and X. P. Xu and B. D. Yabsley and S. Yamada and W. Yan and W. C. Yan and J. Yelton and J. H. Yin and K. Yoshihara and C. Z. Yuan and J. Yuan and Y. Yusa and L. Zani and F. Zeng and M. Zeyrek and B. Zhang and J. S. Zhou and Q. D. Zhou and L. Zhu and V. I. Zhukova and R. Žlebčík}, doi = {10.1103/v1q3-9dy8}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for B0→K*0τ+τ− decays at the belle II experiment}, volume = {135}, year = {2025}, }
• (2025). Nonlocal symmetries of planar feynman integrals. PRL, 135(15), 151603. (www)

  @article{ , abstract = {We prove the invariance of scalar Feynman graphs of any planar topology under the Yangian level-one momentum symmetry given certain constraints on the propagator powers. The proof relies on relating this symmetry to a planarized version of the conformal simplices of Bzowski, McFadden, and Skenderis. In particular, this proves a momentum-space analogue of the position-space conformal condition on propagator powers. When combined with the latter, the invariance under the level-one momentum implies full Yangian symmetry of the considered graphs. These include all scalar Feynman integrals for which a Yangian symmetry was previously demonstrated at the level of examples, e.g., the fishnet or loom graphs, as well as generalizations to graphs with massive propagators.}, archive = {J_PRL}, author = {Florian Loebbert and Lucas Rüenaufer and Sven F. Stawinski}, doi = {10.1103/fvzk-dp1b}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151603}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlocal symmetries of planar feynman integrals}, volume = {135}, year = {2025}, }
• (2025). Krylov spread complexity as holographic complexity beyond jackiw-teitelboim gravity. PRL, 135(15), 151602. (www)

  @article{ , abstract = {One of the important open problems in quantum black hole physics is a dual interpretation of holographic complexity proposals. To date the only quantitative match is the equality between the Krylov spread complexity in the triple-scaled Sachdev-Ye-Kitaev (SYK) model and the complexity volume proposal in classical Jackiw-Teitelboim gravity. Our Letter utilizes the recent connection between the double-scaled SYK model and sine dilaton gravity to show that the quantitative relation between Krylov spread complexity and complexity volume extends to finite temperatures and to full quantum regime on the gravity side at disk level. Furthermore, we isolate the first quantum correction to the complexity volume proposal and propose to view it as a complexity of quantum fields in the bulk. The key lesson from our Letter is that gravity demands to assign complexity also to Euclidean state preparation.}, archive = {J_PRL}, author = {Michal P. Heller and Jacopo Papalini and Tim Schuhmann}, doi = {10.1103/spcr-jgm6}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151602}, shortjournal = {Phys. Rev. Lett.}, title = {Krylov spread complexity as holographic complexity beyond jackiw-teitelboim gravity}, volume = {135}, year = {2025}, }
• (2025). Supertranslations from scattering amplitudes. PRL, 135(15), 151601. (www)

  @article{ , abstract = {On shell methods have found a new application to local observables such as asymptotic radiation fields and gravitational waveforms. While these observables are invariant under small gauge transformations, they are known to depend on a choice of asymptotic gauge; in gravity on asymptotically Minkowski spacetimes, this is a choice of Bondi-Van der Burg-Metzner-Sachs frame. In this Letter, we provide a method for capturing these supertranslations, to all orders in perturbation theory, using the on shell framework of scattering amplitudes.}, archive = {J_PRL}, author = {Asaad Elkhidir and Donal O’Connell and Radu Roiban}, doi = {10.1103/fxdk-5qwc}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151601}, shortjournal = {Phys. Rev. Lett.}, title = {Supertranslations from scattering amplitudes}, volume = {135}, year = {2025}, }
• (2025). Superradiant axionic black-hole clouds as seeds for graviton squeezing. PRL, 135(15), 151501. (www)

  @article{ , abstract = {It is shown that both standard general relativity (GR) and Chern-Simons (CS) gravity, the latter containing chiral gravitational anomaly terms, seed the production of pairs of entangled gravitons in a multi-mode squeezed state. This involves the interaction of gravitons with the axionic cloud surrounding a superradiant Kerr (rotating) black hole background. The order of magnitude of the squeezing effect, specifically the number of graviton excitations in the squeezed vacuum, is estimated in the nonrelativistic limit, relevant for the superradiance process. It is found analytically that the squeezing from the GR process of annihilation of two axions into two gravitons, dominates, by many orders of magnitude, that coming from the axion decay into two gravitons, induced by the higher-derivative CS term. It is also shown that significant squeezing effects are produced in the case of long-lived axionic clouds, whose lifetimes are much longer than the timescale for which superradiance is effective. A brief discussion on current exclusion (for the first time) of very long axion-cloud lifetimes, through comparison of our results with current LIGO data, as well as potential detection of such effects in future interferometers is also given.}, archive = {J_PRL}, author = {Panagiotis Dorlis and N. E. Mavromatos and Sarben Sarkar and Sotirios-Neilos Vlachos}, doi = {10.1103/9crd-zj6l}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151501}, shortjournal = {Phys. Rev. Lett.}, title = {Superradiant axionic black-hole clouds as seeds for graviton squeezing}, volume = {135}, year = {2025}, }
• (2025). Dynamical response of viscous objects to gravitational waves. PRL, 135(15), 151402. (www)

  @article{ , abstract = {We study the dynamical response of viscous materials to gravitational waves, in the context of a fully relativistic theory of fluid dynamics. For the first time, we calculate oscillation modes and scattering properties of viscous stars. Viscous stars absorb high-frequency radiation, following a dispersion relation introduced by Press. In the extremely large viscosity regime, stars would become reflectors of waves, but this regime appears to be forbidden by causality bounds. In the context of black hole mimickers, we show how maximally viscous stars on the threshold of stability mimic the absorption of a black hole with the same mass. Our results suggest that rotating viscous stars will amplify incoming radiation.}, archive = {J_PRL}, author = {Valentin Boyanov and Vitor Cardoso and Kostas D. Kokkotas and Jaime Redondo-Yuste}, doi = {10.1103/smlr-v7b2}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151402}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical response of viscous objects to gravitational waves}, volume = {135}, year = {2025}, }
• (2025). Nonlinearly self-interacting extended bodies move as test bodies in effective external fields. PRL, 135(15), 151401. (www)

  @article{ , abstract = {In electromagnetism, linearized general relativity, and other contexts, previous work has shown that the laws of motion which govern compact, self-interacting bodies can be obtained by applying “Detweiler-Whiting prescriptions” to the laws of motion that govern test bodies. These prescriptions replace any field that appears in a test-body law of motion with a certain effective field which is a quasilocal functional of the physical variables—a functional that can be interpreted as a regularization procedure in a point-particle limit. We generalize these results, presenting a formalism that allows Detweiler-Whiting prescriptions to be be directly derived for extended bodies, even in nonlinear field theories. If a generating functional with particular properties can be constructed, we find effective linear and angular momenta which evolve via Mathisson-Papapetrou-Dixon equations involving appropriate effective fields. These equations implicitly incorporate all self-force, self-torque, and extended-body effects. Although our main focus is on bodies coupled to nonlinear scalar fields, we also remark on the gravitational case.}, archive = {J_PRL}, author = {Abraham I. Harte and Francisco M. Blanco and Éanna É. Flanagan}, doi = {10.1103/k74d-dj7y}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {151401}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinearly self-interacting extended bodies move as test bodies in effective external fields}, volume = {135}, year = {2025}, }
• (2025). Toward a scalable linear-cavity enhanced warm-vapor photonic quantum memory. PRL, 135(15), 150803. (www)

  @article{ , abstract = {The coherent storage, buffering and retrieval of photons in a quantum memory enables the scalable creation of photonic entangled states via linear optics and repeat-until success, unlocking applications in quantum communications and photonic quantum computing. Quantum memories based on off-resonant cascaded absorption (ORCA) in atomic vapors allow this storage to be broadband, noise free, and high efficiency. Here, we implement a cavity-enhanced ORCA memory with reduced footprint and reduced power requirements compared to conventional single-pass schemes. By combining a strong magnetic field with polarization control, we maintain a Doppler-free interaction and eliminate the need for optical pumping. Our design establishes the feasibility of large arrays of ultracompact, low-power, near-unit efficiency, noiseless quantum memories running at GHz bandwidth, without the need for atom trapping or cryogenics.}, archive = {J_PRL}, author = {Bharath Srivathsan and Rafal Gartman and Robert J. A. Francis-Jones and Peter J. Mosley and Joshua Nunn}, doi = {10.1103/jvbn-p38d}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150803}, shortjournal = {Phys. Rev. Lett.}, title = {Toward a scalable linear-cavity enhanced warm-vapor photonic quantum memory}, volume = {135}, year = {2025}, }
• (2025). Scalable and modular generation of W-state entanglements via memory-enhanced fusion. PRL, 135(15), 150802. (www)

  @article{ , abstract = {Efficient generation of large-scale multipartite entangled states is a critical but challenging task in quantum information processing. Although generation of multipartite entanglement within a small set of individual qubits has been demonstrated, further scale-up in system size requires the connection of smaller entangled states into a larger state in a scalable and modular manner. Here, we achieve this goal by implementing memory-enhanced fusion of two multipartite entangled states via photonic interconnects. Through asynchronous preparation of two tripartite -state entanglements in two spatially separated modules of atomic quantum memories and on-demand fusion via single-photon interference, we demonstrate the creation of a four-partite -state entanglement shared by two remote quantum memory modules in a heralded way. We also demonstrate memory-enhanced scaling in efficiencies in the entanglement fusion. The demonstrated scalable generation and fusion of multipartite entangled states pave the way toward realization of large-scale distributed quantum information processing in the future.}, archive = {J_PRL}, author = {Jixuan Shi and Sheng Zhang and Yukai Wu and Yuedong Sun and Yibo Liang and Hai Wang and Yunfei Pu and Luming Duan}, doi = {10.1103/w4w4-lf6r}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150802}, shortjournal = {Phys. Rev. Lett.}, title = {Scalable and modular generation of W-state entanglements via memory-enhanced fusion}, volume = {135}, year = {2025}, }
• (2025). Experimental efficient source-independent quantum secret sharing against coherent attacks. PRL, 135(15), 150801. (www)

  @article{ , abstract = {Source-independent quantum secret sharing (SI QSS), while essential for secure multi-user cryptographic operations in quantum networks, faces significant implementation challenges stemming from the inherent complexity of generating and distributing multipartite entangled states. Recently, a resource-efficient SI QSS protocol utilizing entangled photon pairs combined with a postmatching method has been proposed to address this limitation. In this Letter, we report an experimental demonstration of this protocol using high-fidelity polarization-entangled photon pairs in a star topology. For a three-user network, we obtain secure key rates of 21.18, 4.69, and 1.71 kbps under single-user channel losses of 7.6, 10.9, and 12.9 dB respectively. Furthermore, under conditions of equal channel loss per user, we achieve secure key rates of 6.97, 6.46, and 5.88 kbps for three-, four-, and five-user scenarios respectively. These results demonstrate the advantageous independence of the key rate from the number of users. Our Letter paves the way for large-scale deployment of SI QSS in multiuser quantum networks.}, archive = {J_PRL}, author = {Yi-Ran Xiao and Hua-Lei Yin and Wen-Ji Hua and Xiao-Yu Cao and Zeng-Bing Chen}, doi = {10.1103/7wrk-p6gl}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150801}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental efficient source-independent quantum secret sharing against coherent attacks}, volume = {135}, year = {2025}, }
• (2025). Coupling between a Si/SiGe resonant exchange qubit and a high-impedance microwave resonator. PRL, 135(15), 150604. (www)

  @article{ , abstract = {Coherent spin-photon coupling is believed to play a significant role in silicon-based quantum computation. The resonant exchange (RX) qubit, formed in a triple quantum dot, is a promising platform for spin-photon coupling and qubit scaling due to the large electric dipole moment and full electrical control without auxiliary micromagnets. However, there has been no experimental demonstration of silicon RX qubits and their strong coupling to microwave photons to date. In this work, we report the strong coupling between an RX qubit and a high-impedance resonator on a Si/SiGe heterostructure with coupling strength g s / ( 2 π ) = 65.8 MHz and decoherence rate γ s / ( 2 π ) = 21.4 MHz . Furthermore, the dependence of decoherence rate on detuning is measured and analyzed using a phenomenological model, indicating that the charge noise is the main source of decoherence. Our results demonstrate the viability of RX qubits in silicon, highlighting their crucial role of large-scale qubit integration for silicon quantum computation and opening new possibilities for quantum network.}, archive = {J_PRL}, author = {Shun-Li Jiang and Tian-Yi Jiang and Shu-Kun Ye and Ran-Ran Cai and Tian-Yue Hao and Yong-Qiang Xu and Zong-Hu Li and Yuan Kang and Bao-Chuan Wang and Hai-Ou Li and Guang-Can Guo and Xiang-Xiang Song and Gang Cao and Guo-Ping Guo}, doi = {10.1103/31wk-5yqp}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150604}, shortjournal = {Phys. Rev. Lett.}, title = {Coupling between a Si/SiGe resonant exchange qubit and a high-impedance microwave resonator}, volume = {135}, year = {2025}, }
• (2025). In the shadow of the hadamard test: Using the garbage state for good and further modifications. PRL, 135(15), 150603. (www)

  @article{ , abstract = {The Hadamard test is one of the pillars on which quantum algorithm development rests and, at the same time, is naturally suited for the intermediate regime between the current era of noisy quantum devices and complete fault tolerance. Its applications use measurements of the auxiliary qubit to extract information but disregard the system register completely. Concomitantly, but independently of this development, advances in quantum learning theory have enabled the efficient representation of quantum states via classical shadows. This Letter shows that, strikingly, putting both lines of thought into a new context results in substantial improvements to the Hadamard test on a single auxiliary readout qubit, by suitably exploiting classical shadows on the remaining n -qubit work register. We argue that this combination inherits the best of both worlds and discuss statistical phase estimation as a vignette application. At the same time, the framework is more general and applicable to a wide range of other algorithms. There, we can use the Hadamard test to estimate energies on the auxiliary qubit, while classical shadows on the system register provide access to additional features such as (i) the fidelity of the initial state with certain pure quantum states, (ii) the initial state’s energy, and (iii) how pure and how close the initial state is to an eigenstate of the Hamiltonian. Finally, we also discuss how anticontrolled unitaries can further augment this framework and explain how this Letter settles the exploitation of the Hadamard test for intermediate applications.}, archive = {J_PRL}, author = {Paul K. Faehrmann and Jens Eisert and Richard Kueng}, doi = {10.1103/cqjw-kl8s}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150603}, shortjournal = {Phys. Rev. Lett.}, title = {In the shadow of the hadamard test: Using the garbage state for good and further modifications}, volume = {135}, year = {2025}, }
• (2025). Role of coherence for quantum computational advantage. PRL, 135(15), 150602. (www)

  @article{ , abstract = {Quantifying the resources available to a quantum computer appears to be necessary to separate quantum from classical computation. Among them, entanglement, nonstabilizerness, and coherence are arguably of great significance. We introduce “path coherence” as a measure of the coherent path interferences arising in a quantum computation. Leveraging the sum-over-paths formalism, we obtain a classical algorithm for estimating quantum transition amplitudes, the complexity of which scales with path coherence. As path coherence relates to the hardness of classical estimation of quantum transition amplitudes, it provides a new perspective on the role of coherence in quantum computational advantage. Beyond their fundamental significance, our results have practical applications for simulating large classes of quantum computations with classical computers.}, archive = {J_PRL}, author = {Hugo Thomas and Pierre-Emmanuel Emeriau and Rawad Mezher and Elham Kashefi and Harold Ollivier and Ulysse Chabaud}, doi = {10.1103/1csn-x1cx}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150602}, shortjournal = {Phys. Rev. Lett.}, title = {Role of coherence for quantum computational advantage}, volume = {135}, year = {2025}, }
• (2025). Counting the ground state degeneracy by evolution methods. PRL, 135(15), 150601. (www)

  @article{ , abstract = {Counting ground state degeneracy of a k -local Hamiltonian is important in many fields of physics. Its complexity class is harder than that of finding the ground state of a k -local Hamiltonian. Very few methods can efficiently count the degeneracy of ground state while many are known for finding the ground state. This Letter proposes an algorithm for mapping the problem of counting ground state degeneracy into one for finding a special ground state of a k -local super Hamiltonian in an enlarged system with twice as many qubits or spins. We show that all traditional methods, designed for finding the ground state by evolution under a function of a Hamiltonian, can be employed to find the special ground state of the super Hamiltonian from a well-designed initial state and thus can be used to count the ground degeneracy. We combine our algorithm with the power method, the Lanczos method, and the quantum imaginary time evolution method for selective examples to illustrate the detection of phase boundaries, competition between frustration and quantum fluctuation, and potential implementation with quantum circuits.}, archive = {J_PRL}, author = {Zhen Guo and Li You}, doi = {10.1103/38gb-h7wv}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150601}, shortjournal = {Phys. Rev. Lett.}, title = {Counting the ground state degeneracy by evolution methods}, volume = {135}, year = {2025}, }
• (2025). Accelerating quantum relaxation via temporary reset: A mpemba-inspired approach. PRL, 135(15), 150403. (www)

  @article{ , abstract = {Slow relaxation processes spanning widely separated timescales pose fundamental challenges for probing steady-state properties and engineering functional quantum systems, such as quantum heat engines and quantum computing devices. We introduce a protocol that enables significant acceleration of relaxation in general Markovian open quantum systems by temporarily coupling the system to a reset channel, inspired by the Mpemba effect. Crucially, this acceleration persists even when the slowest decaying Lindbladian modes form complex-conjugate pairs. Unlike previous approaches, which typically target a single mode, our protocol may suppress multiple relaxation modes simultaneously. This framework provides a versatile and experimentally feasible tool for controlling relaxation timescales, with broad implications for quantum thermodynamics, computation, and state preparation.}, archive = {J_PRL}, author = {Ruicheng Bao and Zhonghuai Hou}, doi = {10.1103/g94p-7421}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150403}, shortjournal = {Phys. Rev. Lett.}, title = {Accelerating quantum relaxation via temporary reset: A mpemba-inspired approach}, volume = {135}, year = {2025}, }
• (2025). Exact overlaps for all integrable matrix product states of rational spin chains. PRL, 135(15), 150402. (www)

  @article{ , abstract = {The overlaps between integrable matrix product states (MPSs) and Bethe states are important in both the nonequilibrium statistical physics and the AdS/CFT duality. We present the general MPS overlap formula. The result is a product of a ratio of Gaudin determinants and a prefactor. The Gaudin determinants depend on the spin chain but not on the MPS. The MPS dependent prefactor is given for all integrable MPSs of the , and symmetric spin chains with arbitrary representations.}, archive = {J_PRL}, author = {Tamas Gombor}, doi = {10.1103/4vy2-8cnk}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150402}, shortjournal = {Phys. Rev. Lett.}, title = {Exact overlaps for all integrable matrix product states of rational spin chains}, volume = {135}, year = {2025}, }
• (2025). Nonequilibrium critical scaling of a squeezing phase transition. PRL, 135(15), 150401. (www)

  @article{ , abstract = {We investigate phase transitions in the nonequilibrium dynamics of power-law interacting spin- 1 / 2 bilayer XXZ models, which have recently been shown to allow generation of entanglement in the form of two-mode squeezing. We find a transition between a collective phase characterized by Heisenberg limited squeezing and a partially collective phase with scalable squeezing. We identify universal scaling of the squeezing dynamics in terms of system parameters and a divergent timescale, establishing these as distinct dynamical phases within the framework of nonequilibrium critical phenomena. Our Letter demonstrates a novel dynamical phase transition with potential applications in quantum sensing and quantum simulation in cold-atomic, molecular, or Rydberg platforms.}, archive = {J_PRL}, author = {Arman Duha and Samuel E. Begg and Thomas Bilitewski}, doi = {10.1103/7g55-lpff}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150401}, shortjournal = {Phys. Rev. Lett.}, title = {Nonequilibrium critical scaling of a squeezing phase transition}, volume = {135}, year = {2025}, }
• (2025). Experimental measurement-device-independent verification of continuous-variable entanglement. PRL, 135(15), 150201. (www)

  @article{ , abstract = {Quantum entanglement serves as an essential resource for quantum information technology. In many realistic quantum information tasks, it is necessary to reliably verify entanglement even when the measurement devices are unreliable. In this Letter, we experimentally demonstrate measurement-device-independent verification of continuous-variable (CV) entanglement. We show that the conventional CV entanglement witness may falsely identify a separable state as a CV entangled state when the measurement devices are unreliable. To eliminate such need for trusted measurement devices, we implement a measurement-device-independent entanglement witness for verifying CV entanglement and demonstrate its resilience against local oscillator power and phase modifications. Our Letter sheds light on advancing high-security quantum information processing and its practical implementation in quantum networks.}, archive = {J_PRL}, author = {Xutong Wang and Jing Fu and Jietai Jing}, doi = {10.1103/rk3t-69tb}, journal = {Physical Review Letters}, month = {10}, number = {15}, pages = {150201}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental measurement-device-independent verification of continuous-variable entanglement}, volume = {135}, year = {2025}, }
• (2025). Efficiently driving f1 molecular motor in experiment by suppressing nonequilibrium variation. PRL, 135(14), 148402. (www)

  @article{ , abstract = {F 1 -ATPase ( F 1 ) is central to cellular energy transduction. Forcibly rotated by another motor F o , F 1 catalyzes adenosine triphosphate (ATP) synthesis by converting mechanical work into chemical free energy stored in the molecule ATP. The details of how F o drives F 1 are not fully understood; however, evaluating efficient ways to rotate F 1 could provide fruitful insights into this driving since there is a selective pressure to improve efficiency. Here, we show that rotating F 1 with an angle clamp is significantly more efficient than a constant torque. Our experiments, combined with theory and simulation, indicate that the angle clamp significantly suppresses the nonequilibrium variation that contributes to the futile dissipation of input work.}, archive = {J_PRL}, author = {Takahide Mishima and Deepak Gupta and Yohei Nakayama and W. Callum Wareham and Takumi Ohyama and David A. Sivak and Shoichi Toyabe}, doi = {10.1103/b24h-v7by}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {148402}, shortjournal = {Phys. Rev. Lett.}, title = {Efficiently driving f1 molecular motor in experiment by suppressing nonequilibrium variation}, volume = {135}, year = {2025}, }
• (2025). Light-induced phase separation with finite wavelength selection in photophobic microalgae. PRL, 135(14), 148401. (www)

  @article{ , abstract = {As with many motile microalgae, the freshwater species Chlamydomonas reinhardtii can detect light sources and adapt its motile behavior in response. Here, we show that suspensions of photophobic cells can be unstable to density fluctuations, as a consequence of shading interactions mediated by light absorption. In a circular illumination geometry, this mechanism leads to the complete phase separation of the system into transient branching patterns, providing experimental evidence of finite wavelength selection through a motility-induced phase separation mechanism. The finite wavelength selection is a consequence of a vision-based interaction length scale which is fixed by the illumination geometry. A simple drift-diffusion framework allows us to understand how the wavelength depends on global cell density, light intensity, and medium viscosity. Finally, we show that this active phase separation shields individual cells from the deleterious effects of high light intensity, demonstrating that phototaxis can efficiently contribute to photoprotection through collective behaviors on short timescales.}, archive = {J_PRL}, author = {Isabelle Eisenmann and Alfredo L’Homme and Aliénor Lahlou and Sandrine Bujaldon and Thomas Le Saux and Benjamin Bailleul and Nicolas Desprat and Raphaël Jeanneret}, doi = {10.1103/ss2g-kbpj}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {148401}, shortjournal = {Phys. Rev. Lett.}, title = {Light-induced phase separation with finite wavelength selection in photophobic microalgae}, volume = {135}, year = {2025}, }
• (2025). Cracking down on fracture to functionalize damage. PRL, 135(14), 148202. (www)

  @article{ , abstract = {In this Letter we propose a novel relationship between topology and damage propagation in Maxwell lattices that redefines fracture as a functional design feature rather than mere degradation. We demonstrate that topologically protected modes, inherently robust against perturbations, localize along lattice discontinuities and govern the mechanical response. By precisely engineering the microstructure, we direct these modes to control stress distributions and trigger predictable, controlled damage. Our findings, validated through comprehensive numerical simulations and experiments, advance our understanding of nontrivial mechanical responses in Maxwell lattices and establish a clear framework for designing materials with improved fracture energy. This Letter paves the way for further exploration of topology-driven phenomena in mechanical systems and promises a new direction in the design of robust materials.}, archive = {J_PRL}, author = {Leo de Waal and Matthaios Chouzouris and Marcelo A. Dias}, doi = {10.1103/s28l-zbpz}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {148202}, shortjournal = {Phys. Rev. Lett.}, title = {Cracking down on fracture to functionalize damage}, volume = {135}, year = {2025}, }
• (2025). Theory of reversed ripening in active phase separating systems. PRL, 135(14), 148201. (www)

  @article{ , abstract = {The ripening dynamics in passive systems is governed by the theory of Lifshitz-Slyosov-Wagner (LSW). Here, we present an analog theory for reversed ripening in active systems. To derive the dynamic theory for the droplet size distribution, we consider a minimal ternary emulsion with one active reaction, leading to one conserved quantity. Even for cases where single droplets constantly grow, coupling many droplets via the conserved density in the far field leads to a self-organized reversal of ripening and, thus, a monodisperse emulsion. For late times, we find a scaling ansatz leading to the collapse of the rescaled size distributions, different from the LSW theory. This scaling behavior arises from a stable fixed point in the single droplet dynamics and may capture the late-time behavior of many active matter systems exhibiting reversed ripening.}, archive = {J_PRL}, author = {Jonathan Bauermann and Giacomo Bartolucci and Christoph A. Weber and Frank Jülicher}, doi = {10.1103/f5x9-wp3g}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {148201}, shortjournal = {Phys. Rev. Lett.}, title = {Theory of reversed ripening in active phase separating systems}, volume = {135}, year = {2025}, }
• (2025). Stopping cross sections for protons across different phases of water. PRL, 135(14), 148003. (www)

  @article{ , abstract = {Accurately quantifying the energy loss rate of proton beams in liquid water is crucial for the precise application and improvement of proton therapy, whereas the slowing down of protons in water ices also plays an important role in astrophysics. However, precisely determining the electronic stopping power, particularly for the liquid phase, has been elusive so far. Experimental techniques are difficult to apply to volatile liquids, and the availability of sufficient reliable measurements has been limited to the solid and vapor phases. The accuracy of current models is typically limited to proton energies just above the energy loss maximum, making it difficult to predict radiation effects at an energy range of special relevance. We elucidate the phase differences in proton energy loss in water in a wide energy range ( 0.001 − 10 MeV ) by means of real-time time-dependent density functional theory combined with the Penn method. This nonperturbative model, more computationally efficient than current approaches, describes the phase effects in water in excellent agreement with available experimental data, revealing clear deviations around the maximum of the stopping power curve and below. As an important outcome, our calculations reveal that proton stopping quantities of liquid water and amorphous ice are identical, in agreement with recent similar observations for low-energy electrons, pointing out this equivalence for all charged particles. This could help to overcome the limitation in obtaining reliable experimental information for the biologically relevant liquid water target.}, archive = {J_PRL}, author = {F. Matias and N. E. Koval and P. de Vera and R. Garcia-Molina and I. Abril and J. M. B. Shorto and H. Yoriyaz and J. J. N. Pereira and T. F. Silva and M. H. Tabacniks and M. Vos and P. L. Grande}, doi = {10.1103/ksdx-mnd7}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {148003}, shortjournal = {Phys. Rev. Lett.}, title = {Stopping cross sections for protons across different phases of water}, volume = {135}, year = {2025}, }
• (2025). Walks in rotation spaces return home when doubled and scaled. PRL, 135(14), 147201. (www)

  @article{ , abstract = {The dynamics of numerous physical systems, such as spins and qubits, can be described as a series of rotation operations, i.e., walks in the manifold of the rotation group. A basic question with practical applications is how likely and under what conditions such walks return to the origin (the identity rotation), which means that the physical system returns to its initial state. In three dimensions, we show that almost every walk in SO(3) or SU(2), even a very complicated one, will preferentially return to the origin simply by traversing the walk twice in a row and uniformly scaling all rotation angles. We explain why traversing the walk only once almost never suffices to return, and comment on the problem in higher dimensions.}, archive = {J_PRL}, author = {Jean-Pierre Eckmann and Tsvi Tlusty}, doi = {10.1103/xk8y-hycn}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {147201}, shortjournal = {Phys. Rev. Lett.}, title = {Walks in rotation spaces return home when doubled and scaled}, volume = {135}, year = {2025}, }
• (2025). Energy diffusion in the long-range interacting spin systems. PRL, 135(14), 147102. (www)

  @article{ , abstract = {We investigate energy diffusion in long-range interacting spin systems, where the interaction decays algebraically as V ( r ) ∝ r − α with the distance r between the sites. We consider prototypical spin systems, the transverse Ising model, and the XYZ model in the D -dimensional lattice with a finite exponent α > D which guarantees the thermodynamic extensivity. In one dimension, both normal and anomalous diffusion are observed, where the anomalous diffusion is attributed to anomalous enhancement of the amplitude of the equilibrium current correlation. We prove the power-law clustering property of arbitrary orders of joint cumulants in general dimensions. Applying this theorem to equal-time current correlations, we further prove several theorems leading to the statement that the sufficient condition for normal diffusion in one dimension is α > 3 / 2 regardless of the models. The fluctuating hydrodynamics approach consistently explains Lévy diffusion for α < 3 / 2 , which implies that the condition is optimal. In higher dimensions of D ≥ 2 , normal diffusion is indicated as long as α > D .}, archive = {J_PRL}, author = {Hideaki Nishikawa and Keiji Saito}, doi = {10.1103/hsbt-c46n}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {147102}, shortjournal = {Phys. Rev. Lett.}, title = {Energy diffusion in the long-range interacting spin systems}, volume = {135}, year = {2025}, }
• (2025). Information engine fueled by first-passage times. PRL, 135(14), 147101. (www)

  @article{ , abstract = {Using a mechanical cantilever submitted to electrostatic feedback control, we investigate the thermodynamic properties of an information engine that extracts work from thermal fluctuations. The cantilever position is rapidly sampled and the feedback is triggered by the first passage of the system across a fixed threshold. The information ΔI associated with the feedback is based on the first-passage-time distribution. In this setting, we derive and experimentally verify two distinct fluctuation theorems that involve Δ I and give a tight bound on the work produced by the engine. Our results extend beyond the specific application to our experiment: we develop a general framework for obtaining fluctuation theorems and work bounds, formulated in terms of probability distributions of protocols rather than underlying measurement outcomes.}, archive = {J_PRL}, author = {Aubin Archambault and Caroline Crauste-Thibierge and Alberto Imparato and Christopher Jarzynski and Sergio Ciliberto and Ludovic Bellon}, doi = {10.1103/s9kj-lczm}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {147101}, shortjournal = {Phys. Rev. Lett.}, title = {Information engine fueled by first-passage times}, volume = {135}, year = {2025}, }
• (2025). Generating phase singularities using surface exciton polaritons in an organic natural hyperbolic material. PRL, 135(14), 146906. (www)

  @article{ , abstract = {Surface polaritons (SPs) are electromagnetic waves bound to a surface through their interaction with charge carriers in the surface material. Hyperbolic SPs can be supported by optically anisotropic materials where the in-plane and out-of-plane permittivities have opposite signs. Here we report what we believe to be the first experimental study of hyperbolic surface exciton polaritons (HSEPs). We study the intensity and phase response of HSEPs in the J-aggregate TDBC (a type-II natural hyperbolic material). HSEPs can be used to generate phase singularities; the behavior of these phase singularities is a consequence of the hyperbolic nature of TDBC. The combined intensity and phase response of nonhyperbolic and hyperbolic SPs suggests that they are topologically distinct. We predict analogous effects for hyperbolic surface phonon polaritons in hexagonal boron nitride. Our Letter suggests that organic materials can provide a new platform for the exploration of hyperbolic surface polaritonics at visible frequencies.}, archive = {J_PRL}, author = {Philip A. Thomas and William P. Wardley and William L. Barnes}, doi = {10.1103/sj4r-cb56}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146906}, shortjournal = {Phys. Rev. Lett.}, title = {Generating phase singularities using surface exciton polaritons in an organic natural hyperbolic material}, volume = {135}, year = {2025}, }
• (2025). Unidirectional giant exciton emission into a photonic waveguide. PRL, 135(14), 146905. (www)

  @article{ , abstract = {Efficient coupling of nanolight sources into photonic waveguides is crucial for integrated photonics, quantum technologies, and biosensing. Practical implementations require light sources with simultaneous high brightness and unidirectional emission. However, it is fundamentally incompatible between strong electromagnetic field confinement and directional radiation. Here, we demonstrate the simultaneous giant excitonic photoluminescence (PL) enhancement and unidirectional emission from a two-dimensional InSe film integrated with an asymmetric plasmonic nanocavity. A 3500-fold PL enhancement is achieved by engineering spatial, spectral, and orientational overlap between cavity modes and out-of-plane excitons in InSe. Symmetry breaking within the nanocavity ensures precise control of emission interference, yielding a record-high directivity exceeding 15 dB. The design achieves a high coupling efficiency of 24% and supports guided light propagation of 140 μ m . Our results establish a scalable approach for the ultracompact integration of nanoscale light sources into monolithic photonic circuits and will advance the development of on-chip nanophotonics.}, archive = {J_PRL}, author = {Qifa Wang and Huan Luo and Chaojie Ma and Bingchang Zhang and Cheng Ji and Qinghong Yu and Guoxiang Chai and Yuxin Li and Chenyang Li and Shaojun Wang and Xuetao Gan and Kaihui Liu and Jianlin Zhao and Fajun Xiao}, doi = {10.1103/3fxz-6v6s}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146905}, shortjournal = {Phys. Rev. Lett.}, title = {Unidirectional giant exciton emission into a photonic waveguide}, volume = {135}, year = {2025}, }
• (2025). Ultrafast nonequilibrium enhancement of electron-phonon interaction in 2H−MoTe2. PRL, 135(14), 146904. (www)

  @article{ , abstract = {Understanding nonequilibrium electron-phonon interactions at the microscopic level and on ultrafast timescales is a central goal of modern condensed matter physics. Combining time- and angle-resolved extreme ultraviolet photoemission spectroscopy with constrained density functional perturbation theory, we demonstrate that photoexcited carrier density can serve as a tuning knob to enhance electron-phonon interactions in nonequilibrium conditions. Specifically, nonequilibrium band structure mapping and valley-resolved ultrafast population dynamics in semiconducting transition-metal dichalcogenide 2 H − MoTe 2 reveal band-gap renormalizations and reduced population lifetimes as photoexcited carrier densities increase. Through theoretical analysis of photoinduced electron and phonon energy and linewidth renormalizations, we attribute these transient features to nonequilibrium modifications of electron-phonon coupling matrix elements. This Letter advances our understanding of microscopic coupling mechanisms enabling control over relaxation pathways in driven solids.}, archive = {J_PRL}, author = {Nina Girotto Erhardt and Sotirios Fragkos and Dominique Descamps and Stéphane Petit and Michael Schüler and Dino Novko and Samuel Beaulieu}, doi = {10.1103/dvlz-93t8}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146904}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrafast nonequilibrium enhancement of electron-phonon interaction in 2H−MoTe2}, volume = {135}, year = {2025}, }
• (2025). Generation of pure spin current with insulating antiferromagnetic materials. PRL, 135(14), 146703. (www)

  @article{ , abstract = {The generation of pure spin currents is critical for low-dissipation spintronic applications, yet existing methods relying on spin-orbit coupling or ferromagnetic interfaces face challenges in material compatibility and operational robustness. We propose a paradigm-shifting approach to generate symmetry-protected pure spin currents by applying mechanical stress on insulating antiferromagnetic materials, i.e., the pure piezospintronic effect. We first classify magnetic point groups enabling pure piezospintronic effects. A novel first-principles method is developed to compute the spin dipole moments and coefficients of the piezospintronic effect. Integrating these methodologies with high-throughput screening, we identify FeOOH, Cr 2 O 3 , and NaMn X ( X = As , Bi, P, Sb) with significant pure piezospintronic effects. Interestingly, we reveal that the ionic displacement contribution dominates the piezospintronic effect, in contrast to the piezoelectric effect. Our study not only provides a first-principles approach for investigating spin dipole moment related phenomena (e.g., ferrotoroidicity, fractional quantum spin dipole moment, piezospintronics), but also provides promising piezospintronic materials for experimental verification and industrial applications.}, archive = {J_PRL}, author = {Yingwei Chen and Junyi Ji and Liangliang Hong and Xiangang Wan and Hongjun Xiang}, doi = {10.1103/n8d2-hjnd}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146703}, shortjournal = {Phys. Rev. Lett.}, title = {Generation of pure spin current with insulating antiferromagnetic materials}, volume = {135}, year = {2025}, }
• (2025). Fate of bosonic topological edge modes in the presence of many-body interactions. PRL, 135(14), 146702. (www)

  @article{ , abstract = {Many magnetic materials are predicted to exhibit bosonic topological edge modes in their excitation spectra, because of the nontrivial topology of their magnon, triplon, or other quasiparticle band structures. However, there is a discrepancy between theory prediction and experimental observation, which suggests some underlying mechanism that intrinsically suppresses the expected experimental signatures, like the thermal Hall current. Many-body interactions that are not accounted for in the noninteracting quasiparticle picture are most often identified as the reason for the absence of the topological edge modes. Here we report persistent bosonic edge modes at the boundaries of a ladder quantum paramagnet with gapped triplon excitations in the presence of the full many-body interaction. We use tensor network methods to resolve topological edge modes in the time-dependent spin-spin correlations and the dynamical structure factor, which is directly accessible experimentally. We further show that signatures of these edge modes survive even when the noninteracting quasiparticle theory breaks down; we discuss the topological phase diagram of the model, demonstrate the fractionalization of its low-lying excitations, and propose potential material candidates.}, archive = {J_PRL}, author = {Niclas Heinsdorf and Darshan G. Joshi and Hosho Katsura and Andreas P. Schnyder}, doi = {10.1103/1pty-fvpf}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146702}, shortjournal = {Phys. Rev. Lett.}, title = {Fate of bosonic topological edge modes in the presence of many-body interactions}, volume = {135}, year = {2025}, }
• (2025). Field-induced magnon decay, magnon shadows, and rotonlike excitations in the honeycomb antiferromagnet YbBr3. PRL, 135(14), 146701. (www)

  @article{ , abstract = {Although the search for quantum many-body phenomena in magnetic materials has a strong focus on highly frustrated systems, even unfrustrated quantum magnets show a multitude of unconventional phenomena in their spin excitation spectra. YbBr 3 is an excellent realization of the S = 1 / 2 antiferromagnetic Heisenberg model on the honeycomb lattice, and we have performed detailed spectroscopic experiments with both unpolarized and polarized neutrons at all applied magnetic fields up to saturation. We observe extensive excitation continua, which cause strong renormalization and the decay of single magnons at higher fields, while coherent features include field-induced “shadows” of the single magnons and the spectacular emergence of a rotonlike excitation. To guide and interpret our experiments, we performed systematic calculations by the method of cylinder matrix-product states that provide quantitative agreement with the neutron scattering data and a qualitative benchmark for the spectral signatures of strong quantum fluctuations even in the absence of magnetic frustration.}, archive = {J_PRL}, author = {J. A. Hernández and A. A. Eberharter and M. Schuler and J. Lass and D. G. Mazzone and R. Sibille and S. Raymond and K. W. Krämer and B. Normand and B. Roessli and A. M. Läuchli and M. Kenzelmann}, doi = {10.1103/q29r-8x1m}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146701}, shortjournal = {Phys. Rev. Lett.}, title = {Field-induced magnon decay, magnon shadows, and rotonlike excitations in the honeycomb antiferromagnet YbBr3}, volume = {135}, year = {2025}, }
• (2025). Most two-dimensional bosonic topological orders forbid sign-problem-free quantum monte carlo simulation: Nonpositive gauss sum as an indicator. PRL, 135(14), 146602. (www)

  @article{ , abstract = {Quantum Monte Carlo is a powerful tool for studying quantum many-body physics, yet its efficacy is often curtailed by the notorious sign problem. In this Letter, we introduce a novel criterion for the “intrinsic” sign problem in two-dimensional bosonic topological orders, which cannot be resolved by local basis transformations or adiabatic deformations of the Hamiltonian. Specifically, we find that the positivity of higher Gauss sums is a necessary condition for a two-dimensional bosonic topological order to be realized by a stoquastic Hamiltonian, and hence “sign-problem-free.” Equivalently, a nonpositive higher Gauss sum for a given topological order indicates the presence of an intrinsic sign problem. This condition not only aligns with prior findings but significantly broadens their scope. Using this new criterion, we examine the Gauss sums of all 405 bosonic topological orders classified up to rank 12, and strikingly find that 398 of them exhibit intrinsic sign problems. We also uncover intriguing links between the intrinsic sign problem, the gappability of boundary theories, and time-reversal symmetry, suggesting that sign-problem-free quantum Monte Carlo simulation may fundamentally rely on both time-reversal symmetry and gapped boundaries. These results highlight the deep connection between the intrinsic sign problem and fundamental properties of topological phases, offering valuable insights into their classical simulability.}, archive = {J_PRL}, author = {Donghae Seo and Minyoung You and Hee-Cheol Kim and Gil Young Cho}, doi = {10.1103/c8n5-l11j}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146602}, shortjournal = {Phys. Rev. Lett.}, title = {Most two-dimensional bosonic topological orders forbid sign-problem-free quantum monte carlo simulation: Nonpositive gauss sum as an indicator}, volume = {135}, year = {2025}, }
• (2025). Dichotomy in low- and high-energy band renormalizations in trilayer nickelate La4Ni3O10: A comparison with cuprates. PRL, 135(14), 146506. (www)

  @article{ , abstract = {Band renormalizations comprise crucial insights for understanding the intricate roles of electron-boson coupling and electron correlation in emergent phenomena such as superconductivity. In this Letter, by combining high-resolution angle-resolved photoemission spectroscopy and theoretical calculations, we systematically investigate the electronic structure of the trilayer nickelate superconductor La 4 Ni 3 O 10 at ambient pressure. We reveal a dichotomy in the electronic band renormalizations of La 4 Ni 3 O 10 in comparison to cuprate superconductors. At a high energy scale of hundreds of meV, its band structure is strongly renormalized by an electron correlation effect enhanced by Hund’s coupling. The resultant waterfall-like dispersions resemble the high-energy kinks in cuprate superconductors. However, at low-energy scales of tens of meV, the dispersive bands are nearly featureless and devoid of any resolvable electron-boson interactions, in drastic contrast to the low-energy kinks observed in cuprates and other correlated 3 d transition-metal compounds. The dichotomic band renormalizations highlight the disparity between nickelate and cuprate superconductors and emphasize the importance of strong electron correlation in the superconductivity of Ruddlesden-Popper phase nickelates.}, archive = {J_PRL}, author = {X. Du and Y. L. Wang and Y. D. Li and Y. T. Cao and M. X. Zhang and C. Y. Pei and J. M. Yang and W. X. Zhao and K. Y. Zhai and Z. K. Liu and Z. W. Li and J. K. Zhao and Z. T. Liu and D. W. Shen and Z. Li and Y. He and Y. L. Chen and Y. P. Qi and H. J. Guo and L. X. Yang}, doi = {10.1103/smkf-k7wq}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146506}, shortjournal = {Phys. Rev. Lett.}, title = {Dichotomy in low- and high-energy band renormalizations in trilayer nickelate La4Ni3O10: A comparison with cuprates}, volume = {135}, year = {2025}, }
• (2025). Quantum anomalous hall effects and emergent SU(2) hall ferromagnets at fractional filling of helical trilayer graphene. PRL, 135(14), 146505. (www)

  @article{ , abstract = {Helical trilayer graphene realizes a versatile moiré system for exploring correlated topological states emerging from high Chern bands. Motivated by recent experimental observations of anomalous Hall effects at fractional fillings of magic-angle helical trilayers, we focus on the higher Chern number | C band | = 2 band and explore gapped many-body Hall states beyond the conventional Landau level paradigm. Through extensive exact diagonalization, we predict novel phases unattainable in a single | C band | = 1 band. At filling ν = 2 / 3 and ν = 1 / 3 , a 3 × 3 charge-ordered quantum Hall crystal and a Halperin fractional Chern insulator with Hall conductance | σ H | = 2 e 2 / 3 h are predicted, respectively, indicating strong particle-hole asymmetry of the system. At half-filling ν = 1 / 2 , an extensively degenerate pseudospin Hall ferromagnet featuring emergent SU(2) symmetry is found without the band being flat. Inspired by striking robustness of the ferromagnetic degeneracy, we develop a method to unveil and quantify the emergent symmetry via pseudospin operator construction in the presence of band dispersion and Coulomb interaction and demonstrate persistence of the SU(2) quantum numbers even far away from the chiral limit. Incorporating spin-valley degrees of freedom, we identify an optimal filling regime ν total = 3 + ν for realizing the above states. Notably, interflavor interactions renormalize the bandwidth and stabilize all the gapped phases even in realistic sublattice corrugation parameter regimes.}, archive = {J_PRL}, author = {Sen Niu and Jason Alicea and D. N. Sheng and Yang Peng}, doi = {10.1103/rwd7-92z9}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146505}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum anomalous hall effects and emergent SU(2) hall ferromagnets at fractional filling of helical trilayer graphene}, volume = {135}, year = {2025}, }
• (2025). Emergent inductance from chiral orbital currents in a bulk ferrimagnet. PRL, 135(14), 146504. (www)

  @article{ , abstract = {We report the discovery of a new form of inductance in the bulk ferrimagnet Mn 3 Si 2 Te 6 , which features strong spin-orbit coupling, large magnetic anisotropy, and pronounced magnetoelastic interactions. Below its Curie temperature ( T C ≈ 78 K ), Mn 3 Si 2 Te 6 hosts chiral orbital currents (COC) that circulate within the crystal lattice and give rise to collective electronic behavior [Control of chiral orbital currents in a colossal magnetoresistance material, Nature (London) 611 , 467 (2022) .]. By applying a magnetic field along the hard c axis and driving the system with low-frequency currents, we uncover a giant inductive response up to millhenry scale, originating from first-order reconfigurations of COC domains. These domains act as coherent mesoscopic inductive elements that resist reversal upon current reduction, producing a large electromotive force and sharply increasing voltage. This emergent inductance defies classical models, occurs without superconductivity or engineered nanostructures, and opens a new frontier in orbital-based quantum functionality and device concepts.}, archive = {J_PRL}, author = {Gang Cao and Hengdi Zhao and Yu Zhang and Alex Fix and Tristan R. Cao and Dhruva Ananth and Yifei Ni and Gabriel Schebel and Rahul Nandkishore and Itamar Kimchi and Hua Chen and Feng Ye and Lance E. DeLong}, doi = {10.1103/r22l-y2rr}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146504}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent inductance from chiral orbital currents in a bulk ferrimagnet}, volume = {135}, year = {2025}, }
• (2025). Observation of anisotropic dispersive dark-exciton dynamics in CrSBr. PRL, 135(14), 146503. (www)

  @article{ , abstract = {Many-body excitons in CrSBr are attracting intense interest in view of their highly anisotropic magneto-optical coupling and their potential for novel optical interfaces within spintronic and magnonic devices. Characterizing the orbital character and propagation of these electronic excitations is crucial for understanding and controlling their behavior; however, this information is challenging to access. High resolution resonant inelastic x-ray scattering is a momentum-resolved technique that can address these crucial questions. We present measurements collected at the Cr L 3 -edge which show a rich spectrum of excitations with a variety of spin-orbital characters. While most of these excitations appear to be localized, the dispersion of the lowest energy dark exciton indicates that it is able to propagate along both the a and b directions within the planes of the crystal. This two-dimensional character is surprising as it contrasts with electrical conductivity and the behavior of the bright exciton, both of which are strongly one dimensional. The discovery of this propagating dark exciton highlights an unusual coexistence of one- and two-dimensional electronic behaviors in CrSBr.}, archive = {J_PRL}, author = {J. Sears and B. Zager and W. He and C. A. Occhialini and Y. Shen and M. Lajer and J. W. Villanova and T. Berlijn and F. Yakhou-Harris and N. B. Brookes and D. G. Chica and X. Roy and E. Baldini and J. Pelliciari and V. Bisogni and S. Johnston and M. Mitrano and M. P. M. Dean}, doi = {10.1103/fz3h-6jdx}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146503}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of anisotropic dispersive dark-exciton dynamics in CrSBr}, volume = {135}, year = {2025}, }
• (2025). Identification of gapless phases by a twisting operator. PRL, 135(14), 146502. (www)

  @article{ , abstract = {We propose a general necessary condition for a spin chain with SO(3) spin-rotation symmetry to be gapped. Specifically, we prove that the ground state(s) of an SO(3)-symmetric gapped spin chain must be spin singlet(s), and the expectation value of a twisting operator asymptotically approaches unity in the thermodynamic limit, where finite-size corrections are inversely proportional to the system size. This theorem provides (i) supporting evidence for various conjectured gapped phases and (ii) a sufficient criterion for identifying gapless spin chains. We verify our theorem by numerical simulations for a variety of spin models and show that it offers a novel efficient way to identify gapless phases in spin chains with spin-rotation symmetry.}, archive = {J_PRL}, author = {Hang Su and Tengzhou Zhang and Yuan Yao and Akira Furusaki}, doi = {10.1103/29j7-ltfn}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {146502}, shortjournal = {Phys. Rev. Lett.}, title = {Identification of gapless phases by a twisting operator}, volume = {135}, year = {2025}, }
• (2025). Surface wave electron acceleration from flat foils at parallel laser incidence. PRL, 135(14), 145001. (www)

  @article{ , abstract = {The acceleration of electrons by surface plasma waves (SPWs) generated during the interaction of ultrashort, linearly polarized, and contrast-enhanced laser pulses at a peak intensity of ∼ 6 × 10 20 W cm − 2 with flat, noncorrugated foils at parallel incidence (with respect to the target surface) is investigated. We experimentally demonstrate the generation of a collimated electron beam ( < 0.6 mrad ) with a non-Maxwellian spectrum, characterized by peaks at superponderomotive energies (30–36 MeV) and total charge ∼ 120 pC . Through particle-in-cell (PIC) simulations, we identify the J × B force at the front edge as the primary mechanism for injecting electrons into the SPW, where they are further accelerated. Furthermore, our simulation findings reveal that lateral surface contaminants influence SPW dynamics and give rise to a long-ranging plasmonic mode.}, archive = {J_PRL}, author = {A. McCay and A. McIlvenny and A. Macchi and L. Romagnani and P. Martin and O. Cavanagh and D. P. Molloy and L. Lancia and T. Dzelzainis and H. Ahmed and J. Sarma and S. Kar and D. Margarone and M. Borghesi}, doi = {10.1103/y29y-f63h}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {145001}, shortjournal = {Phys. Rev. Lett.}, title = {Surface wave electron acceleration from flat foils at parallel laser incidence}, volume = {135}, year = {2025}, }
• (2025). Drops can perpetually bounce over a vibrating wettable solid. PRL, 135(14), 144001. (www)

  @article{ , abstract = {On the surface of a vibrating liquid bath, instead of coalescing, a drop will continually bounce on a thin film of air between the drop and the free surface, giving rise to rich chaotic dynamics and quantum analog behavior. However, perpetual bouncing is yet to be demonstrated on a vibrating rigid solid, where the control of the drop’s motion is not limited by the bath dynamics. Here we show that vibration of an atomically smooth mica surface prolongs a drop’s hovering state by several orders of magnitude, increasing the time to wet from less than a second to several minutes. The excitation of the second spherical harmonic mode determines a transition between a bouncing state with high-amplitude rebounds, and a bound state, where the drop’s motion is locked onto the vibrating solid above a thin air layer. We further develop a coupled linear spring model, accounting for the drop’s deformation, that predicts bouncing trajectories without fitting parameters. Our results extend the scope of bouncing drop studies beyond the liquid bath and highlight the potential for precision manipulation of small liquid quantities in air.}, archive = {J_PRL}, author = {Lebo Molefe and Tomas Fullana and François Gallaire and John M. Kolinski}, doi = {10.1103/w3qq-cnj3}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {144001}, shortjournal = {Phys. Rev. Lett.}, title = {Drops can perpetually bounce over a vibrating wettable solid}, volume = {135}, year = {2025}, }
• (2025). Locking orbital angular momentum with linear momentum of light. PRL, 135(14), 143802. (www)

  @article{ , abstract = {Correlation between the propagation direction of light and spin can be induced via the spin-orbit interaction and has been proven to be the workhorse in the emerging field of chiral quantum optics and in the spin-related Hall effects of light. Photonic orbital angular momentum (OAM) provides a high-dimensional degree of freedom in classical and quantum information processing. However, integrated OAM-based information technology is an open challenge, because OAM modes are always generated in pairs with opposite topological charges due to their degeneracy. Here, we observe locking of the OAM and linear momentum of light by using a chiral optical waveguide with an Archimedean cross section to induce the orbit-orbit interaction. This OAM-momentum locking enables the deterministic and robust generation of on-demand OAM vortex light beam in a photonic chip. This new correlation paves the way toward exotic high-dimensional chiral physical effects and also provides the capability of on-chip manipulation of light in high-dimensional space.}, archive = {J_PRL}, author = {Hui-Ming Wang and Yuan Chen and Ming-Yuan Chen and Ying-Yu Fang and Ka-Di Zhu and Cheng-Wei Qiu and Yan-Qing Lu and Keyu Xia and Xian-Min Jin}, doi = {10.1103/tttd-v936}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {143802}, shortjournal = {Phys. Rev. Lett.}, title = {Locking orbital angular momentum with linear momentum of light}, volume = {135}, year = {2025}, }
• (2025). Nanoscale mirrorless superradiant lasing. PRL, 135(14), 143601. (www)

  @article{ , abstract = {We predict collective free-space lasing in a dense nanoscopic emitter arrangement where dipole-dipole coupled atomic emitters synchronize their emission and exhibit lasing behavior without the need for an optical resonator. At the example of a subwavelength-spaced linear emitter chain with varying fractions of pumped and unpumped emitters, we present a comprehensive study of this mirrorless lasing phenomenon. The total radiated power transitions from subradiant suppression under weak pumping to superradiant enhancement at stronger pumping, while exhibiting directional emission confined to a narrow spatial angle. At the same time multiple independent spectral emission lines below the lasing threshold merge toward a single narrow spectral line at high pump power. The most substantial enhancement and line narrowing occur when a fraction of unpumped atoms is present. We show that this leads to superradiant lasing near the bare atomic frequency, making the system a promising candidate for a minimalist active optical frequency reference.}, archive = {J_PRL}, author = {Anna Bychek and Raphael Holzinger and Helmut Ritsch}, doi = {10.1103/rbs2-2pd5}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {143601}, shortjournal = {Phys. Rev. Lett.}, title = {Nanoscale mirrorless superradiant lasing}, volume = {135}, year = {2025}, }
• (2025). Realization of a fast triple-magic all-optical qutrit in sr88. PRL, 135(14), 143401. (www)

  @article{ , abstract = {The optical clock states of alkaline earth and alkaline earthlike atoms are the fundament of state-of-the-art optical atomic clocks. An important prerequisite for the operation of optical clocks is the magic trapping conditions where electronic and motional dynamics decouple. Here, we identify and experimentally demonstrate simultaneous magic trapping for two clock transitions in Sr 88 , realizing so-called triple-magic conditions at a specially chosen magic angle. Under these conditions, we operate an all-optical qutrit comprising the ground state S 0 1 , and the two metastable clock states P 0 3 and P 2 3 . We demonstrate fast optical control in an atom array using two- and three-photon couplings to realize high-fidelity manipulation between all qutrit states. At the magic angle, we probe the coherence achievable in magic-angle-tuned traps and find atom-atom coherence times between the metastable states as long as 715(30) ms. Our work opens several new directions, including qutrit-based quantum metrology on optical transitions and high-fidelity and high-coherence manipulation on the Sr 88 fine-structure qubit.}, archive = {J_PRL}, author = {Maximilian Ammenwerth and Hendrik Timme and Flavien Gyger and Renhao Tao and Immanuel Bloch and Johannes Zeiher}, doi = {10.1103/4kdl-xcwz}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {143401}, shortjournal = {Phys. Rev. Lett.}, title = {Realization of a fast triple-magic all-optical qutrit in sr88}, volume = {135}, year = {2025}, }
• (2025). Study of the beta spectrum shape of rb92 and cs142 decays for the prediction of reactor antineutrino spectra. PRL, 135(14), 142502. (www)

  @article{ , abstract = {The shapes of the beta spectra of Rb 92 and Cs 142 , two of the beta decays most relevant for the prediction of the antineutrino spectrum in reactors, have been measured. A new setup composed of two Δ E − E telescopes has been used. High-purity radioactive beams of the isotopes of interest were provided by the IGISOL facility using the JYFLTRAP double Penning trap. The resulting beta spectra have been compared with model predictions using beta decay feedings from total absorption gamma spectroscopy measurements and shape corrections employed in the calculation of the antineutrino spectrum, corroborating both further. The procedure can be extended to other relevant nuclei in the future, providing solid ground for the prediction of the antineutrino spectrum in reactors.}, archive = {J_PRL}, author = {G. A. Alcalá and A. Algora and M. Estienne and M. Fallot and V. Guadilla and A. Beloeuvre and W. Gelletly and R. Kean and A. Porta and S. Bouvier and J.-S. Stutzmann and E. Bonnet and T. Eronen and D. Etasse and J. Agramunt and J. L. Tain and H. Garcia Cabrera and L. Giot and A. Laureau and J. A. Victoria and Y. Molla and A. Jaries and L. Al Ayoubi and O. Beliuskina and W. Gins and M. Hukkanen and A. Illana and A. Kankainen and S. Kujanpää and I. Moore and I. Pohjalainen and D. Pitman and A. Raggio and M. Reponen and J. Romero and J. Ruotsalainen and M. Stryjczyk and A. Tolosa and V. Virtanen}, doi = {10.1103/hyj7-l22h}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {142502}, shortjournal = {Phys. Rev. Lett.}, title = {Study of the beta spectrum shape of rb92 and cs142 decays for the prediction of reactor antineutrino spectra}, volume = {135}, year = {2025}, }
• (2025). Emulators for scarce and noisy data: Application to auxiliary-field diffusion monte carlo for neutron matter. PRL, 135(14), 142501. (www)

  @article{ , abstract = {Understanding the equation of state (EOS) of pure neutron matter is necessary for interpreting multimessenger observations of neutron stars. Reliable data analyses of these observations require well-quantified uncertainties for the EOS input, ideally propagating uncertainties from nuclear interactions directly to the EOS. This, however, requires calculations of the EOS for a prohibitively larger number of nuclear Hamiltonians, solving the nuclear many-body problem for each one. Quantum Monte Carlo methods, such as auxiliary-field diffusion Monte Carlo (AFDMC), provide precise and accurate results for the neutron matter EOS, but they are very computationally expensive, making them unsuitable for the fast evaluations necessary for uncertainty propagation. Here, we employ parametric matrix models to develop fast emulators for AFDMC calculations of neutron matter and use them to directly propagate uncertainties of coupling constants in the Hamiltonian to the EOS. As these uncertainties include estimates of the effective field theory truncation uncertainty, this approach provides robust uncertainty estimates for use in astrophysical data analyses. This Letter will enable novel applications such as using astrophysical observations to put constraints on coupling constants for nuclear interactions.}, archive = {J_PRL}, author = {Cassandra L. Armstrong and Pablo Giuliani and Kyle Godbey and Rahul Somasundaram and Ingo Tews}, doi = {10.1103/9928-wyjm}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {142501}, shortjournal = {Phys. Rev. Lett.}, title = {Emulators for scarce and noisy data: Application to auxiliary-field diffusion monte carlo for neutron matter}, volume = {135}, year = {2025}, }
• (2025). Precision CP symmetry test and polarization analysis in Σ+ decays. PRL, 135(14), 141804. (www)

  @article{ , abstract = {A stringent test of C P symmetry in hyperon decays is performed using 1.0 × 10 10 J / ψ events and 2.7 × 10 9 ψ ( 3686 ) events collected by the BESIII experiment. The C P asymmetry in the two-body nonleptonic weak decays Σ + → p π 0 and Σ ¯ − → p ¯ π 0 is determined to be A C P = − 0.0118 ± 0.0083 ( stat ) ± 0.0028 ( syst ) , consistent with C P conservation. The average decay parameter ⟨ α 0 ⟩ = − 0.9869 ± 0.0011 ( stat ) ± 0.0016 ( syst ) represents the most precise measurement in the baryon sector to date. A model-independent analysis of the hyperon polarization is performed for the first time at J / ψ and ψ ( 3686 ) resonances, revealing a clear sign reversal and offering new insight into SU(3) symmetry breaking and baryon internal structure. These results provide the most stringent constraints on C P violation in Σ decays and establish a benchmark for future precision studies.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Y. Y. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and F. M. Melendi and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and L. F. Tang and M. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/ysd5-s2gn}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {141804}, shortjournal = {Phys. Rev. Lett.}, title = {Precision CP symmetry test and polarization analysis in Σ+ decays}, volume = {135}, year = {2025}, }
• (2025). Entropy inequalities constrain holographic erasure correction. PRL, 135(14), 141603. (www)

  @article{ , abstract = {We interpret holographic entropy inequalities in terms of erasure correction. The nonsaturation of an inequality is a necessary condition for certain schemes of holographic erasure correction, manifested in the bulk as nonempty overlaps of corresponding entanglement wedges.}, archive = {J_PRL}, author = {Bartłomiej Czech and Sirui Shuai and Yixu Wang}, doi = {10.1103/dl3c-h3hg}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {141603}, shortjournal = {Phys. Rev. Lett.}, title = {Entropy inequalities constrain holographic erasure correction}, volume = {135}, year = {2025}, }
• (2025). Tidal resonance in binary neutron star inspirals: A high-precision study in numerical relativity. PRL, 135(14), 141403. (www)

  @article{ , abstract = {We investigate the tidal resonance of the fundamental ( f ) mode in spinning neutron stars, robustly tracing the onset of the excitation to its saturation, using numerical relativity for the first time. We performed long-term ( ≈ 15 orbits) fully relativistic simulations of a merger of two highly and retrogradely spinning neutron stars. The resonance window of the f mode is extended by self-interaction, and the nonlinear resonance continues up to the final plunging phase. We observe that the quasicircular orbit is maintained throughout since the dissipation of orbit motion due to the resonance is coherent with that due to gravitational waves. The f -mode resonance causes a variation in the stellar spin of ≳ 6.3 % in the linear regime and much more as ∼ 33 % during the later nonlinear regime. At the merger, a phase shift of ≲ 40 rad is rendered in the gravitational waveform as a consequence of the angular momentum and energy transfers into the neutron star oscillations.}, archive = {J_PRL}, author = {Hao-Jui Kuan and Kenta Kiuchi and Masaru Shibata}, doi = {10.1103/j3zk-z17h}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {141403}, shortjournal = {Phys. Rev. Lett.}, title = {Tidal resonance in binary neutron star inspirals: A high-precision study in numerical relativity}, volume = {135}, year = {2025}, }
• (2025). Indefinite causal order and quantum coordinates. PRL, 135(14), 141402. (www)

  @article{ , abstract = {Classically, the causal order of two timelike separated events A and B is fixed—either A before B or B before A . This is no longer true in quantum theory, where it is possible to encounter superpositions of causal orders. The quantum switch is one of the most prominent processes with indefinite causal order. Optical realizations of the quantum switch have been successfully implemented in experiments, but some argue that this merely simulates a process with indefinite causal order and that a superposition of spacetime metrics is required for a true realization. Here, we provide a relativistic definition of causal order between operationally defined events that defines a meaningful observable in both the general relativistic and quantum mechanical sense. Importantly, this observable does not distinguish between the indefinite causal order implemented on an optical bench and the gravitational quantum switch, a gedanken experiment where the indefinite causal order is achieved by a quantum superposition of gravitational fields. Therefore, our results support the thesis that the optical quantum switch is just as much a realization of indefinite causal order as its gravitational counterpart, which makes use of the quantum mechanical behavior of spacetime.}, archive = {J_PRL}, author = {Anne-Catherine de la Hamette and Viktoria Kabel and Marios Christodoulou and Časlav Brukner}, doi = {10.1103/bnkn-4p3f}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {141402}, shortjournal = {Phys. Rev. Lett.}, title = {Indefinite causal order and quantum coordinates}, volume = {135}, year = {2025}, }
• (2025). NuSTAR as an axion helioscope. PRL, 135(14), 141001. (www)

  @article{ , abstract = {We present a novel approach to investigating axions and axionlike particles by studying their potential conversion into x-rays within the Sun’s atmospheric magnetic field. Utilizing high-sensitivity data from the nuclear spectroscopic telescope array (NuSTAR) collected during the 2020 solar minimum, along with advanced solar atmospheric magnetic field models, we establish a new limit on the axion-photon coupling strength g a γ ≲ 7.3 × 10 − 12 GeV − 1 at 95% CL for axion masses m a ≲ 4 × 10 − 7 eV . This constraint surpasses current ground-based experimental limits, studying previously unexplored regions of the axion-photon coupling parameter space up to masses of m a ≲ 3.4 × 10 − 4 eV . These findings mark a significant advancement in our ability to probe axion properties and strengthen indirect searches for dark matter candidates.}, archive = {J_PRL}, author = {J. Ruz and E. Todarello and J. K. Vogel and F. R. Candón and M. Giannotti and B. Grefenstette and H. S. Hudson and I. G. Hannah and I. G. Irastorza and C. S. Kim and M. Regis and D. M. Smith and M. Taoso and J. Trujillo Bueno}, doi = {10.1103/18sn-hxtb}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {141001}, shortjournal = {Phys. Rev. Lett.}, title = {NuSTAR as an axion helioscope}, volume = {135}, year = {2025}, }
• (2025). Prepare-and-measure scenarios with photon-number constraints. PRL, 135(14), 140802. (www)

  @article{ , abstract = {We study correlations in the prepare-and-measure scenario when quantum communication is constrained by photon-number statistics. Such constraints are natural and practical control parameters for semi-device-independent certification in optical platforms. To analyse these scenarios, we show how semidefinite programming relaxations for noncommutative polynomial optimization can be used to bound the set of quantum correlations under restrictions on the photon-number distribution. The practicality of this method is demonstrated by computing optimal performance bounds on several well-known communication tasks. We then apply the method to the certification of semi-device-inpependent random number generation protocols and show how to bound the conditional Shannon entropy. We showcase this versatile tool by improving randomness extraction in established protocols based on coherent states and homodyne measurements.}, archive = {J_PRL}, author = {Carles Roch i Carceller and Jef Pauwels and Stefano Pironio and Armin Tavakoli}, doi = {10.1103/glty-kkbp}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {140802}, shortjournal = {Phys. Rev. Lett.}, title = {Prepare-and-measure scenarios with photon-number constraints}, volume = {135}, year = {2025}, }
• (2025). Heisenberg-limited quantum metrology without ancillae. PRL, 135(14), 140801. (www)

  @article{ , abstract = {Extensive research has been dedicated to the asymptotic theory of quantum metrology, where the goal is to determine the ultimate precision limit of quantum channel estimation when many accesses to the channel are allowed. The ultimate limit has been well established, but in general, a noiseless and controllable ancilla is required for attaining it. Little is known about the metrological performance without noiseless ancillae, which is more relevant in practical circumstances. In this Letter, we present a novel theoretical framework to address this problem, bridging quantum metrology and the asymptotic theory of quantum channels. Leveraging this framework, we prove sufficient conditions for achieving the Heisenberg limit with repeated applications of the channel to be estimated both with and without applying interleaved unitary control operations. For the latter case, we design an algorithm to identify the control operation explicitly.}, archive = {J_PRL}, author = {Qiushi Liu and Yuxiang Yang}, doi = {10.1103/vmd7-twd5}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {140801}, shortjournal = {Phys. Rev. Lett.}, title = {Heisenberg-limited quantum metrology without ancillae}, volume = {135}, year = {2025}, }
• (2025). General approach to error detection of bosonic codes via phase estimation. PRL, 135(14), 140603. (www)

  @article{ , abstract = {We present a general approach to error detection of bosonic quantum error-correction codes via an adaptive quantum phase estimation algorithm assisted by a single ancilla qubit. The approach is applicable to a broad class of bosonic codes whose error syndromes are described by symmetry or stabilizer operators, including the rotation-symmetric codes and Gottesman-Kitaev-Preskill (GKP) codes. The detection precision scales inversely with the total evolution time and thus reaches the Heisenberg limit. We numerically demonstrate the approach for several examples, such as detecting bosonic excitation loss errors in high-order cat or binomial codes and displacement errors in finite-energy GKP codes. We also extend the approach to efficiently generate arbitrary Fock states. Our schemes are feasible in present-day experiments.}, archive = {J_PRL}, author = {Yuan-De Jin and Shi-Yu Zhang and Ulrik L. Andersen and Wen-Long Ma}, doi = {10.1103/h6rv-hz81}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {140603}, shortjournal = {Phys. Rev. Lett.}, title = {General approach to error detection of bosonic codes via phase estimation}, volume = {135}, year = {2025}, }
• (2025). Tessellation codes: Encoded quantum gates by geometric rotation. PRL, 135(14), 140602. (www)

  @article{ , abstract = {We utilize the symmetry groups of regular tessellations on two-dimensional surfaces of different constant curvatures, including spheres, Euclidean planes, and hyperbolic planes to encode a qubit or qudit into the physical degrees of freedom on these surfaces, which we call tessellation codes. We show that tessellation codes exhibit decent error correction properties by analysis via geometric considerations and the representation theory of the isometry groups on the corresponding surfaces. Interestingly, we demonstrate how this formalism enables the implementation of certain logical operations through geometric rotations of surfaces in real space, opening a new approach to logical quantum computation. We provide a variety of concrete constructions of such codes associated with different tessellations, which give rise to different logical groups. This formalism sheds a new light on quantum code and logical operation construction.}, archive = {J_PRL}, author = {Yixu Wang and Yijia Xu (许逸葭 and Zi-Wen Liu}, doi = {10.1103/tljb-f7tt}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {140602}, shortjournal = {Phys. Rev. Lett.}, title = {Tessellation codes: Encoded quantum gates by geometric rotation}, volume = {135}, year = {2025}, }
• (2025). Pontus-mpemba effects. PRL, 135(14), 140404. (www)

  @article{ , abstract = {Mpemba effects occur after a sudden quench of control parameters if, for “far” (or “hot”) initial states with respect to a final target state, the relaxation time toward the target state is shorter than for “close” (or “cold”) initial states. Following a strategy of fishermen in Pontus described by Aristotle, we introduce the Pontus-Mpemba effect as a two-step protocol that includes the time needed for preparing the system in the “far” initial state that can now be an arbitrary nonequilibrium state. Our protocol needs no parameter distance concept and applies to general (classical or quantum) systems. We find that all possible Pontus-Mpemba effects fall into three classes and illustrate the theory for open Markovian two-state quantum systems.}, archive = {J_PRL}, author = {Andrea Nava and Reinhold Egger}, doi = {10.1103/hhgj-89gj}, journal = {Physical Review Letters}, month = {10}, number = {14}, pages = {140404}, shortjournal = {Phys. Rev. Lett.}, title = {Pontus-mpemba effects}, volume = {135}, year = {2025}, }
• (2025). Charging dynamics of electric double-layer nanocapacitors in mean field. PRL, 135(14), 148002. (www)

  @article{ , abstract = {An electric double-layer capacitor (EDLC) stores energy by modulating the spatial distribution of ions in the electrolytic solution that it contains. We determine the mean-field timescales for planar EDLC relaxation to equilibrium after a potential difference is applied. We tackle first the fully symmetric case, where positive and negative ionic species have the same valence and diffusivity, and then the general, more complex, asymmetric case. Depending on the applied voltage and salt concentration, different regimes appear, revealing a remarkably rich phenomenology relevant for nanocapacitors.}, archive = {J_PRL}, author = {Ivan Palaia and Adelchi J. Asta and Megh Dutta and Patrick B. Warren and Benjamin Rotenberg and Emmanuel Trizac}, doi = {10.1103/72b9-c8cq}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {148002}, shortjournal = {Phys. Rev. Lett.}, title = {Charging dynamics of electric double-layer nanocapacitors in mean field}, volume = {135}, year = {2025}, }
• (2025). Memory kernel coupling theory: Obtaining time correlation function from higher-order moments. PRL, 135(14), 148001. (www)

  @article{ , abstract = {Dynamical observables can often be described by time correlation functions (TCFs). However, efficiently calculating TCFs for complex quantum systems is a significant challenge, which generally requires solving the full dynamics of the systems. This Letter presents the memory kernel coupling theory (MKCT), a general formalism for evaluating TCFs. The MKCT builds upon Mori’s memory kernel formalism for TCFs. Our theory further decomposes the memory kernel into auxiliary kernels. Rapid decay of auxiliary kernels allows us to truncate the coupled equations of motion with high accuracy. Notably, only higher-order moments are sufficient as the input for obtaining TCFs. While this formalism is general, we carry out the numerical demonstration for typical open quantum systems—the spin-boson model and the single impurity Anderson model.}, archive = {J_PRL}, author = {Wei Liu and Yu Su and Yao Wang and Wenjie Dou}, doi = {10.1103/qvd5-5z6m}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {148001}, shortjournal = {Phys. Rev. Lett.}, title = {Memory kernel coupling theory: Obtaining time correlation function from higher-order moments}, volume = {135}, year = {2025}, }
• (2025). Pushing photons with electrons: Observation of the polariton drag effect. PRL, 135(14), 146903. (www)

  @article{ , abstract = {We show the direct effect of free electrons colliding with polaritons, changing their momentum. The result of this interaction of the electrons with the polaritons is a change in the angle of emission of the photons from our cavity structure. Because the experiment is a photon-in, photon-out system, this is equivalent to optical beam steering of photons using a direct electrical current. The effect is asymmetric, significantly slowing down the polaritons when they move oppositely to the electrons, while the polariton momentum only slightly increases when the electrons move in the same direction. We present a theoretical model which describes this effect.}, archive = {J_PRL}, author = {D. M. Myers and Q. Yao and H. Alnatah and S. Mukherjee and B. Ozden and J. Beaumariage and L. N. Pfeiffer and K. West and D. W. Snoke}, doi = {10.1103/fb2r-qdq7}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146903}, shortjournal = {Phys. Rev. Lett.}, title = {Pushing photons with electrons: Observation of the polariton drag effect}, volume = {135}, year = {2025}, }
• (2025). Strongly entangled kondo and kagome lattices and the emergent magnetic ground state in heavy-fermion kagome metal YbV6Sn6. PRL, 135(14), 146902. (www)

  @article{ , abstract = {Applying angle-resolved photoemission spectroscopy and density functional theory calculations, we present compelling spectroscopic evidence demonstrating the intertwining and mutual interaction between the Kondo and kagome sublattices in heavy-fermion intermetallic compound YbV 6 Sn 6 . We reveal the Yb 4 f -derived states near the Fermi level, along with the presence of bulk kagome bands and topological surface states. We unveil strong interactions between the 4 f and itinerant electrons, where the kagome bands hosting the Dirac fermions and van Hove singularities predominate. Such findings are well described using a c − f hybridization model. On the other hand, our systematic characterization of magnetic properties demonstrates an unusually enhanced antiferromagnetic ordering, where the kagome-derived van Hove singularities near E F play a vital role in determining the unconventional nature of the Ruderman-Kittel-Kasuya-Yosida interaction and Kondo coupling. These unique kagome-state-mediated exchange interactions have never been reported before and could lead to a novel phase diagram and various quantum critical behaviors in YbV 6 Sn 6 and its siblings. Our results not only expand the family of exotic quantum phases entangled with kagome structure to the strongly correlated regime, but also establish YbV 6 Sn 6 as an unprecedented platform to explore unconventional many-body physics beyond the standard Kondo picture.}, archive = {J_PRL}, author = {Rui Lou and Max Mende and Riccardo Vocaturo and Hao Zhang and Qingxin Dong and Man Li and Pengfei Ding and Erjian Cheng and Zhiguang Liao and Yu Zhang and Junfa Lin and Reza Firouzmandi and Vilmos Kocsis and Laura T. Corredor and Yurii Prots and Oleksandr Suvorov and Anupam Jana and Jun Fujii and Ivana Vobornik and Oleg Janson and Wenliang Zhu and Jeroen van den Brink and Cornelius Krellner and Minghu Pan and Bosen Wang and Tianlong Xia and Jinguang Cheng and Shancai Wang and Claudia Felser and Bernd Büchner and Sergey Borisenko and Rong Yu and Denis V. Vyalikh and Alexander Fedorov}, doi = {10.1103/sqbn-vtcj}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146902}, shortjournal = {Phys. Rev. Lett.}, title = {Strongly entangled kondo and kagome lattices and the emergent magnetic ground state in heavy-fermion kagome metal YbV6Sn6}, volume = {135}, year = {2025}, }
• (2025). Terahertz-induced tunnel ionization drives coherent raman-active phonon in bismuth. PRL, 135(14), 146901. (www)

  @article{ , abstract = {Driving coherent lattice motion with THz pulses has emerged as a novel pathway for achieving dynamic stabilization of exotic phases that are inaccessible in equilibrium quantum materials. In this Letter, we present a previously unexplored mechanism for THz excitation of Raman-active phonons. We show that intense THz pulses centered at 1 THz can excite the Raman-active A 1 g phonon mode at 2.9 THz in a bismuth film. We rule out the possibilities of the phonon being excited through conventional anharmonic coupling to other modes or via a THz sum frequency process. Instead, we demonstrate that the THz-driven tunnel ionization provides a plausible means of creating a displacive driving force to initiate the phonon oscillations. Our Letter highlights a new mechanism for exciting coherent phonons, offering potential for dynamic control over the electronic and structural properties of semimetals and narrow-band semiconductors on ultrafast timescales.}, archive = {J_PRL}, author = {Bing Cheng and Patrick L. Kramer and Mariano Trigo and Mengkun Liu and Ctirad Uher and David A. Reis and Zhi-Xun Shen and Jonathan A. Sobota and Matthias. C. Hoffmann}, doi = {10.1103/ttwf-qgz4}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146901}, shortjournal = {Phys. Rev. Lett.}, title = {Terahertz-induced tunnel ionization drives coherent raman-active phonon in bismuth}, volume = {135}, year = {2025}, }
• (2025). Anyon braiding on the single edge of a fractional quantum hall state. PRL, 135(14), 146601. (www)

  @article{ , abstract = {Anyons are quasiparticles with fractional statistics, bridging between fermions and bosons. We propose an experimental setup to measure the statistical angle of topological anyons emitted from a quantum point contact (QPC) source. The setup involves an Ω -shaped junction along a fractional quantum Hall liquid edge, formed by defining a droplet with two negatively biased gates. In the weak tunneling regime, we calculate the charge current, showing its time evolution depends solely on the anyons’ statistical properties, with temperature and scaling dimension affecting only the constant prefactor. We compute the cross-correlation between the anyon current transmitted from the source and the current after the Ω junction, providing a direct method to detect anyon braiding statistics.}, archive = {J_PRL}, author = {Flavio Ronetti and Noé Demazure and Jérôme Rech and Thibaut Jonckheere and Benoît Grémaud and Laurent Raymond and Masayuki Hashisaka and Takeo Kato and Thierry Martin}, doi = {10.1103/yq1x-kxgm}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146601}, shortjournal = {Phys. Rev. Lett.}, title = {Anyon braiding on the single edge of a fractional quantum hall state}, volume = {135}, year = {2025}, }
• (2025). Spin transport revealed by spin quantum geometry. PRL, 135(14), 146303. (www)

  @article{ , abstract = {We present the framework of spin quantum geometry, which is fundamentally linked to the spin degree of freedom of Bloch electrons and incorporates both the spin quantum geometric tensor (QGT) and the recently introduced Zeeman QGT, to elucidate spin transport. We show that the spin and Zeeman QGTs, respectively, provide a unified framework for revealing known spin currents, such as the intrinsic spin Hall effect, and spin magnetization, such as the Edelstein effect, of Bloch electrons under an electric field. In addition, we predict the linear displacement spin Hall effect, wherein an ac electric field induces a transverse spin current in insulating systems. Furthermore, we propose two novel nonlinear spin responses: the nonlinear Drude spin current (NDSC) and the nonlinear Drude spin magnetization (NDSM), both of which exhibit a quadratic dependence on the relaxation time, like the nonlinear Drude charge current, and are governed by spin quantum geometry. Finally, we evaluate the NDSC and NDSM with Dirac models of topological insulators and find that, in the moderately dirty regime, the NDSC and NDSM can exceed their respective nonlinear intrinsic counterparts, which have recently garnered significant interest in spintronics.}, archive = {J_PRL}, author = {Longjun Xiang and Hao Jin and Jian Wang}, doi = {10.1103/14mp-263q}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146303}, shortjournal = {Phys. Rev. Lett.}, title = {Spin transport revealed by spin quantum geometry}, volume = {135}, year = {2025}, }
• (2025). Multipolar fermi surface deformations in Sr2RuO4 probed by resistivity and sound attenuation: A window into electron viscosity and the collision operator. PRL, 135(14), 146302. (www)

  @article{ , abstract = {Recent developments in electron hydrodynamics have demonstrated the importance of considering the full structure of the electron-electron scattering operator, which encodes a sequence of lifetimes, one for each component of the Fermi surface deformation in a multipolar expansion. In this context, the dipolar lifetime is measured by resistivity, whereas the quadrupolar component probes the viscosity and can be measured in the bulk via sound attenuation. We introduce a framework to extract the collision operator of an arbitrary metal by combining resistivity and sound attenuation measurements with a realistic calculation of the scattering operator that includes multiband and umklapp effects. The collision operator allows for the prediction of a plethora of properties, including the nonlocal conductivity, and can be used to predict hydrodynamic behavior for bulk metals. As a first application, we apply this framework to Sr 2 RuO 4 in a temperature range where electron-electron scattering is dominant. We find quantitative agreement between our model and the temperature dependence of both the resistivity and the sound attenuation, we find the quadrupolar ( B 1 g ) relaxation rate to be 30% higher than the dipolar one due to the presence of hot spots on the γ band, and we predict a strongly anisotropic viscosity arising from the α and β bands.}, archive = {J_PRL}, author = {Davis Thuillier and Sayak Ghosh and B. J. Ramshaw and Thomas Scaffidi}, doi = {10.1103/2fcg-zmwt}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146302}, shortjournal = {Phys. Rev. Lett.}, title = {Multipolar fermi surface deformations in Sr2RuO4 probed by resistivity and sound attenuation: A window into electron viscosity and the collision operator}, volume = {135}, year = {2025}, }
• (2025). Exchange interaction in an InSb quantum well measured with landau-level tunneling spectroscopy. PRL, 135(14), 146301. (www)

  @article{ , abstract = {We studied InSb quantum well devices using Landau-level tunneling spectroscopy through a three-terminal differential conductance technique. This method is similar to filled-state scanning tunneling microscopy but uses a stationary contact instead of a mobile tip to analyze the two-dimensional electron system. Applying magnetic fields up to 15 T, we identified clear peaks in the differential current-voltage profiles, indicative of Landau-level formation. By examining deviations from the expected Landau fan diagram, we extract an absolute value for the exchange-induced energy shift. Through an empirical analysis, we derive a formula describing the exchange shift as a function of both magnetic field strength and electron filling. Our findings indicate that the emptying of the ν = 2 and ν = 3 Landau levels causes an exchange interaction energy shift in the ν = 1 level. Unlike prior studies that infer level energies relative to one another and report oscillatory g -factor behavior, our method references the energy of the Landau levels above the filled states of the contact under a bias voltage, revealing that only the ground state Landau level experiences a measurable exchange shift.}, archive = {J_PRL}, author = {S. K. Clowes and C. P. Allford and D. Shearer and G. V. Smith and R. Simmons and B. N. Murdin and U. Zeitler and P. D. Buckle}, doi = {10.1103/rr3f-3zhd}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146301}, shortjournal = {Phys. Rev. Lett.}, title = {Exchange interaction in an InSb quantum well measured with landau-level tunneling spectroscopy}, volume = {135}, year = {2025}, }
• (2025). No time for surface charge: How bulk conductivity hides charge patterns from kelvin probe force microscopy in contact-electrified surfaces. PRL, 135(14), 146202. (www)

  @article{ , abstract = {Kelvin probe force microscopy (KPFM) is widely used in stationary and dynamic studies of contact electrification. An obvious question that connects these two has been overlooked: when are charge dynamics too fast for stationary studies to be meaningful? Using a rapid transfer system to quickly perform KPFM after contact, we find the dynamics are too fast in all but the best insulators. Our data further suggest that dynamics are caused by bulk as opposed to surface conductivity, and that charge-transfer heterogeneity is less prevalent than previously suggested.}, archive = {J_PRL}, author = {Felix Pertl and Isaac C. D. Lenton and Tobias Cramer and Scott Waitukaitis}, doi = {10.1103/lcsm-xxty}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146202}, shortjournal = {Phys. Rev. Lett.}, title = {No time for surface charge: How bulk conductivity hides charge patterns from kelvin probe force microscopy in contact-electrified surfaces}, volume = {135}, year = {2025}, }
• (2025). Machine learning the energetics of electrified solid-liquid interfaces. PRL, 135(14), 146201. (www)

  @article{ , abstract = {We present a response-augmented machine-learning (ML) approach to the energetics of electrified metal surfaces. We leverage local descriptors to learn the work function as the first-order energy change to introduced bias charges and stabilize this learning through Born effective charges. This permits the efficient extension of ML interatomic potential architectures to include finite bias effects up to second order. Application to OH at Cu(100) rationalizes the experimentally observed p H dependence of the preferred adsorption site in terms of a non-Nernstian charge-induced site switching.}, archive = {J_PRL}, author = {Nicolas Bergmann and Nicéphore Bonnet and Nicola Marzari and Karsten Reuter and Nicolas G. Hörmann}, doi = {10.1103/lm64-m3bn}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146201}, shortjournal = {Phys. Rev. Lett.}, title = {Machine learning the energetics of electrified solid-liquid interfaces}, volume = {135}, year = {2025}, }
• (2025). Handedness selection and hysteresis of chiral orders in crystals. PRL, 135(14), 146102. (www)

  @article{ , abstract = {A phase transition can drive the spontaneous emergence of chiral orders in crystals below a critical temperature. However, selecting either a right- or a left-handed phase with the aid of electromagnetic fields is challenging, particularly when intrinsic polar and axial moments are lacking. In this Letter, we show that purely chiral phases with opposite handedness, when both deriving from one degenerate instability, are linked by accessible transition states. While these states compete with the chirality under an electromagnetic field, a circularly polarized source can select the handedness of the system. This selection is mediated by a chiral monopole and may further result in a hysteresis process of the gyrotropic properties, namely, the optical activity, below the critical temperature. We suggest several materials, among which K 3 NiO 2 , as candidates for possible experimental observation.}, archive = {J_PRL}, author = {Mauro Fava and Aldo H. Romero and Eric Bousquet}, doi = {10.1103/c4v9-nd4b}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {146102}, shortjournal = {Phys. Rev. Lett.}, title = {Handedness selection and hysteresis of chiral orders in crystals}, volume = {135}, year = {2025}, }
• (2025). Observation of two-dimensional branched flow of light. PRL, 135(14), 143801. (www)

  @article{ , abstract = {We present an experimental study on light propagation within a bulk material, wherein a controlled, weakly disordered, three-dimensional spatial fluctuation of the refractive index is induced. We find that the random, varying potential splits a broad wave into a stable, two-dimensional (2D) caustic network, which persists over extended evolution distance. This network remains stable until 2D branched light flow emerges from the interconnection spots of the network. We thus demonstrate the first-ever observation of the stable two-dimensional branched flow of light and experimentally identify the fundamental length scale at which the two-dimensional branching initiates, as well as its power-law dependence on the correlation length and the strength of the random potential.}, archive = {J_PRL}, author = {Yan Liu and Ke Lin and Zhaoyu Liu and Jianwei Qin and Qidong Fu and Peng Wang and Fangwei Ye}, doi = {10.1103/gyqw-d17z}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {143801}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of two-dimensional branched flow of light}, volume = {135}, year = {2025}, }
• (2025). Partial-wave resolved spin-orbit dynamics. PRL, 135(14), 143201. (www)

  @article{ , abstract = {A novel projective measurement technique utilizing conventional photoelectron velocity-map imaging to probe the spatial part of the wave function by projecting it into momentum space is demonstrated. Oscillations between the states | m l = 0 , m s = ± 1 / 2 ⟩ and | m l = ± 1 , m s = ∓ 1 / 2 ⟩ are observed with no detectable decoherence over 170 cycles with a speed of around 1.7 THz driven purely by spin-orbit interaction. Our measurements achieve a quantum operation fidelity of approximately 90%, limited by the photoionization detection scheme. This Letter establishes a new platform for high-fidelity quantum operations driven by the intrinsic spin-orbit coupling.}, archive = {J_PRL}, author = {Wankai Li and Jingxuan Zhang and Yang Jin and Dongdong Zhang and Dajun Ding and Kiyoshi Ueda}, doi = {10.1103/lbw1-kwd5}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {143201}, shortjournal = {Phys. Rev. Lett.}, title = {Partial-wave resolved spin-orbit dynamics}, volume = {135}, year = {2025}, }
• (2025). Quarkonium spectroscopy in the quark-gluon plasma. PRL, 135(14), 142302. (www)

  @article{ , abstract = {The properties of bound states are fundamental to hadronic spectroscopy and play a central role in the transition from hadronic matter to a quark-gluon plasma (QGP). In a strongly coupled QGP (sQGP), the interplay of temperature, binding energy, and large collisional widths of the partons poses formidable challenges in evaluating the in-medium properties of hadronic states and their eventual melting. In particular, the existence of heavy quarkonia in the QGP is a long-standing problem that is hard to solve by considering their spectral properties on the real-energy axis. We address this problem by analyzing in-medium thermodynamic quarkonium T matrices in the complex energy plane. We first validate this method in vacuum, where the T -matrix poles of observed states are readily identified. When deploying this approach to recent self-consistently calculated T matrices in the QGP, we find that poles in the complex energy plane can persist to surprisingly large temperatures, depending on the strength of the in-medium interactions. While the masses and widths of the pole positions are precisely defined, the notion of a binding energy is not due to the absence of thresholds caused by the (large) widths of the underlying quark or anti-quark spectral functions. Our method thus provides a new and definitive quantum-mechanical criterion to determine the melting temperature of hadronic states in the sQGP while increasing the accuracy in the theoretical determination of transport parameters.}, archive = {J_PRL}, author = {Zhanduo Tang and Biaogang Wu and Andrew Hanlon and Swagato Mukherjee and Peter Petreczky and Ralf Rapp}, doi = {10.1103/7zby-gy46}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {142302}, shortjournal = {Phys. Rev. Lett.}, title = {Quarkonium spectroscopy in the quark-gluon plasma}, volume = {135}, year = {2025}, }
• (2025). Precision measurement of net-proton-number fluctuations in Au+Au collisions at RHIC. PRL, 135(14), 142301. (www)

  @article{ , abstract = {We report precision measurements on cumulants ( C n ) and factorial cumulants ( κ n ) of (net) proton number distributions up to fourth order in Au + Au collisions over center-of-mass energies s N N = 7.7 – 27 GeV from phase II of the Beam Energy Scan program at RHIC. (Anti)protons are selected at midrapidity ( | y | < 0.5 ) within a transverse momentum range of 0.4 < p T < 2.0 GeV / c . Relative to various noncritical-point model calculations and peripheral collision 70%–80% data, the net proton C 4 / C 2 measurement in 0%–5% collisions shows a minimum around 19.6 GeV for significance of deviation at ∼ 2 – 5 σ . A minimum in C 4 / C 2 with respect to a noncritical baseline is expected to be a characteristic feature of the signature associated with a critical point in the QCD phase diagram. In addition, deviations from noncritical baselines around the same collision energy region are also seen in proton factorial cumulant ratios, especially in κ 2 / κ 1 and κ 3 / κ 1 . Dynamical model calculations including a critical point are called for in order to understand these precision measurements.}, archive = {J_PRL}, author = {STAR Collaboration and B. E. Aboona and J. Adam and L. Adamczyk and I. Aggarwal and M. M. Aggarwal and Z. Ahammed and A. K. Alshammri and E. C. Aschenauer and S. Aslam and J. Atchison and V. Bairathi and X. Bao and K. Barish and S. Behera and R. Bellwied and P. Bhagat and A. Bhasin and S. Bhatta and S. R. Bhosale and J. Bielcik and J. Bielcikova and J. D. Brandenburg and C. Broodo and X. Z. Cai and H. Caines and M. Calderón de la Barca Sánchez and D. Cebra and J. Ceska and I. Chakaberia and P. Chaloupka and B. K. Chan and Z. Chang and A. Chatterjee and D. Chen and J. Chen and J. H. Chen and Q. Chen and Z. Chen and J. Cheng and Y. Cheng and W. Christie and X. Chu and S. Corey and H. J. Crawford and M. Csanád and G. Dale-Gau and A. Das and I. M. Deppner and A. Deshpande and A. Dhamija and A. Dimri and P. Dixit and X. Dong and J. L. Drachenberg and E. Duckworth and J. C. Dunlop and J. Engelage and G. Eppley and S. Esumi and O. Evdokimov and O. Eyser and R. Fatemi and S. Fazio and Y. Feng and E. Finch and Y. Fisyak and F. A. Flor and C. Fu and T. Fu and C. A. Gagliardi and T. Galatyuk and T. Gao and F. Geurts and N. Ghimire and A. Gibson and K. Gopal and X. Gou and D. Grosnick and A. Gu and A. Gupta and W. Guryn and A. Hamed and R. J. Hamilton and X. Han and S. Harabasz and M. D. Harasty and J. W. Harris and H. Harrison-Smith and L. B. Havener and X. H. He and Y. He and N. Herrmann and L. Holub and C. Hu and Q. Hu and Y. Hu and H. Huang and H. Z. Huang and S. L. Huang and T. Huang and Y. Huang and T. J. Humanic and M. Isshiki and W. W. Jacobs and A. Jalotra and C. Jena and A. Jentsch and Y. Ji and J. Jia and C. Jin and N. Jindal and X. Ju and E. G. Judd and S. Kabana and D. Kalinkin and K. Kang and D. Kapukchyan and K. Kauder and D. Keane and M. Kesler and A. Khanal and Y. V. Khyzhniak and D. P. Kikoła and J. Kim and D. Kincses and I. Kisel and A. Kiselev and A. G. Knospe and J. Kołaś and B. Korodi and L. K. Kosarzewski and L. Kumar and M. C. Labonte and R. Lacey and J. M. Landgraf and C. Larson and J. Lauret and A. Lebedev and J. H. Lee and Y. H. Leung and C. Li and D. Li and H-S. Li and H. Li and W. Li and X. Li and Y. Li and Z. Li and X. Liang and Y. Liang and R. Licenik and T. Lin and Y. Lin and M. A. Lisa and C. Liu and G. Liu and H. Liu and L. Liu and Z. Liu and T. Ljubicic and O. Lomicky and R. S. Longacre and E. M. Loyd and T. Lu and J. Luo and X. F. Luo and L. Ma and R. Ma and Y. G. Ma and N. Magdy and D. Mallick and R. Manikandhan and S. Margetis and C. Markert and O. Matonoha and O. Mezhanska and K. Mi and S. Mioduszewski and B. Mohanty and B. Mondal and M. M. Mondal and I. Mooney and J. Mrazkova and M. I. Nagy and C. J. Naim and A. S. Nain and J. D. Nam and M. Nasim and H. Nasrulloh and D. Neff and J. M. Nelson and M. Nie and G. Nigmatkulov and T. Niida and T. Nonaka and G. Odyniec and A. Ogawa and S. Oh and K. Okubo and B. S. Page and S. Pal and A. Pandav and A. Panday and A. K. Pandey and T. Pani and A. Paul and S. Paul and D. Pawlowska and C. Perkins and J. Pluta and B. R. Pokhrel and I. D. Ponce Pinto and M. Posik and E. Pottebaum and S. Prodhan and T. L. Protzman and A. Prozorov and V. Prozorova and N. K. Pruthi and M. Przybycien and J. Putschke and Z. Qin and H. Qiu and C. Racz and S. K. Radhakrishnan and A. Rana and R. L. Ray and R. Reed and C. W. Robertson and M. Robotkova and M. A. Rosales Aguilar and D. Roy and P. Roy Chowdhury and L. Ruan and A. K. Sahoo and N. R. Sahoo and H. Sako and S. Salur and S. S. Sambyal and J. K. Sandhu and S. Sato and B. C. Schaefer and N. Schmitz and F-J. Seck and J. Seger and R. Seto and P. Seyboth and N. Shah and P. V. Shanmuganathan and T. Shao and M. Sharma and N. Sharma and R. Sharma and S. R. Sharma and A. I. Sheikh and D. Shen and D. Y. Shen and K. Shen and S. Shi and Y. Shi and F. Si and J. Singh and S. Singha and P. Sinha and M. J. Skoby and N. Smirnov and Y. Söhngen and Y. Song and T. D. S. Stanislaus and M. Stefaniak and Y. Su and M. Sumbera and X. Sun and Y. Sun and B. Surrow and M. Svoboda and Z. W. Sweger and A. C. Tamis and A. H. Tang and Z. Tang and T. Tarnowsky and J. H. Thomas and A. R. Timmins and D. Tlusty and T. Todoroki and D. Torres Valladares and S. Trentalange and P. Tribedy and S. K. Tripathy and T. Truhlar and B. A. Trzeciak and O. D. Tsai and C. Y. Tsang and Z. Tu and J. Tyler and T. Ullrich and D. G. Underwood and G. Van Buren and J. Vanek and I. Vassiliev and F. Videbæk and S. A. Voloshin and F. Wang and G. Wang and J. S. Wang and J. Wang and K. Wang and X. Wang and Y. Wang and Z. Wang and A. J. Watroba and J. C. Webb and P. C. Weidenkaff and G. D. Westfall and D. Wielanek and H. Wieman and G. Wilks and S. W. Wissink and R. Witt and C. P. Wong and J. Wu and X. Wu and Wu X and B. Xi and Z. G. Xiao and G. Xie and W. Xie and H. Xu and N. Xu and Q. H. Xu and Y. Xu and Z. Xu and G. Yan and Z. Yan and C. Yang and Q. Yang and S. Yang and Y. Yang and Z. Ye and L. Yi and Y. Yu and H. Zbroszczyk and W. Zha and C. Zhang and D. Zhang and J. Zhang and S. Zhang and W. Zhang and X. Zhang and Y. Zhang and Z. Zhang and F. Zhao and J. Zhao and M. Zhao and S. Zhou and Y. Zhou and X. Zhu and M. Zurek and M. Zyzak}, doi = {10.1103/9l69-2d7p}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {142301}, shortjournal = {Phys. Rev. Lett.}, title = {Precision measurement of net-proton-number fluctuations in Au+Au collisions at RHIC}, volume = {135}, year = {2025}, }
• (2025). Dark-Matter–Electron detectors for dark-Matter–Nucleon interactions. PRL, 135(14), 141803. (www)

  @article{ , abstract = {In a seminal paper now a decade old, it was shown that dark-matter detectors geared at probing interactions with nucleons could also be used to probe dark-matter interactions with electrons. In this Letter, we show that new detector concepts designed to probe dark-matter–electron interactions at low masses can similarly be used to probe new parameter space for dark-matter–nucleon interactions. We demonstrate the power of this approach by using existing data from superconducting detectors to place new limits on the interactions of nuclei with MeV-scale dark matter. Further, we show that advances in detector technology that have been anticipated for electronic interactions will automatically extend sensitivity deep into uncharted territory for nuclear interactions. This doubles the effective science output of future low-threshold experiments.}, archive = {J_PRL}, author = {Sinéad M. Griffin and Guy Daniel Hadas and Yonit Hochberg and Katherine Inzani and Benjamin V. Lehmann}, doi = {10.1103/6qqv-rl7q}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141803}, shortjournal = {Phys. Rev. Lett.}, title = {Dark-Matter–Electron detectors for dark-Matter–Nucleon interactions}, volume = {135}, year = {2025}, }
• (2025). Higgs self-coupling at the future circular e+e− collider. PRL, 135(14), 141802. (www)

  @article{ , abstract = {Single Higgs production at FCC-ee probes the Higgs self-coupling at next-to-leading order (NLO). Extracting a bound requires a global analysis accounting for other possible new physics contributions up to NLO. We determine the FCC-ee sensitivity to Higgs self-coupling modifications δ κ λ within the standard model effective field theory framework, including for the first time flavor, LEP, LHC, and FCC-ee observables in a global analysis with all leading NLO effects via one-loop renormalization group evolution, as well as incorporating finite NLO contributions to electroweak precision and Z H observables. The global sensitivity to δ κ λ is estimated by marginalizing over the effects of all other operators, bringing flavor considerations to the fore. We find that, under reasonable assumptions, FCC-ee sensitivity to δ κ λ can exceed that of the HL-LHC.}, archive = {J_PRL}, author = {Victor Maura and Ben A. Stefanek and Tevong You}, doi = {10.1103/wjcy-1qk6}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141802}, shortjournal = {Phys. Rev. Lett.}, title = {Higgs self-coupling at the future circular e+e− collider}, volume = {135}, year = {2025}, }
• (2025). Most stringent bound on electron neutrino mass obtained with a scalable low-temperature microcalorimeter array. PRL, 135(14), 141801. (www)

  @article{ , abstract = {The determination of the absolute neutrino mass scale remains a fundamental open question in particle physics, with profound implications for both the standard model and cosmology. Direct kinematic measurements, independent of model-dependent assumptions, provide the most robust approach to address this challenge. Here we present the most stringent upper bound on the effective electron neutrino mass ever obtained with a calorimetric measurement of the electron capture decay of Ho 163 . The HOLMES experiment employs an array of ion-implanted transition-edge sensor (TES) microcalorimeters, achieving an average energy resolution of 6 eV FWHM with a scalable, multiplexed readout technique. With a total of 7 × 10 7 decay events recorded over two months and a Bayesian statistical analysis, we derive an upper limit of m β < 27 eV / c 2 at 90% credibility. These results validate the feasibility of Ho 163 calorimetry for next-generation neutrino mass experiments and demonstrate the potential of a scalable TES-based microcalorimetric technique to push the sensitivity of direct neutrino mass measurements beyond the current state of the art.}, archive = {J_PRL}, author = {B. K. Alpert and M. Balata and D. T. Becker and D. A. Bennett and M. Borghesi and P. Campana and R. Carobene and M. De Gerone and W. B. Doriese and M. Faverzani and L. Ferrari Barusso and E. Ferri and J. W. Fowler and G. Gallucci and S. Gamba and J. D Gard and F. Gatti and A. Giachero and M. Gobbo and U. Köster and D. Labranca and M. Lusignoli and P. Manfrinetti and J. A. B. Mates and E. Maugeri and R. Moretti and S. Nisi and A. Nucciotti and G. C. O’Neil and L. Origo and G. Pessina and S. Ragazzi and C. D. Reintsema and D. R. Schmidt and D. Schumann and D. S Swetz and Z. Talip and J. N. Ullom and L. R. Vale}, doi = {10.1103/s9vl-7n24}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141801}, shortjournal = {Phys. Rev. Lett.}, title = {Most stringent bound on electron neutrino mass obtained with a scalable low-temperature microcalorimeter array}, volume = {135}, year = {2025}, }
• (2025). Boundary criticality for the gross-neveu-yukawa models. PRL, 135(14), 141602. (www)

  @article{ , abstract = {We study the boundary criticality for the Gross-Neveu-Yukawa (GNY) models. Employing interacting Dirac fermions on a honeycomb lattice with armchair boundaries, we use determinant quantum Monte Carlo simulation to uncover rich boundary criticalities at the quantum phase transition to a charge density wave (CDW) insulator, including the ordinary, special, and extraordinary transitions. The Dirac fermions satisfy a Dirichlet boundary condition, while the boson field, representing the CDW order, obeys Dirichlet and Neumann conditions at the ordinary and special transitions, respectively, thereby enriching the critical GNY model. We develop a perturbative 4 − ε renormalization group approach to compute the boundary critical exponents. Our framework generalizes to other GNY universality class variants and provides theoretical predictions for experiments.}, archive = {J_PRL}, author = {Huan Jiang and Yang Ge and Shao-Kai Jian}, doi = {10.1103/tjfk-84f8}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141602}, shortjournal = {Phys. Rev. Lett.}, title = {Boundary criticality for the gross-neveu-yukawa models}, volume = {135}, year = {2025}, }
• (2025). Condensates, crystals, and renormalons in the gross-neveu model at finite density. PRL, 135(14), 141601. (www)

  @article{ , abstract = {We study the O ( 2 N ) symmetric Gross-Neveu model at finite density in the presence of a U ( 1 ) chemical potential h for a generic number a ≤ N − 2 of fermion fields. By combining perturbative quantum field theory, semiclassical large N , and Bethe ansatz techniques, we show that at finite N two new dynamically generated scales Λ n and Λ c appear in the theory, governing the mass gap of neutral and charged fermions, respectively. Above a certain threshold value for h , a -fermion bound states condense and form an inhomogeneous configuration, which at infinite N is a crystal spontaneously breaking translations. At large h , this crystal has mean Λ n and spatial oscillations of amplitude Λ c . The two scales also control the nonperturbative corrections to the free energy, resolving a puzzle concerning fractional-power renormalons and predicting new ones.}, archive = {J_PRL}, author = {Francesco Benini and Ohad Mamroud and Tomás Reis and Marco Serone}, doi = {10.1103/trj9-r9j8}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141601}, shortjournal = {Phys. Rev. Lett.}, title = {Condensates, crystals, and renormalons in the gross-neveu model at finite density}, volume = {135}, year = {2025}, }
• (2025). New framework for classical double copies. PRL, 135(14), 141501. (www)

  @article{ , abstract = {The double copy relates gauge and gravitational theories, with widespread application to quantum scattering amplitudes and classical perturbative results. It also connects exact classical solutions of Abelian gauge and gravitational theories in a small number of specific examples, known as classical double copies. These have a number of special properties, such as being algebraically special, and it remains an open question whether examples exist for algebraically general spacetimes or with nontrivial dynamics. Here, we provide a novel framework for understanding classical double copies at the level of the metric, both organizing the known examples and exploring their properties under a new lens. Utilizing Killing vectors as natural gauge fields on a spacetime, we propose a procedure for generating new classical double copies. As a proof of concept, we provide a flat-space single copy for the Kasner metric, an algebraically general spacetime. This example is also a double copy at the level of its curvature and provides the first type-I Weyl double copy on flat spacetime, confirming expectations from perturbation theory. This provides a promising avenue for extending exact double copies to a broader class of general, physically relevant spacetimes.}, archive = {J_PRL}, author = {Brian Kent and Aaron Zimmerman}, doi = {10.1103/xn1j-ddcc}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141501}, shortjournal = {Phys. Rev. Lett.}, title = {New framework for classical double copies}, volume = {135}, year = {2025}, }
• (2025). Resummation of universal tails in gravitational waveforms. PRL, 135(14), 141401. (www)

  @article{ , abstract = {We present a formula for the universal anomalous scaling of the multipole moments of a generic gravitating source in classical general relativity. We derive this formula in two independent ways using effective field theory methods. First, we use the absorption of low-frequency gravitational waves by a black hole to identify the total multipole scaling dimension as the renormalized angular momentum of black hole perturbation theory. More generally, we show that the anomalous dimension is determined by phase shifts of gravitational waves elastically scattering off generic source multipole moments, which reproduces the renormalized angular momentum in the particular case of black holes. The effective field theory approach thus clarifies the role of the renormalized angular momentum in the multipole expansion. The universality of the point particle effective description of compact gravitating systems further allows us to extract the universal part of the anomalous dimension, which is the same for any object, including black holes, neutron stars, and binary systems. As an application, we propose a novel resummation of the universal short-distance logarithms (“tails”) in the gravitational waveform of binary systems, which may improve the modeling of signals from current and future gravitational wave experiments.}, archive = {J_PRL}, author = {Mikhail M. Ivanov and Yue-Zhou Li and Julio Parra-Martinez and Zihan Zhou}, doi = {10.1103/jzd1-qzkt}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141401}, shortjournal = {Phys. Rev. Lett.}, title = {Resummation of universal tails in gravitational waveforms}, volume = {135}, year = {2025}, }
• (2025). Probing vector chirality in the early universe. PRL, 135(14), 141002. (www)

  @article{ , abstract = {We explore the potential of using late-time galaxy spins to test the parity symmetry of primordial vector fossils. Using N -body simulations, we analyze halo spins as a reliable proxy for galaxy spins to investigate the detectability of this effect. We develop a novel approach to generate initial conditions (ICs) that have substantial parity asymmetry but do not alter the initial matter power spectrum. We construct the initial spin fields from the parity broken ICs and halo spin fields using late-time halos evolved from such ICs. Focusing on the helicity of these vector fields, we detect substantial asymmetry in the initial spin field. In addition, we find that over 50% of the initial spin field’s asymmetry remains in the late-time halo spin field on a range of scales. Based on mock galaxy spin fields derived from the halo spin fields, we forecast that a maximum detection at 13 σ is possible with the final DESI BGS for the model considered in this analysis. Our findings demonstrate that primordial vectorial parity violation survives nonlinear gravitational evolution, and thus, can be effectively probed with galaxy spins at late times.}, archive = {J_PRL}, author = {Junsup Shim and Ue-Li Pen and Hao-Ran Yu and Teppei Okumura}, doi = {10.1103/ym2n-lzts}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {141002}, shortjournal = {Phys. Rev. Lett.}, title = {Probing vector chirality in the early universe}, volume = {135}, year = {2025}, }
• (2025). Exponential quantum advantages for practical non-hermitian eigenproblems. PRL, 135(14), 140601. (www)

  @article{ , abstract = {Non-Hermitian physics has emerged as a rich field of study, with applications ranging from P T -symmetry breaking and skin effects to non-Hermitian topological phase transitions. Yet most studies remain restricted to small-scale or classically tractable systems. While quantum computing has shown strong performance in Hermitian eigenproblems, its extension to the non-Hermitian regime remains largely unexplored. Here, we develop a quantum algorithm to address general non-Hermitian eigenvalue problems, specifically targeting eigenvalues near a given line in the complex plane—thereby generalizing previous results on ground state energy and spectral gap estimation for Hermitian matrices. Our method combines a fuzzy quantum eigenvalue detector with a divide-and-conquer strategy to efficiently isolate relevant eigenvalues. This yields a provable exponential quantum speedup for non-Hermitian eigenproblems. Furthermore, we discuss the broad applications in detecting spontaneous P T -symmetry breaking, estimating Liouvillian gaps, and analyzing classical Markov processes. These results highlight the potential of quantum algorithms in tackling challenging problems across quantum physics and beyond.}, archive = {J_PRL}, author = {Xiao-Ming Zhang and Yukun Zhang and Wenhao He and Xiao Yuan}, doi = {10.1103/3n8f-k8pl}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {140601}, shortjournal = {Phys. Rev. Lett.}, title = {Exponential quantum advantages for practical non-hermitian eigenproblems}, volume = {135}, year = {2025}, }
• (2025). Single-ion information engine for charging quantum battery. PRL, 135(14), 140403. (www)

  @article{ , abstract = {Information engines produce mechanical work through measurement and adaptive control. For information engines, the principal challenge lies in how to store the generated work to the external load. Here, we report an experimental demonstration where quantized mechanical motion serves as a quantum battery and gets charged in repeated cycles by a single trapped-ion information engine. This is enabled by a key technological advancement in rapid state discrimination, allowing us to suppress measurement-induced disturbances. Consequently, we were able to obtain an information-to-ergotropy conversion efficiency approaching 67% of the theoretical limit at the optimal temperature, along with a maximum information-to-work conversion efficiency of 70%. The experimental results substantiate that this approach can render trapped ions a promising platform for microscopic information engines with potential applications in the future upon scaling up.}, archive = {J_PRL}, author = {Jialiang Zhang and Pengfei Wang and Wentao Chen and Zhengyang Cai and Mu Qiao and Riling Li and Yingye Huang and Haonan Tian and Chuyang Luan and Hengchao Tu and Kaifeng Cui and Leilei Yan and Junhua Zhang and Jingning Zhang and Manhong Yung and Kihwan Kim}, doi = {10.1103/g45c-ssfx}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {140403}, shortjournal = {Phys. Rev. Lett.}, title = {Single-ion information engine for charging quantum battery}, volume = {135}, year = {2025}, }
• (2025). Critically slow hilbert-space ergodicity in quantum morphic drives. PRL, 135(14), 140402. (www)

  @article{ , abstract = {The maximum entropy principle is foundational for statistical analyses of complex dynamics. This principle has been challenged by the findings of a previous work [ Phys. Rev. X 7 , 031034 (2017) ], where it was argued that a quantum system driven in time by a certain aperiodic sequence without any explicit symmetries, dubbed the Thue-Morse drive, gives rise to emergent nonergodic steady states which are underpinned by effective conserved quantities. Here, we resolve this apparent tension. We rigorously prove that the Thue-Morse drive achieves a very strong notion of quantum ergodicity in the long-time limit: The time evolution of any initial state uniformly visits every corner of its Hilbert space. On the other hand, we find the dynamics also approximates a Floquet drive for arbitrarily long, albeit finite periods of time with no characteristic timescale, resulting in a scale-free ergodic dynamics we call critically slow complete Hilbert-space ergodicity. Furthermore, numerical studies reveal that critically slow complete Hilbert-space ergodicity is not specific to the Thue-Morse drive and is, in fact, exhibited by many other aperiodic drives derived from morphic sequences, i.e., words derived from repeatedly applying substitution rules on basic characters. Our Letter presents a new class of dynamics in time-dependent quantum systems where full ergodicity is eventually attained but only after astronomically long times.}, archive = {J_PRL}, author = {Saúl Pilatowsky-Cameo and Soonwon Choi and Wen Wei Ho}, doi = {10.1103/dmfd-lgcq}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {140402}, shortjournal = {Phys. Rev. Lett.}, title = {Critically slow hilbert-space ergodicity in quantum morphic drives}, volume = {135}, year = {2025}, }
• (2025). Classical non-markovian noise in symmetry-preserving quantum dynamics. PRL, 135(14), 140401. (www)

  @article{ , abstract = {In quantum dynamics, symmetries are vital for identifying and assessing conserved quantities that govern the evolution of a quantum system. When promoted to the open quantum system setting, dynamical symmetries can be negatively altered by system-environment interactions, thus, complicating their analysis. Previous work on noisy symmetric quantum dynamics has focused on the Markovian setting, despite the ubiquity of non-Markovian noise in a number of widely used quantum technologies. In this Letter, we develop a framework for quantifying the impact of non-Markovian noise on symmetric quantum evolution via root space decompositions and the filter function formalism. We demonstrate analytically that symmetry-preserving noise maintains the symmetric subspace, while nonsymmetric noise leads to highly specific leakage errors that are block diagonal in the symmetry representation. We support our findings with numerical studies of a transverse-field Ising model and a quantum error detecting code subject to spatiotemporally correlated multiaxis noise. Our results are broadly applicable, providing new analytic insights into the control and characterization of open quantum system dynamics.}, archive = {J_PRL}, author = {William M. Watkins and Gregory Quiroz}, doi = {10.1103/t78h-c9s3}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {140401}, shortjournal = {Phys. Rev. Lett.}, title = {Classical non-markovian noise in symmetry-preserving quantum dynamics}, volume = {135}, year = {2025}, }
• (2025). Characterizing the multipartite entanglement structure of non-gaussian continuous-variable states with a single evolution operator. PRL, 135(14), 140201. (www)

  @article{ , abstract = {Multipartite entanglement is an essential resource for quantum information tasks, but characterizing entanglement structures in continuous-variable systems remains challenging, especially in multimode non-Gaussian scenarios. In this Letter, we introduce an efficient method for detecting multipartite entanglement structures in continuous-variable states. Based on the quantum Fisher information, we propose a systematic approach to identify an encoding operator that can efficiently capture the quantum correlations in multimode non-Gaussian states. We demonstrate the effectiveness of our method on over 10 5 randomly generated multimode-entangled quantum states, achieving a very high success rate in entanglement detection. Additionally, the robustness of our method can be considerably enhanced against losses by expanding the set of accessible operators. This Letter provides a general framework for characterizing entanglement structures in diverse continuous-variable systems, enabling a number of experimentally relevant applications.}, archive = {J_PRL}, author = {Mingsheng Tian and Xiaoting Gao and Boxuan Jing and Fengxiao Sun and Matteo Fadel and Manuel Gessner and Qiongyi He}, doi = {10.1103/21t1-dqn6}, journal = {Physical Review Letters}, month = {9}, number = {14}, pages = {140201}, shortjournal = {Phys. Rev. Lett.}, title = {Characterizing the multipartite entanglement structure of non-gaussian continuous-variable states with a single evolution operator}, volume = {135}, year = {2025}, }
• (2025). Efficient microcanonical histogram analysis and application to peptide aggregation. PRL, 135(13), 138401. (www)

  @article{ , abstract = {A novel approach designed to directly estimate microcanonical quantities from energy histograms is proposed, which enables the immediate systematic identification and classification of phase transitions in physical systems of any size by means of the recently introduced generalized microcanonical inflection-point analysis method. The application to the aggregation problem of GNNQQNY heptapeptides, for which the entire transition sequence is revealed, shows the power of this promising method.}, archive = {J_PRL}, author = {Michael Bachmann}, doi = {10.1103/rvqy-7jkq}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {138401}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient microcanonical histogram analysis and application to peptide aggregation}, volume = {135}, year = {2025}, }
• (2025). Wall torque controls propulsion of curved microstructures in bacterial baths. PRL, 135(13), 138302. (www)

  @article{ , abstract = {The persistent dynamics of active particles makes them explore extended portions of an obstacle’s boundary during collisions. From impact to escape, the net applied forces depend on the curvature of the wall and increase in the presence of concave features. Here we systematically investigate the forces exerted by swimming bacteria on microfabricated structures, where the radii of curvature can be varied parametrically. We find that these microsails are propelled with a speed that scales linearly with curvature and is directed from concave to convex side along the axis of symmetry. By solving the collision problem for microswimmers subject to aligning torques at the wall, we show that, despite bacteria rapidly aligning with the surface plane, the resulting force law reduces to that of spherical active particles, with the wall-induced reorientation rate effectively replacing rotational diffusion.}, archive = {J_PRL}, author = {Nicola Pellicciotta and Ojus Satish Bagal and Maria Cristina Cannarsa and Silvio Bianchi and Roberto Di Leonardo}, doi = {10.1103/pnjv-6n5r}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {138302}, shortjournal = {Phys. Rev. Lett.}, title = {Wall torque controls propulsion of curved microstructures in bacterial baths}, volume = {135}, year = {2025}, }
• (2025). Scaling laws for passive polymer dynamics in active turbulence. PRL, 135(13), 138301. (www)

  @article{ , abstract = {Biological systems commonly combine intrinsically out-of-equilibrium active components with passive polymeric inclusions to produce unique material properties. To explore these composite systems, idealized models—such as polymers in active fluids—are essential to develop a predictive theoretical framework. We simulate a single, freely jointed passive chain in two-dimensional active turbulence. Active flows advect the polymer, producing a substantially enhanced diffusivity. Our results reveal that the dimensionless diffusivity obeys scaling laws governed by the Péclet, Weissenberg, and Ericksen numbers, which paves the way for designing active/polymeric hybrid materials with predictable properties that differ significantly from those of nondeformable inclusions.}, archive = {J_PRL}, author = {Zahra K. Valei and Tyler N. Shendruk}, doi = {10.1103/w3gp-knnp}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {138301}, shortjournal = {Phys. Rev. Lett.}, title = {Scaling laws for passive polymer dynamics in active turbulence}, volume = {135}, year = {2025}, }
• (2025). Entropic modulation of divalent cation transport. PRL, 135(13), 138001. (www)

  @article{ , abstract = {Aqueous cations permeate subnanoscale pores by crossing free energy barriers dominated by competing enthalpic contributions from transiently decreased ion-solvent and increased ion-pore electrostatic interactions. This commonly accepted view is rooted in the studies of monovalent cation transport. Divalent cations, however, have significantly higher desolvation costs, requiring considerably larger pores to enable retention of the first hydration shell and subsequently transport. We show that this scenario gives rise to a strong enthalpy-entropy competition. Specifically, the first hydration shell is shown to undergo rotational ordering inside the pore, resulting in a tight transition state. Our results shed light on the basic mechanisms of transport barrier formation for aqueous divalent cations permeating nanoporous 2D membranes.}, archive = {J_PRL}, author = {Yechan Noh and Demian Riccardi and Alex Smolyanitsky}, doi = {10.1103/vtw2-z4f8}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {138001}, shortjournal = {Phys. Rev. Lett.}, title = {Entropic modulation of divalent cation transport}, volume = {135}, year = {2025}, }
• (2025). Universal model of urban street networks. PRL, 135(13), 137401. (www)

  @article{ , abstract = {Analyzing 9000 urban areas’ street networks, we identify properties, including extreme betweenness centrality heterogeneity, that typical spatial network models fail to explain. Accordingly we propose a universal, parsimonious, generative model based on a two-step mechanism that begins with a spanning tree as a backbone then iteratively adds edges to match empirical degree distributions. Controlled by a single parameter representing lattice-equivalent node density, it accurately reproduces key universal properties to bridge the gap between empirical observations and generative models.}, archive = {J_PRL}, author = {Marc Barthelemy and Geoff Boeing}, doi = {10.1103/1vj4-n8vn}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {137401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal model of urban street networks}, volume = {135}, year = {2025}, }
• (2025). Exact large-scale correlations in diffusive systems with general interactions. PRL, 135(13), 137102. (www)

  @article{ , abstract = {Characterizing the statistical properties of classical interacting particle systems is a long-standing question. For Brownian particles, the microscopic density obeys a stochastic evolution equation, known as the Dean-Kawasaki equation. This equation remains mostly formal and linearization (or higher-order expansions) is required to obtain explicit expressions for physical observables, with a range of validity not easily defined. Here, by combining macroscopic fluctuation theory with equilibrium statistical mechanics, we provide a systematic alternative to the Dean-Kawasaki framework to characterize large-scale correlations. This approach enables us to obtain explicit and exact results for the large-scale behavior of dynamical observables such as tracer cumulants and bath-tracer correlations in one dimension, both in and out of equilibrium. In particular, we reveal a generic nonmonotonic spatial structure in the response of the bath following a temperature quench. Our approach applies to a broad class of interaction potentials and extends naturally to higher dimensions.}, archive = {J_PRL}, author = {Aurélien Grabsch and Davide Venturelli and Olivier Bénichou}, doi = {10.1103/gwdh-3vqm}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {137102}, shortjournal = {Phys. Rev. Lett.}, title = {Exact large-scale correlations in diffusive systems with general interactions}, volume = {135}, year = {2025}, }
• (2025). Super-resolved anomalous diffusion: Deciphering the joint distribution of anomalous exponent and diffusion coefficient. PRL, 135(13), 137101. (www)

  @article{ , abstract = {The molecular motion in heterogeneous media displays anomalous diffusion by the mean-squared displacement ⟨ X 2 ( t ) ⟩ = 2 D t α . Motivated by experiments reporting populations of the anomalous diffusion parameters α and D , we aim to disentangle their respective contributions to the observed variability when this last is due to a true population of these parameters and when it arises due to finite-duration recordings. We introduce estimators of the anomalous diffusion parameters on the basis of the time-averaged mean-squared displacement and study their statistical properties. By using a copula approach, we derive a formula for the joint density function of their estimations conditioned on their actual values. The methodology introduced is indeed universal, it is valid for any Gaussian process and can be applied to any quadratic time-averaged statistics. We also explain the experimentally reported relation D ∝ exp ( α c 1 + c 2 ) for which we provide the exact expression. We compare our findings to numerical simulations of the fractional Brownian motion and quantify their accuracy by using the Hellinger distance. Finally, we provide guidelines and routines for fitting experimental data.}, archive = {J_PRL}, author = {Yann Lanoiselée and Gianni Pagnini and Agnieszka Wyłomańska}, doi = {10.1103/y5pn-5ynd}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {137101}, shortjournal = {Phys. Rev. Lett.}, title = {Super-resolved anomalous diffusion: Deciphering the joint distribution of anomalous exponent and diffusion coefficient}, volume = {135}, year = {2025}, }
• (2025). Electrically tunable picosecond-scale octupole fluctuations in chiral antiferromagnets. PRL, 135(13), 136704. (www)

  @article{ , abstract = {We present a theory for the relaxation time of the octupole order parameter in nanoscale chiral antiferromagnets (AFMs) coupled to thermal baths and spin injection sources. Using stochastic spin dynamics simulations, we demonstrate that the octupole moment relaxes through two distinct mechanisms—escape over a barrier and precessional dephasing—as the barrier for octupole fluctuations is lowered relative to the thermal energy. Notably, the octupole moment relaxes orders of magnitude faster than the typical dipolar order parameters, reaching picosecond timescales. By combining Langer’s theory with an effective low-energy description of octupole dynamics in chiral AFMs, we derive analytical expressions for the relaxation times. We find that relaxation in chiral AFMs parallels dipole relaxation in magnets, with exchange fields serving the role of the dipole fields. Further, by drawing on the analogy between order parameter dynamics in magnets under spin injection and current-biased Josephson junctions, we propose a new scheme for electrically tuning the octupole relaxation times. Our Letter offers fundamental insights for the development of next-generation spintronic devices that harness octupole order parameters for information encoding.}, archive = {J_PRL}, author = {Shiva T. Konakanchi and Sagnik Banerjee and Mohammad M. Rahman and Yuta Yamane and Shun Kanai and Shunsuke Fukami and Pramey Upadhyaya}, doi = {10.1103/w2wj-c9jx}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136704}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically tunable picosecond-scale octupole fluctuations in chiral antiferromagnets}, volume = {135}, year = {2025}, }
• (2025). Thermal spin wave noise as a probe for the dzyaloshinskii-moriya interaction. PRL, 135(13), 136703. (www)

  @article{ , abstract = {Interfacial Dzyaloshinskii-Moriya interaction (DMI) is a key ingredient in the stabilization of chiral magnetic states in thin films. Its sign and strength often determine crucial properties of magnetic objects, like their topology or how they can be manipulated with currents. A few experimental techniques are currently available to measure DMI quantitatively, based on the study of domain walls, spin waves, or spin-orbit torques. In this Letter, we propose a qualitative variant of spin wave methods. We rely on magnetic noise from confined thermal spin waves in domain walls and skyrmions in perpendicularly magnetized thin films, which we probe with scanning nitrogen-vacancy center relaxometry. We show both numerically and experimentally that the sign of the DMI can be inferred from the amplitude of the detected noise, which is affected by the nonreciprocity in the spin wave dispersion. Furthermore, we also demonstrate that the noise distribution around the contour of magnetic skyrmions reveals their Néel or Bloch nature, giving therefore also insight into the strength of DMI involved in their stabilization.}, archive = {J_PRL}, author = {Aurore Finco and Pawan Kumar and Van Tuong Pham and Joseba Urrestarazu-Larrañaga and Rodrigo Guedas Garcia and Maxime Rollo and Olivier Boulle and Joo-Von Kim and Vincent Jacques}, doi = {10.1103/dvbq-9z5f}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136703}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal spin wave noise as a probe for the dzyaloshinskii-moriya interaction}, volume = {135}, year = {2025}, }
• (2025). Large magnetoresistance in an electrically tunable van der waals antiferromagnet. PRL, 135(13), 136702. (www)

  @article{ , abstract = {The interplay between magnetic order and electronic band structure in antiferromagnets has garnered increasing interest due to its potential for spintronic applications. While magnetic transitions have been shown to induce substantial band structure modifications in optical measurements, their influence on electronic transport remains poorly understood. In this work, we investigate the transport properties of CrSBr, a van der Waals antiferromagnetic semiconductor, over a wide range of carrier densities modulated by gate voltage. We observe a drastic contrast in magnetoresistance behavior between the low- and high-carrier density regimes. Through a combination of experiment and modeling, we identify magnetically driven carrier concentration modulation and mobility modulation as the dominant mechanisms governing magnetoresistance in the respective regimes. These findings advance the understanding of magnetoelectric transport in antiferromagnets and suggest promising routes for energy-efficient spintronic technologies in memory, logic, and sensing applications.}, archive = {J_PRL}, author = {Chung-Tao Chou and Eugene Park and Josep Ingla-Aynes and Julian Klein and Kseniia Mosina and Jagadeesh S. Moodera and Zdenek Sofer and Frances M. Ross and Luqiao Liu}, doi = {10.1103/hpmq-rnh4}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136702}, shortjournal = {Phys. Rev. Lett.}, title = {Large magnetoresistance in an electrically tunable van der waals antiferromagnet}, volume = {135}, year = {2025}, }
• (2025). Robust triple-q magnetic order with trainable spin vorticity in Na2Co2TeO6. PRL, 135(13), 136701. (www)

  @article{ , abstract = {Recent studies suggest that the candidate Kitaev magnet Na 2 Co 2 TeO 6 possesses novel triple- q magnetic order instead of conventional single- q zigzag order. Here we present dedicated experiments in a search for distinct properties expected of the triple- q order, namely, insensitivity of the magnetic Bragg intensities to weak C 3 symmetry-breaking fields and fictitious magnetic fields generated by the spin vorticity. In structurally pristine single crystals, we show that C 3 symmetry-breaking in-plane uniaxial strains do not affect the order’s magnetic neutron diffraction signals. We further show that c -axis propagating light exhibits large Faraday rotations in the ordered state due to the spin vorticity, the sign of which can be trained via the system’s ferrimagnetic moment. These results favor the triple- q order in Na 2 Co 2 TeO 6 and reveal its unique emerging behavior.}, archive = {J_PRL}, author = {Xianghong Jin and Mengqiao Geng and Fabio Orlandi and Dmitry Khalyavin and Pascal Manuel and Yang Liu and Yuan Li}, doi = {10.1103/hd1p-rdyc}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136701}, shortjournal = {Phys. Rev. Lett.}, title = {Robust triple-q magnetic order with trainable spin vorticity in Na2Co2TeO6}, volume = {135}, year = {2025}, }
• (2025). Observation of embedded topology in a trivial bulk via projective crystal symmetry. PRL, 135(13), 136602. (www)

  @article{ , abstract = {Bulk-boundary correspondence is the foundational principle of topological physics, first established in the quantum Hall effect, where a D -dimensional topologically nontrivial bulk gives rise to ( D − 1 )-dimensional boundary states. The advent of higher-order topology has generalized this principle to a hierarchical chain, enabling topological states to appear at ( D − 2 ) or even lower-dimensional boundaries. To date, all known realizations of topological systems must require a topologically nontrivial bulk to initiate the chain of action for bulk-boundary correspondence. Here, in an acoustic crystal platform, we experimentally demonstrate an exception to this paradigm—embedded topology in a trivial bulk—where the bulk-boundary correspondence originates from a trivial bulk. Rather than relying on global symmetries, we employ projective crystal symmetry, which induces nontrivial topology not at the outset in the D -dimensional bulk, but midway through the correspondence hierarchy in lower-dimensional boundaries. We further realize a three-dimensional system exhibiting embedded topology that supports zero-dimensional topological states, achieving the longest possible chain of action for such an unconventional bulk-boundary correspondence in physical space. Our Letter experimentally establishes a new form of bulk-boundary correspondence initiated from a trivial bulk, opening additional degrees of freedom for the design of robust topological devices.}, archive = {J_PRL}, author = {Hau Tian Teo and Yang Long and Hong-yu Zou and Kailin Song and Haoran Xue and Yong Ge and Shou-qi Yuan and Hong-xiang Sun and Baile Zhang}, doi = {10.1103/9tq1-37j1}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136602}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of embedded topology in a trivial bulk via projective crystal symmetry}, volume = {135}, year = {2025}, }
• (2025). Brillouin platycosms and topological phases. PRL, 135(13), 136601. (www)

  @article{ , abstract = {There exist ten distinct closed flat 3D manifolds, known as “platycosms,” that hold significance in mathematics and have been postulated as potential geometric models for our Universe. In this Letter, we demonstrate their manifestation as universes of Bloch particles, namely as momentum-space units referred to as Brillouin platycosms, which are natural extensions of the Brillouin torus within a broader framework of projective crystallographic symmetries. Moreover, we provide exact K -theoretical classifications of topological insulators over these platycosms by the Atiyah-Hirzebruch spectral sequence, and formulate a complete set of topological invariants for their identification. Topological phase transitions are generically characterized by Weyl semimetals, adhering to the generalized Nielsen-Ninomiya theorem: the total chirality number over a Brillouin platycosm is even (zero) if the platycosm is nonorientable (orientable). Our Letter generalizes the notion of Brillouin torus to ten Brillouin platycosms and therefore fundamentally diversifies the stages on which Bloch wave functions can perform their topological dance.}, archive = {J_PRL}, author = {Chen Zhang and Peiyuan Wang and Junkun Lyu and Y. X. Zhao}, doi = {10.1103/pllk-n4h3}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136601}, shortjournal = {Phys. Rev. Lett.}, title = {Brillouin platycosms and topological phases}, volume = {135}, year = {2025}, }
• (2025). Orbital-selective quasiparticle depletion across the density wave transition in trilayer nickelate La4Ni3O10. PRL, 135(13), 136505. (www)

  @article{ , abstract = {We investigate the evolution of polarized electronic response in trilayer nickelate , reporting a systematic reduction of the incoherent electron continuum across the density wave transition in the and representations. Analysis based on the Fermi surface band curvatures points to quasiparticle coherence in momentum positions with dominant orbital character. Our findings establish the symmetry channels and the active role of orbitals involved in the density wave formation, offering important insight into the electronic and magnetic correlations in the nickelate.}, archive = {J_PRL}, author = {Dong-Hyeon Gim and Chung Ha Park and Kee Hoon Kim}, doi = {10.1103/1tp1-y73g}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136505}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital-selective quasiparticle depletion across the density wave transition in trilayer nickelate La4Ni3O10}, volume = {135}, year = {2025}, }
• (2025). Simulating the two-dimensional t−J model at finite doping with neural quantum states. PRL, 135(13), 136504. (www)

  @article{ , abstract = {Simulating large, strongly interacting fermionic systems remains a major challenge for existing numerical methods. In this Letter, we introduce Gutzwiller projected hidden fermion determinant states (G-HFDS) to simulate the strongly interacting limit of the Fermi-Hubbard model, namely the t − J model, across the entire doping regime. We demonstrate that the G-HFDS achieve energies competitive with matrix product states on lattices as large as 10 × 10 sites while using several orders of magnitude fewer parameters, suggesting the potential for efficient application to even larger system sizes. This remarkable efficiency enables us to probe low-energy physics across the full doping range, providing new insights into the competition between kinetic and magnetic interactions and the nature of emergent quasiparticles. Starting from the low-doping regime, where magnetic polarons dominate the low energy physics, we track their evolution with increasing doping and different next-nearest neighbor hopping amplitudes through analyses of spin and polaron correlation functions as well as the Fermi surface. Our findings demonstrate the potential of determinant-based neural quantum states with an inherent fermionic sign structure, opening the way for simulating large-scale fermionic systems at any particle filling.}, archive = {J_PRL}, author = {Hannah Lange and Annika Böhler and Christopher Roth and Annabelle Bohrdt}, doi = {10.1103/rc31-5hl9}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136504}, shortjournal = {Phys. Rev. Lett.}, title = {Simulating the two-dimensional t−J model at finite doping with neural quantum states}, volume = {135}, year = {2025}, }
• (2025). Band renormalization, quarter metals, and chiral superconductivity in rhombohedral tetralayer graphene. PRL, 135(13), 136503. (www)

  @article{ , abstract = {Recently, exotic superconductivity emerging from a spin-and-valley-polarized metallic phase has been discovered in rhombohedral tetralayer graphene. To explain this observation, we study the role of electron-electron interactions in driving flavor symmetry breaking, using the Hartree-Fock (HF) approximation, and in stabilizing superconductivity mediated by repulsive interactions. Though mean-field HF correctly predicts the isospin flavors and reproduces the experimental phase diagram, it overestimates the band renormalization near the Fermi energy and suppresses superconducting instabilities. To address this, we introduce a physically motivated scheme that includes internal screening in the HF calculation. Using this formalism, we find superconductivity arising from the spin-valley polarized phase, on the electron-doped side, for a range of electric fields and electron dopings. Our findings reproduce the experimental observations and reveal a p -wave, finite-momentum, time-reversal-symmetry-broken superconducting state, encouraging further investigation into exotic phases in graphene multilayers.}, archive = {J_PRL}, author = {Guillermo Parra-Martínez and Alejandro Jimeno-Pozo and Võ Tiến Phong and Héctor Sainz-Cruz and Daniel Kaplan and Peleg Emanuel and Yuval Oreg and Pierre A. Pantaleón and José Ángel Silva-Guillén and Francisco Guinea}, doi = {10.1103/zfmh-rjzc}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136503}, shortjournal = {Phys. Rev. Lett.}, title = {Band renormalization, quarter metals, and chiral superconductivity in rhombohedral tetralayer graphene}, volume = {135}, year = {2025}, }
• (2025). Self-reconstruction of order parameter in spin-triplet superconductor UTe2. PRL, 135(13), 136502. (www)

  @article{ , abstract = {We investigate the effect of easy-axis metamagnetic crossover on superconductivity in along the axis through measurements of ac susceptibility, magnetization, and the magnetocaloric effect. In ultraclean single crystals, we identify a field-induced phase transition within the superconducting state at 5.6 T, driven by metamagnetism. This transition leads to a high-field superconducting state, significantly increasing the upper critical field to 12 T. A sudden increase in entropy at the transition suggests a self-reconstruction of the order parameter, enabling multicomponent superconducting states to adapt to external perturbations.}, archive = {J_PRL}, author = {Y. Tokiwa and P. Opletal and H. Sakai and K. Kubo and S. Kambe and E. Yamamoto and M. Kimata and S. Awaji and T. Sasaki and D. Aoki and Y. Yanase and Y. Tokunaga and Y. Haga}, doi = {10.1103/z8yx-yzdh}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136502}, shortjournal = {Phys. Rev. Lett.}, title = {Self-reconstruction of order parameter in spin-triplet superconductor UTe2}, volume = {135}, year = {2025}, }
• (2025). New pathway to impact ionization in a photoexcited one-dimensional ionic hubbard model. PRL, 135(13), 136501. (www)

  @article{ , abstract = {Using the time-dependent Lanczos method, we study the nonequilibrium dynamics of the half-filled one-dimensional ionic Hubbard model, deep within the Mott insulating regime, under the influence of a transient laser pulse. In equilibrium, increasing the staggered potential in the Mott regime reduces the Mott gap and broadens the Hubbard bands, creating favorable conditions for impact ionization. After laser excitation, impact ionization is observed, with its occurrence depending on both the staggered potential and the laser pump frequency. By analyzing the time evolution of the kinetic, ionic, and Coulomb interaction energies, we identify a novel mechanism for impact ionization, in which excess ionic potential energy is converted into additional double occupancy—distinct from the conventional mechanism where excess kinetic energy drives this process. We further reveal that impact ionization arises from interference between excited states driven by photon excitations of the same order. These results present a new pathway for realizing impact ionization in strongly correlated electron systems.}, archive = {J_PRL}, author = {Zhenyu Cheng and Li Yang and Xiang Hu and Hantao Lu and Zhongbing Huang and Liang Du}, doi = {10.1103/jnzl-r8rm}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136501}, shortjournal = {Phys. Rev. Lett.}, title = {New pathway to impact ionization in a photoexcited one-dimensional ionic hubbard model}, volume = {135}, year = {2025}, }
• (2025). Switchable chern insulators and competing quantum phases in rhombohedral graphene moiré superlattices. PRL, 135(13), 136302. (www)

  @article{ , abstract = {Graphene-based moiré superlattices provide a versatile platform for exploring novel correlated and topological electronic states, driven by enhanced Coulomb interactions within flat bands. The intrinsic tunability of graphene’s multiple degrees of freedom enables precise control over these complex quantum phases. In this study, we observe a range of competing phases and their transitions in rhombohedral stacked hexalayer graphene on hexagonal boron nitride ( ) moiré superlattices. When electrons are polarized away from the moiré superlattice, we first identify a Chern insulator with reversible Chern numbers at (one electron per moiré cell), revealing a competition between bulk and edge orbital magnetization. At , three distinct insulating phases—spin-antiferromagnetic, spin-polarized, and valley-polarized—emerge under vertical displacement field and magnetic field , governed by hierarchical isospin symmetry breaking. Furthermore, charge density wave (CDW) states at and , along with a magnetic-field-induced stripe phase at , demonstrate tunable correlated orders at fractional fillings. Our findings reveal a rich interplay of charge, isospin, topology, and magnetic field in rhombohedral graphene moiré superlattices.}, archive = {J_PRL}, author = {Jian Zheng and Size Wu and Kai Liu and Bosai Lyu and Shuhan Liu and Yating Sha and Zhengxian Li and Kenji Watanabe and Takashi Taniguchi and Jinfeng Jia and Zhiwen Shi and Guorui Chen}, doi = {10.1103/chsq-ndzs}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136302}, shortjournal = {Phys. Rev. Lett.}, title = {Switchable chern insulators and competing quantum phases in rhombohedral graphene moiré superlattices}, volume = {135}, year = {2025}, }
• (2025). Carrier localization and spontaneous formation of two-dimensional polarization domain in halide perovskites. PRL, 135(13), 136301. (www)

  @article{ , abstract = {Halide perovskites are known for their rich phase diagram and superior performance in diverse optoelectronics applications. The latter property is often attributed to the long electron-hole recombination time, whose underlying physical mechanism has been a long-standing controversy. In this Letter, we investigate the transport and localization properties of electron and hole carriers in a prototypical halide perovskite ( CsPbBr 3 ), through ab initio tight-binding nonadiabatic dynamics approach for large-scale (tens of nm size) supercell calculations, to simulate electron and ion dynamics on the same footing. We found distinct structural, lattice polarization, and electron-phonon coupling properties at low (below 100 K) and high temperatures, consistent with experimental observations. In particular, at low temperature we find spontaneous formation of polar grain boundaries in the nonpolar bulk systems, which result in two-dimensional polarization patterns that serve to localize and separate electrons and holes. We reveal phonon-assisted variable-range hopping mostly responsible for low-temperature transport, and their characteristic frequency correlates with temperature-dependent phonon power spectrum and energy oscillation frequency in nonadiabatic dynamics. We answer the critical questions of long electron-hole recombination lifetime at low temperature and offer the correlation among polarization domains, electron-phonon couplings, and photocarrier dynamics.}, archive = {J_PRL}, author = {Andrew Grieder and Marcos Calegari Andrade and Hiroyuki Takenaka and Tadashi Ogitsu and Liang Z. Tan and Yuan Ping}, doi = {10.1103/4kyt-jj6w}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136301}, shortjournal = {Phys. Rev. Lett.}, title = {Carrier localization and spontaneous formation of two-dimensional polarization domain in halide perovskites}, volume = {135}, year = {2025}, }
• (2025). Spatially resolved vibronic excitations of an isolated adsorbed organometallic complex via multiple tunneling channels. PRL, 135(13), 136202. (www)

  @article{ , abstract = {Vibronic excitations of molecules at nanoscale interfaces are important for molecular electronics and spintronics and have therefore attracted considerable attention. For single molecules in mechanically controlled break junctions or in a scanning tunneling microscope (STM), vibronic excitations are typically described by a double-barrier tunneling junction model. In this model, a homogeneous electric field is considered and the atomic structure of the metal contacts is neglected. Here, we report experimental STM data of a new nonplanar organometallic complex, [ Mo ( CO ) 3 ( Pyridine 3 S 3 ) ], on Ag(111). Spatially resolved maps of the vibronic excitations show several features related to the reordering of the occupied molecular orbitals due to the rapidly decaying potential of the tip apex. Such rearrangement leads to a significant shift in the vibronic levels as the tip position is changed. These observations, together with our modelling results, demonstrate that the molecular orbitals can be controlled by the field of the STM tip, whose atomic-scale variation deserves more attention in studies of nonplanar molecules.}, archive = {J_PRL}, author = {Xiangzhi Meng and Kai Uwe Clausen and Marie-Laure Bocquet and Alexander Weismann and Niklas Ide and Felix Tuczek and Richard Berndt}, doi = {10.1103/xxtf-98vs}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136202}, shortjournal = {Phys. Rev. Lett.}, title = {Spatially resolved vibronic excitations of an isolated adsorbed organometallic complex via multiple tunneling channels}, volume = {135}, year = {2025}, }
• (2025). Revealing band-hybrid cooper pairs on the surface of a superconductor with spin-orbit coupling. PRL, 135(13), 136201. (www)

  @article{ , abstract = {Most superconductors exhibit spin-singlet pairing within a single band. In multiband systems with strong spin-orbit coupling, more exotic scenarios can emerge, including Cooper pairs between bands with distinct symmetries. Here, we present evidence of the formation of Cooper pairs between spin-nondegenerate helical surface bands in the superconductor . Scanning tunneling microscopy reveals anisotropic Yu-Shiba-Rusinov (YSR) resonances induced by vanadium impurities, with long-range amplitude modulations attributed to spin-conserving Bogoliubov quasiparticle interference (BQPI). Analysis of BQPI at the subgap YSR energy shows that only a selective subset of normal-state scattering processes contributes to Cooper pair formation, indicating interband mixing. We trace this selectivity to the hybridization of a helical surface band with others via the impurity.}, archive = {J_PRL}, author = {Javier Zaldívar and Jon Ortuzar and Miguel Alvarado and Stefano Trivini and Julie Baumard and Carmen Rubio-Verdú and Edwin Herrera and Hermann Suderow and Alfredo Levy Yeyati and F. Sebastian Bergeret and Jose Ignacio Pascual}, doi = {10.1103/6jfy-cv89}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136201}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing band-hybrid cooper pairs on the surface of a superconductor with spin-orbit coupling}, volume = {135}, year = {2025}, }
• (2025). In-plane anisotropy of charge density wave fluctuations in 1T−TiSe2. PRL, 135(13), 136102. (www)

  @article{ , abstract = {We report measurements of anisotropic triple- q charge density wave (CDW) fluctuations in the transition metal dichalcogenide 1 T − TiSe 2 over a large volume of reciprocal space with x-ray diffuse scattering. Above the transition temperature, T CDW , the in-plane diffuse scattering is marked by ellipses which reveal that the in-plane fluctuations are anisotropic. In addition, the out-of-plane diffuse scattering is characterized by rodlike structures which indicate that the CDW fluctuations in neighboring layers are largely decoupled. Our analysis of the diffuse scattering line shapes and orientations suggests that the three charge density wave components contain independent phase fluctuations with a hierarchy of length scales, leading to intricate fluctuation patterns that go beyond the conventional 2D-to-3D crossover picture.}, archive = {J_PRL}, author = {Xuefei Guo and Anshul Kogar and Jans Henke and Felix Flicker and Fernando de Juan and Stella X.-L. Sun and Issam Khayr and Yingying Peng and Sangjun Lee and Matthew J. Krogstad and Stephan Rosenkranz and Raymond Osborn and Jacob P. C. Ruff and David B. Lioi and Goran Karapetrov and Daniel J. Campbell and Johnpierre Paglione and Jasper van Wezel and Tai C. Chiang and Peter Abbamonte}, doi = {10.1103/j8vm-wb65}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136102}, shortjournal = {Phys. Rev. Lett.}, title = {In-plane anisotropy of charge density wave fluctuations in 1T−TiSe2}, volume = {135}, year = {2025}, }
• (2025). Unified high-pressure phase-transition sequence in the f-electron metals: OF16→oF8 transition in terbium. PRL, 135(13), 136101. (www)

  @article{ , abstract = {The lanthanide elements have long been reported as having a common series of structural phase transitions on compression, but recent diffraction studies have revealed two series of transitions: one in the low-Z lanthanides (Nd and Sm) involving an 8-atom orthorhombic structure ( o F 8 ), also seen in some actinide elements, and another in the high-Z lanthanides (Gd, Tb, Dy, and Ho) involving an isosymmetric 16-atom structure ( o F 16 ), unique to the lanthanides. No element has yet been found to exhibit both structures. We have followed the structural evolution of Tb to 308 GPa and find that o F 16 -Tb transforms to o F 8 -Tb at 234 GPa, which is stable to at least 308 GPa. This transition is confirmed by theoretical results which show the o F 8 phase becoming energetically favorable above 280 GPa. This observation of the o F 16 → o F 8 transition unites the two phase-transition sequences and suggests that there is a common o F 16 → o F 8 → o C 4 → t I 2 transition sequence in the lanthanide elements under pressure.}, archive = {J_PRL}, author = {C. V. Storm and S. E. Finnegan and J. D. McHardy and M. J. Duff and M. I. McMahon and S. G. MacLeod and E. Plekhanov and C. Weber}, doi = {10.1103/r3zx-k97x}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136101}, shortjournal = {Phys. Rev. Lett.}, title = {Unified high-pressure phase-transition sequence in the f-electron metals: OF16→oF8 transition in terbium}, volume = {135}, year = {2025}, }
• (2025). Nonlinear planar hall effect from superconducting vortex motion. PRL, 135(13), 136001. (www)

  @article{ , abstract = {We report the nonreciprocal charge transport along the longitudinal and transverse directions in the vortex flow regime of FeSe superconducting films. Clear nonreciprocal signals under an in-plane magnetic field reveal symmetry breaking at the film surfaces, since the crystal structure of FeSe is centrosymmetric. Although the symmetry in such polar superconductors allows the nonreciprocal transverse response under a magnetic field parallel to the electric current, its observation is physically counterintuitive, because vortex motion is not expected in this configuration. We propose that thermally excited (anti)vortices due to the two-dimensional nature of FeSe give rise to the nonreciprocal transverse signals when the mirror symmetry is broken by the in-plane magnetic field.}, archive = {J_PRL}, author = {Mio Hashimoto and Takako Konoike and Tomoki Kobayashi and Shintaro Hoshino and Takuya Kawada and Tomoyuki Yokouchi and Shinya Uji and Atsutaka Maeda and Yuki Shiomi}, doi = {10.1103/4mq6-z8q7}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {136001}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear planar hall effect from superconducting vortex motion}, volume = {135}, year = {2025}, }
• (2025). Vibrational modes and particle rearrangements in sheared quasi-two-dimensional complex plasmas. PRL, 135(13), 135301. (www)

  @article{ , abstract = {In dense colloids and simulated glasses, it has been discovered that plastic particle rearrangements correlate with nonphononic low-frequency vibrational modes. Here, we demonstrate that this correlation also holds for a very different material class of complex plasmas under shear, characterized by long-range interactions and nonreciprocal forces. We perform experiments with a deformed amorphous quasi-two-dimensional binary complex plasma under optical pressure, which gives rise to a controlled shear rate, and confirm our findings with extensive particle-resolved computer simulations.}, archive = {J_PRL}, author = {Yang Miao and Alexei V. Ivlev and Hartmut Löwen and Volodymyr Nosenko and He Huang and Wei Yang and Hubertus M. Thomas and Jing Zhang and Cheng-Ran Du}, doi = {10.1103/6bjy-m2j4}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {135301}, shortjournal = {Phys. Rev. Lett.}, title = {Vibrational modes and particle rearrangements in sheared quasi-two-dimensional complex plasmas}, volume = {135}, year = {2025}, }
• (2025). Generation of relativistic structured spin-polarized lepton beams. PRL, 135(13), 135001. (www)

  @article{ , abstract = {Relativistic structured spin-polarized (SSP) particle beams, characterized by polarization structures, are of critical importance in a wide range of applications, such as material properties investigation, imaging, and information storage. However, the generation of relativistic SSP beams faces significant challenges. Here, we put forward a novel method for generating relativistic SSP lepton beams via employing a state-of-the-art THz source. Building upon our foundational work on velocity-matched spin rotation in dielectric-lined waveguides [ Phys. Rev. Lett. 134 , 075001 (2025) ], we present the first demonstration of spin-polarization mode matching—a novel mechanism that establishes a direct relation between waveguide modes and beam polarization states. This breakthrough enables precise spatial control over spin structures at relativistic energies, generating customizable spin-polarization configurations such as spiderlike, azimuthal, and helical structures. Such SSP beams have the potential to generate high-energy structured photon beams and open a new avenue for research on relativistic structured particle beams, especially in nuclear physics, high-energy physics, materials science, and atomic physics.}, archive = {J_PRL}, author = {Zhong-Peng Li and Yu Wang and Yousef I. Salamin and Mamutjan Ababekri and Feng Wan and Qian Zhao and Kun Xue and Ye Tian and Jian-Xing Li}, doi = {10.1103/sj2g-wvzt}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {135001}, shortjournal = {Phys. Rev. Lett.}, title = {Generation of relativistic structured spin-polarized lepton beams}, volume = {135}, year = {2025}, }
• (2025). Turbulence without walls: Whither the zeroth law of turbulence?. PRL, 135(13), 134001. (www)

  @article{ , abstract = {Experimental and numerical studies of incompressible turbulence suggest that the mean dissipation rate of kinetic energy remains constant as the Reynolds number tends to infinity (or the nondimensional viscosity tends to zero). This anomalous behavior is central to many theories of high-Reynolds-number turbulence and has been termed the “zeroth law” for this reason. Here, we report a sequence of direct numerical simulations of incompressible Navier-Stokes in a box with periodic boundary conditions, which indicate the likelihood that the anomaly vanishes at a rate that agrees with the scaling of third moment of absolute velocity increments. Our results suggest that turbulence without solid boundaries or walls may not develop strong enough singularities to sustain the strict version of the zeroth law.}, archive = {J_PRL}, author = {Kartik P. Iyer and Theodore D. Drivas and Gregory L. Eyink and Katepalli R. Sreenivasan}, doi = {10.1103/xpwj-txlp}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {134001}, shortjournal = {Phys. Rev. Lett.}, title = {Turbulence without walls: Whither the zeroth law of turbulence?}, volume = {135}, year = {2025}, }
• (2025). Universal kerr-thermal dynamics of self-injection-locked microresonator dark pulses. PRL, 135(13), 133803. (www)

  @article{ , abstract = {Microcombs, formed in optical microresonators driven by continuous-wave lasers, are miniaturized optical frequency combs. Leveraging integrated photonics and laser self-injection locking, compact microcombs can be constructed via hybrid integration of a semiconductor laser with a chip-based microresonator. While the current linear self-injection locking theory has successfully addressed the linear coupling between the laser cavity and the external microresonator, it fails to describe the complicated nonlinear processes, especially for dark-pulse microcomb formation. Here, we investigate—theoretically, numerically, and experimentally—the Kerr-thermal dynamics of a semiconductor laser self-injection locked to an integrated silicon nitride microresonator. We unveil intriguing yet universal dark-pulse formation and switching behavior with discrete steps, and establish a theoretical model scrutinizing the synergy of laser-microresonator mutual coupling, Kerr nonlinearity, and photothermal effect. Numerical simulation confirms the experimental result and identifies the origins. Exploiting this unique phenomenon, we showcase an application on low-noise photonic microwave generation with phase noise purified by 23.5 dB. Our study not only adds critical insight of pulse formation in laser-microresonator hybrid systems, but also enables all-passive, photonic-chip-based microwave oscillators with high spectral purity.}, archive = {J_PRL}, author = {Shichang Li and Kunpeng Yu and Dmitry A. Chermoshentsev and Wei Sun and Jinbao Long and Xiaoying Yan and Chen Shen and Artem E. Shitikov and Nikita Yu. Dmitriev and Igor A. Bilenko and Junqiu Liu}, doi = {10.1103/zlqs-yc51}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133803}, shortjournal = {Phys. Rev. Lett.}, title = {Universal kerr-thermal dynamics of self-injection-locked microresonator dark pulses}, volume = {135}, year = {2025}, }
• (2025). Toward chaotic group velocity hopping of an on-chip dissipative kerr soliton. PRL, 135(13), 133802. (www)

  @article{ , abstract = {Chaos enables randomness-based applications, particularly in photonic systems. Integrated optical frequency combs (microcombs) have previously been observed in either chaotic modulation instability or stable, low-noise dissipative Kerr soliton (DKS) regimes. In this Letter, we demonstrate a new microcomb state where a single DKS exhibits chaotic behavior. By phase modulating the Kerr-induced synchronization (KIS) between a DKS and an externally injected reference laser, we observe chaotic group velocity hopping of the soliton, causing random transitions of the repetition rate. Using a chip-integrated octave-spanning microcomb, we experimentally validate the second-order Adler equation describing KIS, allowing us to predict and demonstrate this chaotic DKS hopping. This Letter connects nonlinear dynamics with optical soliton physics, providing a deterministic framework for triggering microcomb chaos in the solitonic state.}, archive = {J_PRL}, author = {Grégory Moille and Sashank Kaushik Sridhar and Pradyoth Shandilya and Avik Dutt and Curtis Menyuk and Kartik Srinivasan}, doi = {10.1103/2k7d-p7rm}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133802}, shortjournal = {Phys. Rev. Lett.}, title = {Toward chaotic group velocity hopping of an on-chip dissipative kerr soliton}, volume = {135}, year = {2025}, }
• (2025). Spontaneous emission decay and excitation in photonic time crystals. PRL, 135(13), 133801. (www)

  @article{ , abstract = {Over the last few decades, the predominant strategies for controlling spontaneous emission have involved tailoring the spatial surroundings of quantum emitters or atoms to create resonant or spatially periodic photonic structures. However, the rise of time-varying photonics has prompted a reevaluation of spontaneous emission in dynamically changing environments, especially within photonic time crystals, where optical properties undergo time-periodic modulation. Here, we apply classical light-matter interaction theory together with Floquet analysis to reveal a substantial enhancement of the spontaneous emission decay rate at the momentum gap frequency in photonic time crystals. Moreover, our findings suggest that photonic time crystals enable a nonequilibrium light-matter interaction process: the spontaneous excitation of an atom from its ground state to an excited state, accompanied by the concurrent emission of a photon, referred to as spontaneous emission excitation.}, archive = {J_PRL}, author = {Jagang Park and Kyungmin Lee and Ruo-Yang Zhang and Hee-Chul Park and Jung-Wan Ryu and Gil Young Cho and Min Yeul Lee and Zhaoqing Zhang and Namkyoo Park and Wonju Jeon and Jonghwa Shin and C. T. Chan and Bumki Min}, doi = {10.1103/5v2w-yg7v}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133801}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous emission decay and excitation in photonic time crystals}, volume = {135}, year = {2025}, }
• (2025). Unraveling dicke superradiant decay with separable coherent spin states. PRL, 135(13), 133602. (www)

  @article{ , abstract = {We show that idealized Dicke superradiant decay from a fully inverted state can at all times be described by a positive statistical mixture of coherent spin states (CSS). Since CSS are separable, this implies that no entanglement is involved in Dicke decay. Based on this result, we introduce a new numerical quantum trajectory approach leading to low-entanglement unravelings. This opens up new possibilities for employing matrix product state (MPS) techniques for large-scale numerical simulations with collective decay processes.}, archive = {J_PRL}, author = {P. Rosario and L. O. R. Solak and A. Cidrim and R. Bachelard and J. Schachenmayer}, doi = {10.1103/xcxr-sm9c}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133602}, shortjournal = {Phys. Rev. Lett.}, title = {Unraveling dicke superradiant decay with separable coherent spin states}, volume = {135}, year = {2025}, }
• (2025). Role of matter interactions in superradiant phenomena. PRL, 135(13), 133601. (www)

  @article{ , abstract = {The superradiant phenomenon, usually described by the Dicke model, is a hallmark of strong light-matter interaction. We explore how matter-matter interactions influence this phenomenon by performing ground-state simulations of Dicke-like models with both isotropic and anisotropic interactions. We find that Ising-type interactions produce two qualitatively distinct phase boundaries, one of which gives rise to an antiferromagnetic-normal phase connected to the superradiant regime via a first-order phase transition. Under anisotropic couplings, we uncover a strongly correlated phase where in-plane spin order coexists with superradiance, exhibiting sublinear scaling of the photon occupation per site and power-law decay of spin correlations. Furthermore, superradiance is strengthened by tuning either isotropic or anisotropic interactions, highlighting the role of intrinsic many-body correlations in shaping light-matter quantum phases.}, archive = {J_PRL}, author = {João Pedro Mendonça and Krzysztof Jachymski and Yao Wang}, doi = {10.1103/z8gv-7yyk}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133601}, shortjournal = {Phys. Rev. Lett.}, title = {Role of matter interactions in superradiant phenomena}, volume = {135}, year = {2025}, }
• (2025). Optical lattice quantum simulator of dynamics beyond born-oppenheimer. PRL, 135(13), 133402. (www)

  @article{ , abstract = {Here, we propose a platform based on ultracold fermionic molecules trapped in optical lattices to simulate nonadiabatic effects, as they appear in certain molecular dynamical problems. The idea consists of a judicious choice of two rotational states as the simulated electronic or nuclear degrees of freedom, in which their dipolar interactions induce the required attractive or repulsive interactions between them. We benchmark our proposal by studying the scattering of an electron or a proton against a hydrogen atom, showing the effect of electronic exchange and inelastic ionization as the mass ratio between the simulated nuclei and electrons—a tunable experimental parameter in our simulator—becomes comparable. These benchmarks illustrate how the simulator can qualitatively emulate phenomena like those appearing in molecular dynamical problems even if the simulated interaction occurs in two dimensions with a dipolar scaling. Beyond the molecular implementation proposed here, our proposal can be readily extrapolated to other atomic platforms, e.g., based on fermionic Rydberg atoms.}, archive = {J_PRL}, author = {Javier Argüello-Luengo and Alejandro González-Tudela and J. Ignacio Cirac}, doi = {10.1103/x5cd-fbj8}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133402}, shortjournal = {Phys. Rev. Lett.}, title = {Optical lattice quantum simulator of dynamics beyond born-oppenheimer}, volume = {135}, year = {2025}, }
• (2025). Precision measurement of spin-dependent dipolar splitting in li6 p-wave feshbach resonances. PRL, 135(13), 133401. (www)

  @article{ , abstract = {The magnetic dipolar splitting of a p -wave Feshbach resonance is governed by the spin-orbital configuration of the valence electrons in the triplet molecular state. We perform high-resolution trap-loss spectroscopy on ultracold Li 6 atoms to resolve this splitting with sub-milligauss precision. By comparing electron-spin-polarized ( | m S | = 1 ) and electron-spin-mixture ( m S = 0 ) configurations of the triplet state, we observe a clear spin-dependent reversal in the splitting structure, confirmed via momentum-resolved absorption imaging. This behavior directly reflects the interplay between electron spin projection m S and orbital angular momentum m ℓ in the molecular states. Our results provide a stringent benchmark for dipole-dipole interaction models and lay the groundwork for controlling the pairing in p -wave superfluid systems.}, archive = {J_PRL}, author = {Shuai Peng and Sijia Peng and Lijun Ren and Shaokun Liu and Bin Liu and Jiaming Li and Le Luo}, doi = {10.1103/5nns-xkt4}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {133401}, shortjournal = {Phys. Rev. Lett.}, title = {Precision measurement of spin-dependent dipolar splitting in li6 p-wave feshbach resonances}, volume = {135}, year = {2025}, }
• (2025). Superfluid density in linear response theory: Pulsar glitches from the inner crust of neutron stars. PRL, 135(13), 132701. (www)

  @article{ , abstract = {The question of whether there are enough superfluid neutrons in the inner crust of neutron stars to explain pulsar glitches remains a topic of debate. Previous band structure calculations suggest that the entrainment effect significantly reduces the superfluid density. In this Letter, a new derivation of the BCS expression for the superfluid density is given. We compute it in the superfluid band theory framework through linear response theory, for a small relative velocity between superfluid and normal components, under the assumption that the pairing gap in the rest frame of the superfluid is constant and not affected by the perturbation. Our result suggests that a formula extensively used in neutron star physics is incomplete. Numerical evaluations for two realistic configurations reveal that the previously neglected contribution drastically alters the picture of the superfluid reservoir in the inner crust of neutron stars, suggesting that about 90% of the neutrons are effectively superfluid.}, archive = {J_PRL}, author = {Giorgio Almirante and Michael Urban}, doi = {10.1103/mg61-gw93}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {132701}, shortjournal = {Phys. Rev. Lett.}, title = {Superfluid density in linear response theory: Pulsar glitches from the inner crust of neutron stars}, volume = {135}, year = {2025}, }
• (2025). Observation of Λ hyperon local polarization in p-pb collisions at sNN=8.16 TeV. PRL, 135(13), 132301. (www)

  @article{ , abstract = {The polarization of the Λ and Λ ¯ hyperons along the beam direction has been measured in proton-lead ( p -Pb ) collisions at a center-of-mass energy per nucleon pair of 8.16 TeV. The data were obtained with the CMS detector at the LHC and correspond to an integrated luminosity of 186.0 ± 6.5 nb − 1 . A significant azimuthal dependence of the hyperon polarization, characterized by the second-order Fourier sine coefficient P z , s 2 , is observed. The P z , s 2 values decrease as a function of charged particle multiplicity, but increase with transverse momentum. A hydrodynamic model that describes the observed P z , s 2 values in nucleus-nucleus collisions by introducing vorticity effects does not reproduce either the sign or the magnitude of the p -Pb results. These observations pose a challenge to the current theoretical implementation of spin polarization in heavy ion collisions and offer new insights into the origin of spin polarization in hadronic collisions at LHC energies.}, archive = {J_PRL}, author = {CMS Collaboration and A. Hayrapetyan and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and T. Van Laer and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and J. Jaramillo and A. Khalilzadeh and F. A. Khan and K. Lee and A. Malara and S. Paredes and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and Y. Hong and J. Knolle and L. Lambrecht and D. Marckx and K. Mota Amarilo and K. Skovpen and N. Van Den Bossche and J. van der Linden and L. Wezenbeek and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and G. A. Alves and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and T. Laux Kuhn and M. Macedo and J. Martins and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and D. Laroze and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and L. Zhang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and K. Yi and J. Zhang and Z. Chen and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and F. Ramirez and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and A. A. Abdelalim and S. Elgammal and A. Ellithi Kamel and M. A. Mahmoud and Y. Mohammed and K. Ehataht and M. Kadastik and T. Lange and S. Nandan and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and H. Kirschenmann and K. Osterberg and M. Voutilainen and S. Bharthuar and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Myllymäki and M. m. Rantanen and H. Siikonen and J. Tuominiemi and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and A. Cappati and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Nguyen and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and I. Bagaturia and I. Lomidze and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and D. Noll and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and A. Stein and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and A. Cardini and C. Cheng and F. Colombina and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and Y. Otarid and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and A. Saggio and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bein and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and T. Chwalek and A. Dierlamm and A. Droll and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and R. Koppenhöfer and O. Lavoryk and J. M. Lawhorn and M. Link and A. Lintuluoto and S. Maier and S. Mitra and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and N. Trevisani and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and P. Kontaxakis and G. Melachroinos and Z. Painesis and I. Papavergou and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and P. Major and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Ahmed and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Baradia and S. Barman and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and T. Mishra and B. Parida and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and V. K. Muraleedharan Nair Bindhu and K. Naskar and A. Nayak and S. Nayak and K. Pal and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and C. Tuve and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and M. Biasotto and P. Bortignon and G. Bortolato and A. Bragagnolo and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and F. Gasparini and U. Gasparini and S. Giorgetti and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and M. Magherini and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and M. Musich and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and C. Baldenegro Barrera and P. Barria and C. Basile and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and R. Gargiulo and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and B. Kim and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and J. Yoo and J. Goh and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and H. Kwon and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and K. Hwang and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and C. A. Mondragon Herrera and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and L. Grzanka and M. Malawski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and S. Sánchez Navas and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and E. Palencia Cortezon and J. Prado Pico and C. Ramón Álvarez and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Bhowmik and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and A. A. Bin Anuar and A. Bocci and L. Borgonovi and C. Botta and E. Brondolin and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and K. A. Wozniak and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and C. Martin Perez and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and U. Kiminsu and Y. Komurcu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and S. Turkcapar and E. Uslan and I. S. Zorbakir and G. Sokmen and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and G. G. Dincer and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and V. J. Smith and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and C. E. Brown and O. Buchmuller and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and C. Cosby and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and L. Gouskos and M. Hadley and U. Heintz and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and D. Li and J. Luo and S. Mondal and T. Russell and S. Sagir and X. Shen and F. Simpson and M. Stamenkovic and N. Venkatasubramanian and X. Yan and S. Abbott and B. Barton and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and S. Yoo and F. Zhang and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and M. Quinnan and B. V. Sathia Narayanan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and S. Wang and D. Zhang and A. Bornheim and O. Cerri and A. Latorre and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and G. Karathanasis and N. Manganelli and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and S. Bright-Thonney and X. Chen and D. J. Cranshaw and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and J. Dickinson and I. Dutta and V. D. Elvira and Y. Feng and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and R. Heller and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and C. Madrid and K. Maeshima and C. Mantilla and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and M. M. Baarmand and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and A. H. Merrit and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and T. Roy and S. Rudrabhatla and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Wang and J. Bendavid and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and B. M. Joshi and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and J. Li and M. Lu and G. Madigan and R. Mccarthy and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and D. Wood and J. Bueghly and S. Dittmer and K. A. Hahn and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. W. Ho and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and D. Stickland and C. Tully and L. H. Vage and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and V. Scheurer and J. F. Schulte and M. Stojanovic and J. Thieman and A. K. Virdi and F. Wang and A. Wildridge and W. Xie and Y. Yao and J. Dolen and N. Parashar and A. Pathak and D. Acosta and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and I. Krommydas and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and J. Reichert and H. Routray and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and H. Wang and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and D. Rathjens and A. Safonov and N. Akchurin and J. Damgov and N. Gogate and V. Hegde and A. Hussain and Y. Kazhykarim and K. Lamichhane and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Neu and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and D. Budkouski and I. Golutvin and I. Gorbunov and V. Karjavine and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and V. Palichik and V. Perelygin and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and V. Smirnov and O. Teryaev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and P. Levchenko and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and Yu. Andreev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and I. Tlisova and A. Toropin and T. Aushev and K. Ivanov and V. Gavrilov and N. Lychkovskaya and A. Nikitenko and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and A. Demiyanov and A. Ershov and A. Gribushin and L. Khein and O. Kodolova and V. Korotkikh and S. Obraztsov and S. Petrushanko and V. Savrin and A. Snigirev and I. Vardanyan and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and Y. Skovpen and V. Kachanov and D. Konstantinov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin}, doi = {10.1103/6ywq-gm61}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {132301}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of Λ hyperon local polarization in p-pb collisions at sNN=8.16 TeV}, volume = {135}, year = {2025}, }
• (2025). Next-to-leading-order QCD corrections to nucleon dirac form factors. PRL, 135(13), 131903. (www)

  @article{ , abstract = {The leading-order perturbative QCD (pQCD) predictions for nucleon electromagnetic form factors were first made in late 1970s. In this Letter, for the first time, we accomplish the calculation of the next-to-leading-order (NLO) QCD corrections to nucleon Dirac form factors at large momentum transfer to leading-twist accuracy in the collinear factorization approach, specifically within the Krankl and Manashov renormalization scheme. The effect of NLO perturbative corrections turns out to be positive and substantial. Taking the nucleon leading-twist light-cone distribution amplitudes determined from the recent lattice simulations as input, we find that the state-of-the-art pQCD predictions significantly underestimate the available nucleon Dirac form factors in both spacelike and timelike domains. This nuisance indicates that some additional soft nonfactorizable contribution might be called for to account for the measured nucleon electromagnetic form factor data up to Q 2 ≈ 30 GeV 2 .}, archive = {J_PRL}, author = {Long-Bin Chen and Wen Chen and Feng Feng and Siwei Hu and Yu Jia}, doi = {10.1103/r25y-rsz5}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131903}, shortjournal = {Phys. Rev. Lett.}, title = {Next-to-leading-order QCD corrections to nucleon dirac form factors}, volume = {135}, year = {2025}, }
• (2025). Nature of χc1(3872) and tcc+(3875). PRL, 135(13), 131902. (www)

  @article{ , abstract = {Two decades ago the χ c 1 ( 3872 ) state was discovered in the hadron spectrum with two heavy quarks. The discovery fueled a surge in experimental research, uncovering dozens of so called X Y Z exotics states lying outside the conventional quark model, as well as theoretical investigations into new forms of matter, such as quark-gluon hybrids, tetraquarks, and pentaquarks, with the potential of disclosing new information about the fundamental strong force. Among the X Y Z s , the χ c 1 ( 3872 ) and T c c + ( 3875 ) states stand out for their striking characteristics and unleashed many discussions about their nature. Here, we address this question using the Born-Oppenheimer effective field theory (BOEFT) and show how QCD settles the issue of their composition. Not only do we describe well the main features of the χ c 1 ( 3872 ) and T c c + ( 3875 ) states, but we also obtain predictions in the bottomonium sector. This opens the way to systematic applications of BOEFT to all X Y Z s .}, archive = {J_PRL}, author = {Nora Brambilla and Abhishek Mohapatra and Tommaso Scirpa and Antonio Vairo}, doi = {10.1103/pdy7-hvg7}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131902}, shortjournal = {Phys. Rev. Lett.}, title = {Nature of χc1(3872) and tcc+(3875)}, volume = {135}, year = {2025}, }
• (2025). QCD theory meets information theory. PRL, 135(13), 131901. (www)

  @article{ , abstract = {We present a novel technique to incorporate precision calculations from quantum chromodynamics into fully differential particle-level Monte Carlo simulations. By minimizing an information-theoretic quantity subject to constraints, our reweighted Monte Carlo incorporates systematic uncertainties absent in individual Monte Carlo predictions, achieving consistency with the theory input in precision and its estimated systematic uncertainties. Our method can be applied to arbitrary observables known from precision calculations, including multiple observables simultaneously. It generates strictly positive weights, thus offering a clear path to statistically powerful and theoretically precise computations for current and future collider experiments. As a proof of concept, we apply our technique to event-shape observables at electron-positron colliders, leveraging existing precision calculations of thrust. Our analysis highlights the importance of logarithmic moments of event shapes, which have not been previously studied in the collider physics literature.}, archive = {J_PRL}, author = {Benoît Assi and Stefan Höche and Kyle Lee and Jesse Thaler}, doi = {10.1103/gf42-qzd9}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131901}, shortjournal = {Phys. Rev. Lett.}, title = {QCD theory meets information theory}, volume = {135}, year = {2025}, }
• (2025). Probing new hadronic forces with heavy exotic atoms. PRL, 135(13), 131803. (www)

  @article{ , abstract = {We explore the potential of precision spectroscopy of heavy exotic atoms where electrons are substituted by negative hadrons to detect new force carriers with hadronic couplings. The selected transitions are unaffected by nuclear contact terms, thus enabling highly accurate calculations using bound-state QED, provided that the nuclear polarization is under control. Alternatively, we demonstrate that the dipole polarizability, a fundamental property of nuclei, can be extracted from the spectroscopy of exotic atoms in a novel way by combining two transitions while maintaining high sensitivity to new physics. Based on existing data, we extracted world-leading bounds on mediator masses ranging from 0.1 to 10 MeV for two benchmark models and show that forthcoming experiments could enhance the sensitivity to new physics by 2 orders of magnitude.}, archive = {J_PRL}, author = {Hongkai Liu and Ben Ohayon and Omer Shtaif and Yotam Soreq}, doi = {10.1103/ndfg-42w7}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131803}, shortjournal = {Phys. Rev. Lett.}, title = {Probing new hadronic forces with heavy exotic atoms}, volume = {135}, year = {2025}, }
• (2025). Muon-decay parameters from COHERENT. PRL, 135(13), 131802. (www)

  @article{ , abstract = {We demonstrate that measurements of coherent elastic neutrino-nucleus scattering at spallation sources are valuable probes of muon-decay physics. Using COHERENT data we derive the first direct constraint on the Michel parameters governing the energy distribution. We also discuss future sensitivities, the implications for the Lorentz structure of the interactions mediating muon decay, and the application to other neutrino-production mechanisms like pion decay.}, archive = {J_PRL}, author = {Víctor Bresó-Pla and Sergio Cruz-Alzaga and Martín González-Alonso and Suraj Prakash}, doi = {10.1103/mlhl-v822}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131802}, shortjournal = {Phys. Rev. Lett.}, title = {Muon-decay parameters from COHERENT}, volume = {135}, year = {2025}, }
• (2025). Search for a dark higgs boson produced in association with inelastic dark matter at the belle II experiment. PRL, 135(13), 131801. (www)

  @article{ , abstract = {Inelastic dark matter models that have two dark matter particles and a massive dark photon can reproduce the observed relic dark matter density without violating cosmological limits. The mass splitting between the two dark matter particles χ 1 and χ 2 , with m ( χ 2 ) > m ( χ 1 ) , is induced by a dark Higgs field and a corresponding dark Higgs boson h ′ . We present a search for dark matter in events with two vertices, at least one of which must be displaced from the interaction region, and missing energy. Using a 365 fb − 1 data sample collected at Belle II, which operates at the SuperKEKB e + e − collider, we observe no evidence for a signal. We set upper limits on the product of the production cross section σ ( e + e − → h ′ χ 1 χ 2 ) , and the product of branching fractions B ( χ 2 → χ 1 e + e − ) × B ( h ′ → x + x − ) , where x + x − indicates μ + μ − , π + π − , or K + K − , as functions of h ′ mass and lifetime at the level of 10 − 1 fb . We set model-dependent upper limits on the dark Higgs mixing angle at the level of 10 − 5 and on the dark photon kinetic mixing parameter at the level of 10 − 3 . This is the first search for dark Higgs bosons in association with inelastic dark matter.}, archive = {J_PRL}, author = {The Belle II Collaboration and I. Adachi and L. Aggarwal and H. Ahmed and H. Aihara and N. Akopov and S. Alghamdi and M. Alhakami and A. Aloisio and N. Althubiti and K. Amos and M. Angelsmark and N. Anh Ky and C. Antonioli and D. M. Asner and H. Atmacan and V. Aushev and M. Aversano and R. Ayad and V. Babu and N. K. Baghel and S. Bahinipati and P. Bambade and Sw. Banerjee and S. Bansal and M. Barrett and M. Bartl and J. Baudot and A. Baur and A. Beaubien and F. Becherer and J. Becker and J. V. Bennett and F. U. Bernlochner and V. Bertacchi and M. Bertemes and E. Bertholet and M. Bessner and S. Bettarini and B. Bhuyan and F. Bianchi and T. Bilka and D. Biswas and A. Bobrov and D. Bodrov and A. Bolz and A. Bondar and G. Bonvicini and J. Borah and A. Boschetti and A. Bozek and M. Bračko and P. Branchini and T. E. Browder and A. Budano and S. Bussino and Q. Campagna and M. Campajola and L. Cao and G. Casarosa and C. Cecchi and J. Cerasoli and M.-C. Chang and R. Cheaib and P. Cheema and Y.-T. Chen and B. G. Cheon and K. Chilikin and J. Chin and K. Chirapatpimol and H.-E. Cho and K. Cho and S.-J. Cho and S.-K. Choi and S. Choudhury and J. Cochran and I. Consigny and L. Corona and J. X. Cui and E. De La Cruz-Burelo and S. A. De La Motte and G. de Marino and G. De Nardo and G. De Pietro and R. de Sangro and M. Destefanis and S. Dey and A. Di Canto and F. Di Capua and J. Dingfelder and Z. Doležal and I. Domínguez Jiménez and T. V. Dong and X. Dong and M. Dorigo and D. Dossett and K. Dugic and G. Dujany and P. Ecker and J. Eppelt and P. Feichtinger and T. Ferber and T. Fillinger and C. Finck and G. Finocchiaro and A. Fodor and F. Forti and B. G. Fulsom and A. Gabrielli and A. Gale and E. Ganiev and M. Garcia-Hernandez and R. Garg and G. Gaudino and V. Gaur and V. Gautam and A. Gaz and A. Gellrich and G. Ghevondyan and D. Ghosh and H. Ghumaryan and G. Giakoustidis and R. Giordano and A. Giri and P. Gironella Gironell and A. Glazov and B. Gobbo and R. Godang and O. Gogota and P. Goldenzweig and W. Gradl and E. Graziani and D. Greenwald and Z. Gruberová and Y. Guan and K. Gudkova and I. Haide and Y. Han and T. Hara and C. Harris and K. Hayasaka and H. Hayashii and S. Hazra and C. Hearty and M. T. Hedges and A. Heidelbach and I. Heredia de la Cruz and M. Hernández Villanueva and T. Higuchi and M. Hoek and M. Hohmann and R. Hoppe and P. Horak and C.-L. Hsu and T. Humair and T. Iijima and K. Inami and G. Inguglia and N. Ipsita and A. Ishikawa and R. Itoh and M. Iwasaki and P. Jackson and D. Jacobi and W. W. Jacobs and E.-J. Jang and Q. P. Ji and S. Jia and Y. Jin and A. Johnson and K. K. Joo and H. Junkerkalefeld and A. B. Kaliyar and J. Kandra and K. H. Kang and G. Karyan and T. Kawasaki and F. Keil and C. Ketter and C. Kiesling and C.-H. Kim and D. Y. Kim and J.-Y. Kim and K.-H. Kim and Y. J. Kim and Y.-K. Kim and H. Kindo and K. Kinoshita and P. Kodyš and T. Koga and S. Kohani and K. Kojima and A. Korobov and S. Korpar and E. Kovalenko and R. Kowalewski and P. Križan and P. Krokovny and T. Kuhr and Y. Kulii and D. Kumar and R. Kumar and K. Kumara and T. Kunigo and A. Kuzmin and Y.-J. Kwon and S. Lacaprara and K. Lalwani and T. Lam and L. Lanceri and J. S. Lange and T. S. Lau and M. Laurenza and R. Leboucher and F. R. Le Diberder and M. J. Lee and C. Lemettais and P. Leo and H.-J. Li and L. K. Li and Q. M. Li and W. Z. Li and Y. Li and Y. B. Li and Y. P. Liao and J. Libby and J. Lin and S. Lin and M. H. Liu and Q. Y. Liu and Y. Liu and Z. Q. Liu and D. Liventsev and S. Longo and T. Lueck and T. Luo and C. Lyu and Y. Ma and C. Madaan and M. Maggiora and S. P. Maharana and R. Maiti and G. Mancinelli and R. Manfredi and E. Manoni and M. Mantovano and D. Marcantonio and S. Marcello and C. Marinas and C. Martellini and A. Martens and A. Martini and T. Martinov and L. Massaccesi and M. Masuda and K. Matsuoka and D. Matvienko and S. K. Maurya and M. Maushart and J. A. McKenna and R. Mehta and F. Meier and D. Meleshko and M. Merola and C. Miller and M. Mirra and S. Mitra and K. Miyabayashi and H. Miyake and R. Mizuk and G. B. Mohanty and S. Mondal and S. Moneta and A. L. Moreira de Carvalho and H.-G. Moser and R. Mussa and I. Nakamura and M. Nakao and H. Nakazawa and Y. Nakazawa and M. Naruki and Z. Natkaniec and A. Natochii and M. Nayak and G. Nazaryan and M. Neu and S. Nishida and S. Ogawa and R. Okubo and H. Ono and Y. Onuki and G. Pakhlova and S. Pardi and K. Parham and H. Park and J. Park and K. Park and S.-H. Park and B. Paschen and A. Passeri and S. Patra and S. Paul and T. K. Pedlar and I. Peruzzi and R. Peschke and R. Pestotnik and M. Piccolo and L. E. Piilonen and P. L. M. Podesta-Lerma and T. Podobnik and S. Pokharel and A. Prakash and C. Praz and S. Prell and E. Prencipe and M. T. Prim and S. Privalov and I. Prudiiev and H. Purwar and P. Rados and G. Raeuber and S. Raiz and K. Ravindran and J. U. Rehman and M. Reif and S. Reiter and M. Remnev and L. Reuter and D. Ricalde Herrmann and I. Ripp-Baudot and G. Rizzo and S. H. Robertson and M. Roehrken and J. M. Roney and A. Rostomyan and N. Rout and L. Salutari and D. A. Sanders and S. Sandilya and L. Santelj and V. Savinov and B. Scavino and J. Schmitz and S. Schneider and M. Schnepf and C. Schwanda and Y. Seino and A. Selce and K. Senyo and J. Serrano and M. E. Sevior and C. Sfienti and W. Shan and G. Sharma and C. P. Shen and X. D. Shi and T. Shillington and T. Shimasaki and J.-G. Shiu and D. Shtol and B. Shwartz and A. Sibidanov and F. Simon and J. B. Singh and J. Skorupa and R. J. Sobie and M. Sobotzik and A. Soffer and A. Sokolov and E. Solovieva and W. Song and S. Spataro and B. Spruck and M. Starič and P. Stavroulakis and S. Stefkova and R. Stroili and J. Strube and Y. Sue and M. Sumihama and K. Sumisawa and N. Suwonjandee and H. Svidras and M. Takahashi and M. Takizawa and U. Tamponi and K. Tanida and F. Tenchini and A. Thaller and O. Tittel and R. Tiwary and E. Torassa and K. Trabelsi and I. Tsaklidis and M. Uchida and I. Ueda and T. Uglov and K. Unger and Y. Unno and K. Uno and S. Uno and P. Urquijo and Y. Ushiroda and S. E. Vahsen and R. van Tonder and K. E. Varvell and M. Veronesi and A. Vinokurova and V. S. Vismaya and L. Vitale and V. Vobbilisetti and R. Volpe and A. Vossen and M. Wakai and S. Wallner and M.-Z. Wang and A. Warburton and M. Watanabe and S. Watanuki and C. Wessel and E. Won and X. P. Xu and B. D. Yabsley and S. Yamada and W. Yan and W. C. Yan and S. B. Yang and J. Yelton and J. H. Yin and K. Yoshihara and J. Yuan and L. Zani and F. Zeng and M. Zeyrek and B. Zhang and V. Zhilich and J. S. Zhou and Q. D. Zhou and L. Zhu and R. Žlebčík}, doi = {10.1103/37w5-glpp}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for a dark higgs boson produced in association with inelastic dark matter at the belle II experiment}, volume = {135}, year = {2025}, }
• (2025). Recursive landau analysis. PRL, 135(13), 131603. (www)

  @article{ , abstract = {We propose a recursive method that makes use of the basic principle of unitarity to calculate the Landau singularities of n -point scattering amplitudes directly in kinematic space. For a vast class of Feynman diagrams, the method enables rapid analytic computation of Landau singularities beyond current state-of-the-art technology. This includes new predictions relevant for two- and higher-loop processes in the standard model involving both massive quarks and electroweak particles.}, archive = {J_PRL}, author = {Simon Caron-Huot and Miguel Correia and Mathieu Giroux}, doi = {10.1103/8rwk-bnph}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131603}, shortjournal = {Phys. Rev. Lett.}, title = {Recursive landau analysis}, volume = {135}, year = {2025}, }
• (2025). Bondi-metzner-sachs particles. PRL, 135(13), 131602. (www)

  @article{ , abstract = {We construct wave functions for unitary irreducible representations (UIRs) of the Bondi-Metzner-Sachs (BMS) group, i.e., BMS particles, and show that they describe quantum superpositions of (Poincaré) particles propagating on inequivalent gravity vacua. This follows from reconsidering McCarthy’s classification of BMS group UIRs through a unique, Lorentz-invariant, but nonlinear, decomposition of supermomenta into hard and soft pieces.}, archive = {J_PRL}, author = {Xavier Bekaert and Laura Donnay and Yannick Herfray}, doi = {10.1103/8376-fync}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131602}, shortjournal = {Phys. Rev. Lett.}, title = {Bondi-metzner-sachs particles}, volume = {135}, year = {2025}, }
• (2025). Emergence of unitarity and locality from hidden zeros at one-loop order. PRL, 135(13), 131601. (www)

  @article{ , abstract = {Recent investigations into the geometric structure of scattering amplitudes have revealed the surprising existence of “hidden zeros”: secret kinematic loci where tree-level amplitudes in Tr ( ϕ 3 ) theory, the nonlinear sigma model (NLSM), and Yang-Mills theory vanish. In this Letter, we propose the extension of hidden zeros to one-loop order in Tr ( ϕ 3 ) theory and the NLSM using the “surface integrand” technology introduced by Arkani-Hamed et al. We demonstrate that, under the assumption of locality, one-loop integrands in Tr ( ϕ 3 ) are unitary if and only if they satisfy these loop hidden zeros. We also present strong evidence that the hidden zeros themselves contain the constraints from locality, leading us to conjecture that the one-loop Tr ( ϕ 3 ) integrand can be fixed by hidden zeros from a generically nonlocal, nonunitary Ansatz . Near the one-loop zeros, we uncover a simple factorization behavior and conjecture that NLSM integrands are fixed by this property, also assuming neither locality nor unitarity. This Letter represents the first extension of such uniqueness results to loop integrands, demonstrating that locality and unitarity emerge from other principles even beyond leading order in perturbation theory.}, archive = {J_PRL}, author = {Jeffrey V. Backus and Laurentiu Rodina}, doi = {10.1103/7lwk-m5yb}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131601}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of unitarity and locality from hidden zeros at one-loop order}, volume = {135}, year = {2025}, }
• (2025). Long-term stable nonlinear evolutions of ultracompact black-hole mimickers. PRL, 135(13), 131402. (www)

  @article{ , abstract = {We study the stability of ultracompact boson stars admitting light rings combining a perturbative analysis with 3 + 1 numerical-relativity simulations with and without symmetry assumptions. We observe excellent agreement between all perturbative and numerical results, which uniformly support the hypothesis that this family of black-hole mimickers is separated into stable and unstable branches by extremal-mass configurations. This separation includes, in particular, thin-shell boson stars with light rings located on the stable branch, which we conclude to represent long-term stable black-hole mimickers.}, archive = {J_PRL}, author = {Gareth Arturo Marks and Seppe J. Staelens and Tamara Evstafyeva and Ulrich Sperhake}, doi = {10.1103/lk48-7r2f}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131402}, shortjournal = {Phys. Rev. Lett.}, title = {Long-term stable nonlinear evolutions of ultracompact black-hole mimickers}, volume = {135}, year = {2025}, }
• (2025). First law of binary black hole scattering. PRL, 135(13), 131401. (www)

  @article{ , abstract = {In the last decade, the first law of binary black hole mechanics played an important unifying role in the gravitational two-body problem. More recently, binary black hole scattering and the application of high-energy physics methods have provided a new avenue into this classical problem. In this Letter, we connect these two themes by extending the first law to the case of scattering orbits. We present derivations based on classical S-matrix, Hamiltonian, and pseudo-Hamiltonian methods, the last of which allows us to include dissipative effects for the first time. Finally, a “boundary to bound” map links this first law to the traditional bound-orbit version. Through this map a little-known observable for scatter orbits, the elapsed proper time, is mapped to the Detweiler redshift for bound orbits, which is an invariant building block in gravitational waveform models.}, archive = {J_PRL}, author = {Riccardo Gonzo and Jack Lewis and Adam Pound}, doi = {10.1103/s85p-gh7b}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131401}, shortjournal = {Phys. Rev. Lett.}, title = {First law of binary black hole scattering}, volume = {135}, year = {2025}, }
• (2025). Nailing down the theoretical uncertainties of d¯ spectrum produced from dark matter. PRL, 135(13), 131002. (www)

  @article{ , abstract = {The detection of cosmic antideuterons ( D ¯ ) at kinetic energies below a few GeV / n could provide a smoking gun signature for dark matter (DM). However, the theoretical uncertainties of coalescence models have represented so far one of the main limiting factors for precise predictions of the D ¯ flux. In this Letter, we present a novel calculation of the D ¯ source spectra, based on the Wigner formalism, for which we implement the Argonne v 18 antideuteron wave function that does not have any free parameters related to the coalescence process. We show that the Argonne-Wigner model excellently reproduces the D ¯ multiplicity measured by ALEPH at the Z -boson pole, which is usually adopted to tune the coalescence models based on different approaches. Our analysis is based on the p ythia 8 Monte Carlo event generator and the state-of-the-art shower algorithm. We succeed, with our model, to reduce the current theoretical uncertainty on the prediction of the D ¯ source spectra to a few percent, for D ¯ kinetic energies relevant to DM searches with the General Antiparticle Spectrometer and Alpha Magnetic Spectrometer, and for DM masses above a few tens of GeV. This result implies that the theoretical uncertainties due to the coalescence process are no longer the main limiting factor in the predictions. We provide the tabulated source spectra for all the relevant DM annihilation and decay channels and DM masses between 5 and 100 TeV, on the CosmiXs GitHub repository.}, archive = {J_PRL}, author = {Mattia Di Mauro and Nicolao Fornengo and Adil Jueid and Roberto Ruiz de Austri and Francesca Bellini}, doi = {10.1103/w6n5-vs4d}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131002}, shortjournal = {Phys. Rev. Lett.}, title = {Nailing down the theoretical uncertainties of d¯ spectrum produced from dark matter}, volume = {135}, year = {2025}, }
• (2025). New limits on ultralight axionlike dark matter from reanalyzed data. PRL, 135(13), 131001. (www)

  @article{ , abstract = {New limits on the axion-nucleon coupling over the axion mass region 10 − 24 ≤ m a ≤ 5 × 10 − 21 eV are derived by reanalyzing data from laboratory measurements on Lorentz and C P T violations. These results establish the first laboratory constraints on the axion-nucleon coupling for axion masses below 10 − 22 eV . For 10 − 22 ≤ m a ≤ 5 × 10 − 21 eV , the results improve upon previous laboratory limits by more than three orders of magnitude, exceeding for the first time the astrophysical limits from supernova SN1987A cooling. For the axion mass range of interest corresponding to ultralow frequencies, the crucial local phase of the axion field is considered. Furthermore, the obtained limits are nearly equivalent to those projected for a recently proposed experiment employing high-intensity neutron beams at the European Spallation Source. For an alternative type of axion-nucleon interaction, the quadratic wind coupling, the constraints exceed the current best results by approximately two orders of magnitude.}, archive = {J_PRL}, author = {K. Y. Zhang and L. Y. Wu and H. Yan}, doi = {10.1103/l8kd-yhlg}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {131001}, shortjournal = {Phys. Rev. Lett.}, title = {New limits on ultralight axionlike dark matter from reanalyzed data}, volume = {135}, year = {2025}, }
• (2025). Deterministic nonlocal quantum gate with room-temperature memory modules. PRL, 135(13), 130806. (www)

  @article{ , abstract = {Scaling quantum computation is a crucial challenge for practical applications, hindered by the inherent errors and noises in real-world quantum systems. The quantum modular architecture offers a possible solution, where smaller quantum modules are individually constructed and assembled into a larger architecture. In this architecture, the nonlocal quantum gates are the building blocks; until now, it has remained challenging for practical applications to implement a nonlocal quantum gate with the memory modules under deterministic and room-temperature conditions, due to intrinsic probability and hardware complexity. Here, we propose and demonstrate a scheme to deterministically implement a nonlocal quantum gate between the room-temperature memory modules. The key technologies include cavity-enhanced atomic modules, two of which are connected by a single pair of distributed entangled optical modes and real-time mutual feedforward controls. The nonlocal quantum nondemolition gate between two room-temperature memory modules is deterministically demonstrated with different input coherent states, and the quantum nature is confirmed by outputting entangled atomic modules. Our results illustrate the functionality and feasibility of nonlocal quantum gate and may have potential applications in modular quantum information processing.}, archive = {J_PRL}, author = {Xing Lei and Jiatong Li and Xiaoyu Zhou and Jieli Yan and Minwen Ji and Zhihui Yan and Xiaojun Jia and Changde Xie and Kunchi Peng}, doi = {10.1103/xt77-2gpw}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130806}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic nonlocal quantum gate with room-temperature memory modules}, volume = {135}, year = {2025}, }
• (2025). Practical advantage of classical communication in entanglement detection. PRL, 135(13), 130805. (www)

  @article{ , abstract = {Entanglement is the cornerstone of quantum communication, yet conventional detection relies solely on local measurements. In this Letter, we present an experimental demonstration, based on an improved theoretical framework showing that one-way local operations and classical communication (1-LOCC) can significantly outperform purely local measurements in detecting quantum entanglement. By casting the entanglement detection problem as a semidefinite program, we derive protocols that minimize false negatives at fixed false-positive rates. A variational generative machine-learning algorithm efficiently searches over high-dimensional parameter spaces, identifying states and measurement strategies that exhibit a clear 1-LOCC advantage. Experimentally, we realize a genuine event-ready protocol on a three-dimensional photonic entanglement source, employing fiber delays as short-lived quantum memories. We implement rapid, field-programmable gate array-based sampling of the optimized probabilistic instructions, allowing Bob’s measurement settings to adapt to Alice’s outcomes in real time. Our results validate the predicted 1-LOCC advantage in a realistic noisy setting and reduce the experimental trials needed to certify entanglement. These findings mark a step toward scalable, adaptive entanglement detection methods crucial for quantum networks and computing, paving the way for more efficient generation and verification of high-dimensional entangled states.}, archive = {J_PRL}, author = {Wen-Bo Xing (邢文博 and Min-Yu Lv (吕敏玉 and Lingxia Zhang (张凌霞 and Yu Guo (郭钰 and Mirjam Weilenmann and Zhaohui Wei (魏朝晖 and Chuan-Feng Li (李传锋 and Guang-Can Guo (郭光灿 and Xiao-Min Hu (胡晓敏 and Bi-Heng Liu (柳必恒 and Miguel Navascués and Zizhu Wang (王子竹}, doi = {10.1103/hlcv-qcnw}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130805}, shortjournal = {Phys. Rev. Lett.}, title = {Practical advantage of classical communication in entanglement detection}, volume = {135}, year = {2025}, }
• (2025). Constant-overhead fault-tolerant bell-pair distillation using high-rate codes. PRL, 135(13), 130804. (www)

  @article{ , abstract = {We present a fault-tolerant Bell-pair distillation scheme achieving constant overhead through high-rate quantum low-density parity-check (qLDPC) codes. Our approach maintains a constant distillation rate equal to the code rate while requiring no additional overhead beyond the physical qubits of the code. Full circuit-level analysis demonstrates fault-tolerance for input Bell-pair infidelities below a threshold , readily achievable with near-term capabilities. Unlike previous proposals, our scheme keeps the output Bell pairs encoded in qLDPC codes at each node, eliminating unencoding overhead and enabling direct use in distributed quantum applications through recent advances in qLDPC computation. These results establish qLDPC-based distillation as a practical route toward resource-efficient quantum networks and distributed quantum computing.}, archive = {J_PRL}, author = {J. Pablo Bonilla Ataides and Hengyun Zhou and Qian Xu and Gefen Baranes and Bikun Li and Mikhail D. Lukin and Liang Jiang}, doi = {10.1103/s39k-r2kq}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130804}, shortjournal = {Phys. Rev. Lett.}, title = {Constant-overhead fault-tolerant bell-pair distillation using high-rate codes}, volume = {135}, year = {2025}, }
• (2025). Measurement-based entanglement distillation and constant-rate quantum repeaters over arbitrary distances. PRL, 135(13), 130803. (www)

  @article{ , abstract = {Measurement-based quantum repeaters employ entanglement distillation and swapping across links using locally prepared resource states of minimal size and local Bell measurements. In this Letter, we introduce a systematic protocol for measurement-based entanglement distillation and its application to repeaters that can leverage any stabilizer code. Given a code, we explicitly define the corresponding resource state and derive an error-recovery operation based on all Bell measurement outcomes. Our approach offers deeper insights into the impact of resource state noise on repeater performance while also providing strategies for efficient preparation and fault-tolerant preservation of resource states. As an application, we propose a measurement-based repeater protocol based on quantum low-density parity-check (QLDPC) codes, enabling constant-yield Bell state distribution over arbitrary distances. Numerical simulations identify a fault-tolerant threshold on the total physical error per repeater segment—including errors on resource states, remotely generated Bell states, and Bell measurements—and confirm that increasing the QLDPC code size further suppresses the logical error while maintaining a fixed encoding rate. This Letter establishes a scalable backbone for future global-scale fault-tolerant quantum networks.}, archive = {J_PRL}, author = {Yu Shi and Ashlesha Patil and Saikat Guha}, doi = {10.1103/2bp8-cdxc}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130803}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement-based entanglement distillation and constant-rate quantum repeaters over arbitrary distances}, volume = {135}, year = {2025}, }
• (2025). Quantum-optimal frequency estimation of stochastic ac fields. PRL, 135(13), 130802. (www)

  @article{ , abstract = {Resolving frequencies in a time-dependent field is classically limited by the measurement bandwidth. Using tools from quantum metrology and quantum control may overcome this limit, yet the full advantage afforded by entanglement so far remains elusive. Here we map the problem of frequency measurement to that of estimating a global dephasing quantum channel. In this way, we determine the ultimate quantum limits of frequency estimation in stochastic ac sensing. We find exact quantum Fisher information bounds for estimating frequency and frequency differences of stochastic fields. In particular, given two close signals with frequency separation ω r , we find that the quantum Fisher information for the separation estimation is approximately 2 / ω r 2 , i.e., inversely proportional to the separation parameter. The bounds are achievable in certain regimes by superpositions of Dicke states. GHZ states are suboptimal but improve precision over unentangled states, achieving Heisenberg scaling in the low-bandwidth limit. This Letter establishes a robust framework for stochastic ac signal sensing that can be extended to arbitrary time-dependent and stochastic fields.}, archive = {J_PRL}, author = {Anirban Dey and Sara Mouradian and Cosmo Lupo and Zixin Huang}, doi = {10.1103/v4x6-2dzs}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130802}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-optimal frequency estimation of stochastic ac fields}, volume = {135}, year = {2025}, }
• (2025). Universal bounds for quantum metrology in the presence of correlated noise. PRL, 135(13), 130801. (www)

  @article{ , abstract = {We derive fundamental bounds for general quantum metrological models involving both temporal or spatial correlations (mathematically described by quantum combs), which may be effectively computed in the limit of a large number of probes or sensing channels involved. Although the bounds are not guaranteed to be tight in general, their tightness may be systematically increased by increasing the numerical complexity of the procedure. Interestingly, this approach yields bounds tighter than the state of the art also for uncorrelated channels. We apply the bounds to study the limits for the most general adaptive phase estimation models in the presence of temporally correlated dephasing. We consider dephasing both parallel (no Heisenberg scaling) and perpendicular (Heisenberg scaling possible) to the signal. In the former case our new bounds show that negative correlations are beneficial; for the latter we show evidence that the bounds are tight. We also apply the bounds to collisional thermometry, i.e., estimation of a parameter of the environment, showing evidence that entangled probes may provide only a limited advantage.}, archive = {J_PRL}, author = {Stanisław Kurdziałek and Francesco Albarelli and Rafał Demkowicz-Dobrzański}, doi = {10.1103/jy3v-wkcb}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130801}, shortjournal = {Phys. Rev. Lett.}, title = {Universal bounds for quantum metrology in the presence of correlated noise}, volume = {135}, year = {2025}, }
• (2025). Trotterization is substantially efficient for low-energy states. PRL, 135(13), 130602. (www)

  @article{ , abstract = {Trotterization is one of the central approaches for simulating quantum many-body dynamics on quantum computers or tensor networks. In addition to its simple implementation, recent studies have revealed that its error and cost can be reduced if the initial state is closed in the low-energy subspace. However, the improvement by the low-energy property diminishes rapidly as the Trotter order grows in the previous studies, and thus, it is mysterious whether there exists a genuine advantage of low-energy initial states. In this Letter, we resolve this problem by proving the optimal error bound and cost of Trotterization for low-energy initial states. For generic local Hamiltonians composed of positive-semidefinite terms, we show that the Trotter error is at most linear in the initial state energy and polylogarithmic in the system size . As a result, the computational cost becomes substantially small for low-energy states with compared to the one for arbitrary initial states, where denotes the energy per site and means the whole-system energy. Our error bound and cost of Trotterization achieve the theoretically best scaling in the initial state energy . In addition, they can be partially extended to weakly correlated initial states having low-energy expectation values, which are not necessarily closed in the low-energy subspace. Our results will pave the way for fast and accurate simulations of low-energy states, which are one of the central targets in condensed matter physics and quantum chemistry.}, archive = {J_PRL}, author = {Kaoru Mizuta and Tomotaka Kuwahara}, doi = {10.1103/q87n-5xhz}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130602}, shortjournal = {Phys. Rev. Lett.}, title = {Trotterization is substantially efficient for low-energy states}, volume = {135}, year = {2025}, }
• (2025). Active leakage cancellation in single qubit gates. PRL, 135(13), 130601. (www)

  @article{ , abstract = {The ability to perform fast and accurate rotations between the computational basis states of quantum bits is one of the most fundamental requirements for building a quantum computer. Because physical qubits generally contain more than two levels, faster gates often result in a higher leakage rate outside of the computational space. In this Letter, we enhance the state-of-the-art single qubit gate by introducing active leakage cancellation. This is accomplished via a second drive tone near the leakage transition such that we cancel the leakage caused by the main drive. Furthermore, we describe a measurement sequence that can be used to calibrate the parameters of this leakage cancellation drive. Finally, we apply the technique to superconducting transmon qubits and achieve leakage suppression by up to a factor of 20 when compared to pulses shaped with the standard derivative removal by adiabatic gate technique. This results in a coherence-limited gate infidelity of 7.5 × 10 − 5 with leakage below 10 − 5 level, for a 10 ns π / 2 gate and 196 MHz qubit anharmonicity.}, archive = {J_PRL}, author = {Ben Chiaro and Yaxing Zhang}, doi = {10.1103/4kz9-w97h}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130601}, shortjournal = {Phys. Rev. Lett.}, title = {Active leakage cancellation in single qubit gates}, volume = {135}, year = {2025}, }
• (2025). Quantum work statistics across a critical point: Full crossover from sudden quench to the adiabatic limit. PRL, 135(13), 130402. (www)

  @article{ , abstract = {When an external parameter drives a system across a quantum phase transition at a finite rate, work is performed on the system and entropy is dissipated, due to creation of excitations via the Kibble-Zurek mechanism. Although both the adiabatic and sudden-quench limits have been studied in detail, the quantum work statistics along the crossover connecting these limits has largely been an open question. Here, we obtain exact scaling functions for the work statistics along the full crossover from adiabatic to sudden-quench limits for critical quantum impurity problems, by combining linear response theory, conformal field theory, and the numerical renormalization group. These predictions can be tested in charge-multichannel Kondo quantum dot devices, where the dissipated work corresponds to the creation of nontrivial excitations such as Majorana fermions or Fibonacci anyons.}, archive = {J_PRL}, author = {Zhanyu Ma and Andrew K. Mitchell and Eran Sela}, doi = {10.1103/vn83-mt2v}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130402}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum work statistics across a critical point: Full crossover from sudden quench to the adiabatic limit}, volume = {135}, year = {2025}, }
• (2025). Accurate gauge-invariant tensor-network simulations for abelian lattice gauge theory in (2+1)D: Ground-state and real-time dynamics. PRL, 135(13), 130401. (www)

  @article{ , abstract = {We propose a novel tensor-network method to achieve accurate and efficient simulations of Abelian lattice gauge theories (LGTs) in ( 2 + 1 ) D for both ground-state and real-time dynamics. The first key is to identify a gauge canonical form of gauge-invariant tensor-network states, which already simplifies existing algorithms for ( 1 + 1 ) D LGTs. The second key is to employ the gauge canonical form of a projected entangled-pair state (PEPS) combining with variational Monte Carlo, enabling efficient computations for ( 2 + 1 ) D LGTs. We demonstrate the versatile capability of this approach for accurate ground-state simulation of pure Z 2 , Z 3 , and Z 4 gauge theory, odd- Z 2 gauge theories, and Z 2 gauge theory coupled to hard-core bosons, on square lattices up to 32 × 32 . Furthermore, we demonstrate that it allows for accurate simulations of real-time dynamics up to long time, exemplified by the dynamics of elementary excitations of the deconfined Z 2 gauge field at 10 × 10 . This is also the first example of simulating the real-time dynamics of PEPS with variational Monte Carlo, whose impact may extend beyond gauge theory. Our Letter establishes gauge-invariant PEPS as a powerful approach for both ground-state and dynamical simulations, opening up a new avenue for nonperturbatively studying ( 2 + 1 ) D LGTs.}, archive = {J_PRL}, author = {Yantao Wu and Wen-Yuan Liu}, doi = {10.1103/3m3j-ds18}, journal = {Physical Review Letters}, month = {9}, number = {13}, pages = {130401}, shortjournal = {Phys. Rev. Lett.}, title = {Accurate gauge-invariant tensor-network simulations for abelian lattice gauge theory in (2+1)D: Ground-state and real-time dynamics}, volume = {135}, year = {2025}, }
• (2025). Shape switching and tunable oscillations of adaptive droplets. PRL, 135(12), 128404. (www)

  @article{ , abstract = {Living materials adapt their shape to signals from the environment, yet the impact of shape changes on signal processing and associated feedback dynamics remains unclear. We find that droplets with signal-responsive interfacial tensions exhibit shape bistability, excitable dynamics, and oscillations. The underlying critical points reveal novel mechanisms for physical signal processing through shape adaptation in soft active materials. We recover signatures of one such critical point in experimental data from zebrafish embryos, where it supports boundary formation.}, archive = {J_PRL}, author = {Tim Dullweber and Roman Belousov and Camilla Autorino and Nicoletta I. Petridou and Anna Erzberger}, doi = {10.1103/1cq4-x499}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {128404}, shortjournal = {Phys. Rev. Lett.}, title = {Shape switching and tunable oscillations of adaptive droplets}, volume = {135}, year = {2025}, }
• (2025). Three-dimensional chiral active ornstein-uhlenbeck model for helical motion of microorganisms. PRL, 135(12), 128403. (www)

  @article{ , abstract = {Active movement is essential for the survival of microorganisms like bacteria, algae, and unicellular parasites. In three dimensions, both swimming and gliding microorganisms often exhibit helical trajectories. One such case are malaria parasites gliding through 3D hydrogels, for which we find that the internal correlation time for the stochastic process generating propulsion is similar to the time taken for one helical turn. Motivated by this experimental finding, here we theoretically analyze the case of finite internal correlation time for microorganisms with helical trajectories as chiral active particles with an Ornstein-Uhlenbeck process for torque. We present an analytical solution which is in very good agreement with computer simulations. We then show that, for this type of internal noise, chirality and rotation increase the persistence of motion and results in helical trajectories that have a larger long-time mean squared displacement than straight trajectories at the same propulsion speed. Finally, we provide experimental evidence for this prediction for the case of malaria parasites.}, archive = {J_PRL}, author = {Leon Lettermann and Falko Ziebert and Mirko Singer and Friedrich Frischknecht and Ulrich S. Schwarz}, doi = {10.1103/4kxb-h6p4}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {128403}, shortjournal = {Phys. Rev. Lett.}, title = {Three-dimensional chiral active ornstein-uhlenbeck model for helical motion of microorganisms}, volume = {135}, year = {2025}, }
• (2025). Strings, branes and twistons: Topological analysis of phase defects in excitable media such as the heart. PRL, 135(12), 128402. (www)

  @article{ , abstract = {Several excitable systems, such as the heart, self-organize into complex spatiotemporal patterns that involve wave collisions and rotating vortices. The dynamics between these structures are incompletely understood. Here we establish a comprehensive topological framework in three spatial dimensions. Conduction blocks are identified as phase defect surfaces, on which three types of closed curves move and carry a topological vector charge. Our framework not only sheds new light on twistons and hybrid reentry but also predicts new states: a Möbius scroll wave and conduction block surfaces that can split, branch, or contain multiple filaments. We hypothesize that the latter play a role in cardiac arrhythmias.}, archive = {J_PRL}, author = {Louise Arno and Desmond Kabus and Hans Dierckx}, doi = {10.1103/5pgp-1wj6}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {128402}, shortjournal = {Phys. Rev. Lett.}, title = {Strings, branes and twistons: Topological analysis of phase defects in excitable media such as the heart}, volume = {135}, year = {2025}, }
• (2025). Motility modulates the partitioning of bacteria in aqueous two-phase systems. PRL, 135(12), 128401. (www)

  @article{ , abstract = {We study the partitioning of motile bacteria in an aqueous two-phase mixture of dextran (DEX) and polyethylene glycol (PEG), which can phase separate into DEX-rich and PEG-rich phases. While nonmotile bacteria partition exclusively into the DEX-rich phase in all conditions tested, we observed that motile bacteria penetrate the soft DEX-PEG interface and partition variably among the two phases. For our model organism Bacillus subtilis , the fraction of motile bacteria in the DEX-rich phase increased from 0.58 to 1 as we increased the DEX composition within the two-phase region. We hypothesized that the chemical affinity between DEX and the bacteria cell wall acts to weakly confine the bacteria within the DEX-rich phase; however, motility can generate sufficient mechanical forces to overcome the soft confinement and propel the bacteria into the PEG-rich phase. Using optical tweezers to drag a bacterium across the DEX-PEG interface, we demonstrate that the overall bacteria partitioning is determined by a competition between the interfacial forces and bacterial propulsive forces. Our measurements are supported by a theoretical model of dilute active rods embedded within a periodic soft confinement potential.}, archive = {J_PRL}, author = {Jiyong Cheon and Kyu Hwan Choi and Kevin J. Modica and Robert J. Mitchell and Sho C. Takatori and Joonwoo Jeong}, doi = {10.1103/6gm5-cnv1}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {128401}, shortjournal = {Phys. Rev. Lett.}, title = {Motility modulates the partitioning of bacteria in aqueous two-phase systems}, volume = {135}, year = {2025}, }
• (2025). Topological rigidity in twisted, elastic ribbons. PRL, 135(12), 128201. (www)

  @article{ , abstract = {Topology is an important determinant of the behavior of a great number of condensed-matter systems, but until recently it has played a minor role in elasticity. We develop a theory for the deformations of a class of twisted non-Euclidean sheets, which have a symmetry based on the celebrated Bonnet isometry. We show that nonorientability is an obstruction to realizing the symmetry globally, and it induces a geometric phase that captures a memory analogous to a previously identified one in 2D metamaterials. However, we show that orientable ribbons can also obstruct realizing the symmetry globally. This new obstruction is mediated by how the unit normal vector winds around the centerline of the ribbon and provides conditions for constructing soft modes of deformation compatible with the topology of multiply twisted connected ribbons.}, archive = {J_PRL}, author = {Carlos E. Moguel-Lehmer and Christian D. Santangelo}, doi = {10.1103/q2dk-wf7t}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {128201}, shortjournal = {Phys. Rev. Lett.}, title = {Topological rigidity in twisted, elastic ribbons}, volume = {135}, year = {2025}, }
• (2025). Activation volume facilitating chemical reaction under mechanical stress. PRL, 135(12), 128001. (www)

  @article{ , abstract = {Activation volume is a crucial concept in mechanochemistry because it describes how the applied mechanical energy facilitates chemical reactions. The activation volume can be determined readily from the load dependence of a chemical reaction based on the stress-assisted thermal activation theory (also known as the Bell model), but it is still very challenging to fully understand what activation volume means physically and how to compute it. Here, by introducing a concept of inherent stress difference ( σ T ) between the initial and transition states, which is associated with the displacement of reacting atoms, a universal formula of activation volume ( Δ V * ) for the interfacial reactions is derived, that is, Δ V * = ( V eff σ T / E ) , where E and V eff refer to the Young’s modulus and the volume influenced by reaction, respectively. This formula implicates that Δ V * is related to the volume change from the initial to transition states. Then, the first-principles calculation was used to confirm the validity of the proposed definition in diverse types of chemical reactions. This Letter provides clear physical insight into how a chemical reaction that is unlikely to occur under thermal conditions is facilitated by mechanical stress, explaining the core principle of mechanochemistry.}, archive = {J_PRL}, author = {Yilong Jiang and Junyu Bin and Junhui Sun and Seong H. Kim and Linmao Qian and Lei Chen and Yang Wang}, doi = {10.1103/ndrl-df2d}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {128001}, shortjournal = {Phys. Rev. Lett.}, title = {Activation volume facilitating chemical reaction under mechanical stress}, volume = {135}, year = {2025}, }
• (2025). Manipulating phases in many-body interacting systems with subsystem resetting. PRL, 135(12), 127103. (www)

  @article{ , abstract = {Stabilizing thermodynamically unstable phases in many-body systems, such as suppressing pathological neuronal synchronization in Parkinson’s disease or maintaining magnetic order across broad temperature ranges, remains a persistent challenge. In traditional approaches, such phases are stabilized through intervening in the dynamics of all system constituents or introducing additional interactions. Here, we offer a hitherto-unexplored alternative, namely, subsystem resetting, whereby intervention in the dynamics of only a part of the system, and that too only occasionally in time, is implemented through resetting its state to a reset configuration. Just playing with a few parameters, e.g., the nature of the reset configuration and the size of the reset subsystem, one achieves a remarkable and robust control over the phase diagram of the bare dynamics. We demonstrate that these universal effects span a wide variety of scenarios, including equilibrium and nonequilibrium, mean-field and non-mean-field dynamics, with and without quenched disorder. Despite the challenges posed by memory effects, we obtain explicit analytical predictions, validated by simulations.}, archive = {J_PRL}, author = {Anish Acharya and Rupak Majumder and Shamik Gupta}, doi = {10.1103/np7q-hxld}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {127103}, shortjournal = {Phys. Rev. Lett.}, title = {Manipulating phases in many-body interacting systems with subsystem resetting}, volume = {135}, year = {2025}, }
• (2025). Velocity trapping in the lifted totally asymmetric simple exclusion process and the true self-avoiding random walk. PRL, 135(12), 127102. (www)

  @article{ , abstract = {We discuss nonreversible Markov-chain Monte Carlo algorithms that, for particle systems, rigorously sample the positional Boltzmann distribution and that have faster than physical dynamics. These algorithms all feature a nonthermal velocity distribution. They are exemplified by the lifted totally asymmetric simple exclusion process (lifted TASEP), a one-dimensional lattice reduction of event-chain Monte Carlo. We analyze its dynamics in terms of a velocity trapping that arises from correlations between the local density and the particle velocities. This allows us to formulate a conjecture for its out-of-equilibrium mixing timescale, and to rationalize its equilibrium superdiffusive timescale. Both scales are faster than for the (unlifted) TASEP. They are further justified by our analysis of the lifted TASEP in terms of many-particle realizations of true self-avoiding random walks. We discuss velocity trapping beyond the case of one-dimensional lattice models and in more than one physical dimensions. Possible applications beyond physics are pointed out.}, archive = {J_PRL}, author = {Brune Massoulié and Clément Erignoux and Cristina Toninelli and Werner Krauth}, doi = {10.1103/mqdr-x95j}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {127102}, shortjournal = {Phys. Rev. Lett.}, title = {Velocity trapping in the lifted totally asymmetric simple exclusion process and the true self-avoiding random walk}, volume = {135}, year = {2025}, }
• (2025). Universal scale-free decay of tracer-bath correlations in d-dimensional interacting particle systems. PRL, 135(12), 127101. (www)

  @article{ , abstract = {Quantifying the correlations between the position of a tagged tracer and the density of surrounding bath particles is crucial for understanding tracer diffusion in interacting particle systems, and for characterizing the response properties of the bath. We address this problem analytically for both hard-core and soft-core interactions, using minimal yet paradigmatic models in spatial dimensions. In both cases, we derive analytical expressions for the spatial correlation profiles in the reference frame of the tracer. We reveal unexpected universal features in their large-distance behavior, characterized by power-law tails with exponents that depend solely on the spatial dimensionality of the system. Beyond these simple models, we demonstrate the robustness of our results across different regimes using particle-based numerical simulations.}, archive = {J_PRL}, author = {Davide Venturelli and Pierre Illien and Aurélien Grabsch and Olivier Bénichou}, doi = {10.1103/55qy-sflc}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {127101}, shortjournal = {Phys. Rev. Lett.}, title = {Universal scale-free decay of tracer-bath correlations in d-dimensional interacting particle systems}, volume = {135}, year = {2025}, }
• (2025). Femtosecond-laser-delamination cavities for resonant acousto-magneto-plasmonics. PRL, 135(12), 126904. (www)

  @article{ , abstract = {Femtosecond lasers are routinely used for inducing local modification, including nanostructuring, and ultrafast laser spectroscopy in solids. However, these studies are often being performed separately making the unveiling of exciting physical properties of laser-fabricated materials out of reach. Here, we present an all-optical platform combining the fabrication of nano to micrometer size single-shot “femtosecond-laser-delamination” membranes or cavities of ferromagnetic thin films and multilayers together with their quasi in situ characterization using the Abbe-limited interferometric, ultrafast scanning photo-acoustic and magneto-plasmonic microscopies. Ferromagnetic nickel and iron cavities display high-Q acoustic resonances providing access to long-lived ultrahigh frequency coherent phonon modes in the above 100 GHz frequency range. Cavities in cobalt-gold bilayers allow for magnetically controlled surface plasmon resonance experiments in the Otto configuration, which is otherwise very difficult to implement experimentally. Quantitative experimental characterization of functional magnetic cavities, supported by the numerical modeling of all experimental data, opens an avenue to design and fabricate tunable nanoscaled femtosecond-laser-delamination architectures in thin films and multilayers.}, archive = {J_PRL}, author = {Pavel Varlamov and Akira Barros and Aditya Swaminathan and Jan Marx and Andreas Ostendorf and Anna Semisalova and Denys Makarov and Alexey M. Lomonosov and Paolo Vavassori and Yannis Laplace and Michele Raynaud and Vasily V. Temnov}, doi = {10.1103/99sl-xxb2}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126904}, shortjournal = {Phys. Rev. Lett.}, title = {Femtosecond-laser-delamination cavities for resonant acousto-magneto-plasmonics}, volume = {135}, year = {2025}, }
• (2025). Direct evidence of interfacial coherent electron-phonon coupling in single-unit-cell FeSe film on nb-doped SrTiO3. PRL, 135(12), 126903. (www)

  @article{ , abstract = {Interface-enhanced superconductivity in single-unit-cell FeSe on has been extensively pursued recently. The interfacial electron-phonon coupling (EPC) is widely proposed to enhance pairing, yet to be directly verified. Herein, using ultrafast pump-probe spectroscopy, we discover a coherent 4.2 THz optical phonon mode that emerges only upon photoexcitation in FeTe/FeSe/ or FeTe/ heterostructures, but is absent in bare Nb-doped under identical subgap pumping. Atomic-scale electron energy loss spectroscopy in scanning transmission electron microscopy identifies this mode as out-of-plane oxygen vibrations localized at double terminated interface. Crucially, the phonon amplitude in FeTe/FeSe/ is more than twice as large as that in FeTe/ , which can be attributed to higher electron doping that strengthens dipole moments penetrating the FeSe layer, thereby resulting in an enhanced interfacial EPC. Temperature-dependent dynamics further highlight the unique electronic nature of monolayer FeSe in sustaining this robust coupling. These findings provide direct evidence for dipole-mediated interfacial EPC as a critical mechanism of interfacial superconductivity in .}, archive = {J_PRL}, author = {Mengdi Zhang and Ruochen Shi and Rui Wu and Xiaotong Jiao and Mingxia Shi and Jiaxin Liu and Yubin Wang and Wenfeng Dong and Cui Ding and Tingxiao Qin and Haiyun Liu and Lili Wang and Zhenyu Zhang and Peng Gao and Qi-Kun Xue and Qihua Xiong}, doi = {10.1103/qxfc-khzf}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126903}, shortjournal = {Phys. Rev. Lett.}, title = {Direct evidence of interfacial coherent electron-phonon coupling in single-unit-cell FeSe film on nb-doped SrTiO3}, volume = {135}, year = {2025}, }
• (2025). Nonreciprocal thermal fizeau drag radiation around asymmetric exceptional points. PRL, 135(12), 126902. (www)

  @article{ , abstract = {Magnet-free, far-field infrared nonreciprocal thermal radiation has been reported using Weyl semimetals or spatiotemporal modulation nanostructures, but these methods face challenges like requiring extremely low temperatures or high modulation frequencies and have limited spectral or angular ranges. Here, we demonstrate far-field nonreciprocal thermal Fizeau drag radiation around asymmetric exceptional points (EPs) by drifting electrons in graphene sheets on dielectric periodic nanostructures. First, the generation and evolution mechanisms of symmetric scattering EP pairs have been unveiled in parameter spaces (i.e., w − θ space, w and θ are filling ratio of gratings and incident angle respectively). The EP pairs are connected by bulk Fermi arc along the θ axis whose length can be tuned over the whole angular range by modifying dielectric optical index. Drifting electrons contribute to asymmetrically redistributing EPs with specific angular and spectral positions at low drifting velocities due to Fizeau drag effects. These nonreciprocal behaviors of EPs in angle space have been used to shape magnet-free infrared nonreciprocal emissivity and absorptivity with different numbers of resonant peaks, resulting in more than an order of magnitude increase in wavelength-integrated thermal nonreciprocity. The physics that underpins the synergy between nonreciprocity and EPs offers new insights into areas such as non-Hermitian physics, nonreciprocal optics, and nonreciprocal thermal photonics.}, archive = {J_PRL}, author = {Mengqi Liu and Shuihua Yang and Weijin Chen and Jiahao Zhou and Changying Zhao and Cheng-Wei Qiu}, doi = {10.1103/hfyw-8z5k}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126902}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal thermal fizeau drag radiation around asymmetric exceptional points}, volume = {135}, year = {2025}, }
• (2025). Light-matter correlation energy functional of the cavity-coupled two-dimensional electron gas via quantum monte carlo simulations. PRL, 135(12), 126901. (www)

  @article{ , abstract = {We perform extensive simulations of the two-dimensional cavity-coupled electron gas in a modulating potential as a minimal model for cavity quantum materials. These simulations are enabled by a newly developed quantum-electrodynamical (QED) auxiliary-field quantum Monte Carlo method. We present a procedure to greatly reduce finite-size effects in such calculations. Based on our results, we show that a modified version of weak-coupling perturbation theory is remarkably accurate for a large parameter region. We further provide a simple parametrization of the light-matter correlation energy as a functional of the cavity parameters and the electronic density. These results provide a crucial step toward a numerical foundation for the development of the QED density functional theory, which was previously reliant on analytical approximations, to allow quantitative modeling of a wide range of systems with light-matter coupling.}, archive = {J_PRL}, author = {Lukas Weber and Miguel A. Morales and Johannes Flick and Shiwei Zhang and Angel Rubio}, doi = {10.1103/lq1y-q74h}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126901}, shortjournal = {Phys. Rev. Lett.}, title = {Light-matter correlation energy functional of the cavity-coupled two-dimensional electron gas via quantum monte carlo simulations}, volume = {135}, year = {2025}, }
• (2025). Nonvolatile electric control of antiferromagnetic states on nanosecond timescales. PRL, 135(12), 126704. (www)

  @article{ , abstract = {Electrical manipulation of antiferromagnetic (AFM) states, a cornerstone of AFM spintronics, is a great challenge, requiring novel material platforms. Here we report the full control over AFM states by voltage pulses in the insulating Co 3 O 4 spinel well below its Néel temperature. We show that the strong linear magnetoelectric effect is fully governed by the orientation of the Néel vector. As a unique feature of Co 3 O 4 , the magnetoelectric energy can easily overcome the weak magnetocrystalline anisotropy; thus, the Néel vector can be manipulated on demand, either rotated smoothly or reversed suddenly, by combined electric and magnetic fields. We achieve the nonvolatile switching within a few tens of nanoseconds between time-reversed AFM states in macroscopic volumes by voltage pulses. These observations render quasicubic antiferromagnets, like Co 3 O 4 , an ideal platform for the ultrafast (picosecond to nanosecond) manipulation of microscopic AFM domains and may pave the way for the realization of AFM spintronic devices.}, archive = {J_PRL}, author = {S. Ghara and M. Winkler and S. W. Schmid and L. Prodan and K. Geirhos and V. Tsurkan and Wenbo Ge and Weida Wu and A. Halbritter and S. Krohns and I. Kézsmárki}, doi = {10.1103/yzrk-h3rz}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126704}, shortjournal = {Phys. Rev. Lett.}, title = {Nonvolatile electric control of antiferromagnetic states on nanosecond timescales}, volume = {135}, year = {2025}, }
• (2025). Vertical soliton-assisted current switching in extremely thick FeGd ferrimagnets. PRL, 135(12), 126703. (www)

  @article{ , abstract = {Current-induced spin-orbit torques (SOTs) can electrically switch magnetic films. The thickness of these films is usually limited to a few tenths of nanometers. Toward stable spintronic nanodevices, it is important to explore the upper thickness limit and to identify the associated SOT switching mechanism, if it is different from standard models. Here, we experimentally show that the SOT switching could occur in trilayers with a thickness of ferrimagnetic films up to 200 nm, all at room temperature. The contributions from the Oersted field, bulk SOTs, and thermal activation induced by Joule heating are also discussed. Through performing atomistic spin simulations, we identify the critical role of nucleation and propagation of vertical magnetic solitons along the thickness direction, which could explain such unprecedented SOT switching behaviors in extremely thick ferrimagnets. The revelation of the vertical soliton-assisted SOT switching of the extremely thick ferrimagnets can be used for miniaturizing spintronic devices.}, archive = {J_PRL}, author = {Teng Xu and Zhengde Xu and Yiqing Dong and Yang Cheng and Ledong Wang and Hongmei Feng and Hao Bai and Kun Xu and Xinyu Shu and Pu Yu and Heng-An Zhou and Enlong Liu and Shikun He and Chuanying Xi and Guoqiang Yu and Xuepeng Qiu and Se Kwon Kim and Jing Zhu and Zhifeng Zhu and Wanjun Jiang}, doi = {10.1103/z89w-1vp9}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126703}, shortjournal = {Phys. Rev. Lett.}, title = {Vertical soliton-assisted current switching in extremely thick FeGd ferrimagnets}, volume = {135}, year = {2025}, }
• (2025). Strong coupling of chiral magnons in altermagnets. PRL, 135(12), 126702. (www)

  @article{ , abstract = {Altermagnets have recently been identified as a new class of magnets that break time-reversal symmetry without exhibiting net magnetization. The role of the dipole-dipole interaction (DDI) on their dynamical properties, however, is yet to be addressed. In this work, we show that the DDI can induce the strong coupling between exchange magnons with opposite chiralities in altermagnets, manifesting as a significant level repulsion in the magnon spectrum. Crucially, the predicted magnon-magnon coupling is highly anisotropic, and observable in practical experiments. These exotic features are absent in conventional antiferromagnets. Our findings open a new pathway for quantum magnonic information processing based on altermagnetism.}, archive = {J_PRL}, author = {Zhejunyu Jin and Tianci Gong and Jie Liu and Huanhuan Yang and Zhaozhuo Zeng and Yunshan Cao and Peng Yan}, doi = {10.1103/gn6c-1q19}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126702}, shortjournal = {Phys. Rev. Lett.}, title = {Strong coupling of chiral magnons in altermagnets}, volume = {135}, year = {2025}, }
• (2025). Spin demons in d-wave altermagnets. PRL, 135(12), 126701. (www)

  @article{ , abstract = {Demons are a type of plasmons, which consist of out-of-phase oscillations of electrons in different bands. Here, we show that -wave altermagnets, a recently discovered class of collinear magnetism, naturally realize a spin demon, which consists of out-of-phase movement of the two spin species. The spin demon lives outside of the particle-hole continuum of one of the spin species, and is therefore significantly underdamped, reaching quality factors of . We show that the spin demon carries a magnetic moment, which inherits the -wave symmetry. Finally, we consider both three- and two-dimensional -wave altermagnets, and show that spin demons exist in both.}, archive = {J_PRL}, author = {Pieter M. Gunnink and Jairo Sinova and Alexander Mook}, doi = {10.1103/99zp-s88m}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126701}, shortjournal = {Phys. Rev. Lett.}, title = {Spin demons in d-wave altermagnets}, volume = {135}, year = {2025}, }
• (2025). Hopf bifurcation of nonlinear non-hermitian skin effect. PRL, 135(12), 126610. (www)

  @article{ , abstract = {The non-Hermitian skin effect, nonreciprocity-induced anomalous localization of an extensive number of eigenstates, represents a hallmark of non-Hermitian topological systems with no analogs in Hermitian systems. Despite its significance across various open classical and quantum systems, the influence of nonlinearity has remained largely unclear. Here, we reveal the Hopf bifurcation of the nonlinear skin effect as a critical phenomenon unique to nonlinear non-Hermitian systems. We demonstrate that nonlinearity destabilizes skin states and instead gives rise to the emergence of delocalized states associated with limit cycles in phase space. We also uncover the algebraically localized critical skin effect precisely at the Hopf bifurcation point. We illustrate this behavior in a nonlinear extension of the Hatano-Nelson model in both continuum and lattice. Our Letter shows a significant role of nonlinearity in the skin effect and uncovers rich phenomena arising from the interplay between non-Hermiticity and nonlinearity.}, archive = {J_PRL}, author = {Kohei Kawabata and Daichi Nakamura}, doi = {10.1103/vxgf-59xt}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126610}, shortjournal = {Phys. Rev. Lett.}, title = {Hopf bifurcation of nonlinear non-hermitian skin effect}, volume = {135}, year = {2025}, }
• (2025). Emerging (2+1)D electrodynamics and topological instanton in pseudo-hermitian two-level systems. PRL, 135(12), 126609. (www)

  @article{ , abstract = {We reveal a hidden electrodynamical structure emerging from a general 2 × 2 pseudo-Hermitian system that exhibits real spectra. Even when the Hamiltonian does not explicitly depend on time, the Berry curvature can be mapped onto a 2 + 1 -dimensional electromagnetic field arising from an artificial spacetime instanton, in sharp contrast to the Hermitian systems where the Berry curvature is equivalent to the static magnetic field of a magnetic monopole in three spatial dimensions. The instanton appearing as a spacetime singularity carries a topological charge that quantizes the jump of magnetic flux of the Berry curvature at the time origin. Our findings are demonstrated in a simple example related to antiferromagnetic magnons.}, archive = {J_PRL}, author = {Kuangyin Deng and Ran Cheng}, doi = {10.1103/kcls-cn82}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126609}, shortjournal = {Phys. Rev. Lett.}, title = {Emerging (2+1)D electrodynamics and topological instanton in pseudo-hermitian two-level systems}, volume = {135}, year = {2025}, }
• (2025). Emergence of chiral phonons in two-dimensional kagome lattices harboring electronic chirality. PRL, 135(12), 126608. (www)

  @article{ , abstract = {Chiral phonons have recently been established to emerge in systems containing intrinsically chiral atomic structures or magnetic systems. Here we show that such intriguing chiral phonons can also be induced in nonmagnetic Kagome lattices that lack atomic structural chirality but harbor electronic chirality rooted in the presence of loop current order. This central finding is demonstrated using two types of loop current order, the restricted chiral flux phase characterized by a pure imaginary charge bond order and the more generalized chiral flux phase characterized by a complex charge bond order, as typified in layered ( , Rb, K). At a mechanistic level, the time-reversal symmetry breaking caused by the electronic chirality is shown to pronouncedly influence their vibrational properties through electron-phonon coupling. The electronic chirality in either chiral flux phase is accompanied by a nonzero molecular Berry curvature, which in turn manifests as a nonlocal effective magnetic field of vectorial nature acting on the phonons. Consequently, the double degeneracy at each Brillouin zone corner is lifted, empowering chirality to the phonon modes. This Letter provides an indispensable component toward a more complete understanding of various chiral collective electronic phenomena in such structurally achiral systems.}, archive = {J_PRL}, author = {Yanru Chen and Wei Qin and Shunhong Zhang and Ping Cui and Qian Niu and Zhenyu Zhang}, doi = {10.1103/bfll-sdrb}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126608}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of chiral phonons in two-dimensional kagome lattices harboring electronic chirality}, volume = {135}, year = {2025}, }
• (2025). Coexistence of topological surface states and superconductivity in dirac semimetal NiTe2. PRL, 135(12), 126607. (www)

  @article{ , abstract = {The coexistence of topological bands around the Fermi level ( E F ) and superconductivity provides a fundamental platform for exploring their interplay. However, few materials inherently display both properties. In this Letter, we demonstrate the coexistence of topological surface states at the E F and superconductivity in NiTe 2 single crystals, a material hitherto not recognized as superconducting. Quasiparticle interference measurements performed via scanning tunneling microscopy suggest the presence of topological surface states at the E F , which is further corroborated by density functional theory simulations. Experimental evidence for superconductivity is provided via electronic transport measurements and specific heat capacity analyses. Our results suggest that NiTe 2 represents a promising platform for investigating the rich interplay between topological states and superconductivity.}, archive = {J_PRL}, author = {Chen He and Jian-Zhou Zhao and Mei Du and Luo-Zhao Zhang and Jia-Ying Zhang and Kuo Yang and Noah F. Q. Yuan and Aleksandr Seliverstov and Ewald Janssens and Jun-Yi Ge and Zhe Li}, doi = {10.1103/vpl7-n6bp}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126607}, shortjournal = {Phys. Rev. Lett.}, title = {Coexistence of topological surface states and superconductivity in dirac semimetal NiTe2}, volume = {135}, year = {2025}, }
• (2025). Enhancing the hyperpolarizability of crystals with quantum geometry. PRL, 135(12), 126606. (www)

  @article{ , abstract = {We demonstrate that higher-order electric susceptibilities in crystals can be enhanced and understood through nontrivial topological invariants and quantum geometry, using one-dimensional -conjugated chains as representative model systems. First, we show that the crystalline-symmetry-protected topology of these chains imposes a lower bound on their quantum metric and hyperpolarizabilities. Second, we employ numerical simulations to reveal the tunability of nonlinear, quantum geometry-driven optical responses in various one-dimensional crystals in which band topology can be externally controlled. Third, we develop a semiclassical picture to deliver an intuitive understanding of these effects. Our findings offer a firm interpretation of otherwise elusive experimental observations of colossal hyperpolarizabilities and establish guidelines for designing topological materials of any dimensionality with enhanced nonlinear optical properties.}, archive = {J_PRL}, author = {Wojciech J. Jankowski and Robert-Jan Slager and Michele Pizzochero}, doi = {10.1103/z7lp-pqp6}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126606}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing the hyperpolarizability of crystals with quantum geometry}, volume = {135}, year = {2025}, }
• (2025). Modified interferometer to measure anyonic braiding statistics. PRL, 135(12), 126605. (www)

  @article{ , abstract = {Existing quantum Hall interferometers measure twice the braiding phase, e i 2 θ , of Abelian anyons, i.e., the phase accrued when one quasiparticle encircles another clockwise. We propose a modified Fabry-Pérot or Mach-Zehnder interferometer that can measure e i θ .}, archive = {J_PRL}, author = {Steven A. Kivelson and Chaitanya Murthy}, doi = {10.1103/x4w5-h3bb}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126605}, shortjournal = {Phys. Rev. Lett.}, title = {Modified interferometer to measure anyonic braiding statistics}, volume = {135}, year = {2025}, }
• (2025). Genuine topological anderson insulator from impurity induced chirality reversal. PRL, 135(12), 126604. (www)

  @article{ , abstract = {We investigate a model of Dirac fermions with mass impurities that open a global topological gap even in the dilute limit. Surprisingly, we find that the chirality of this mass term, i.e., the sign of the Chern number, can be reversed by tuning the magnitude of the single-impurity scattering. Consequently, the disorder induces a phase disconnected from the simple clean limit of the topological insulator, which is achieved via an impurity resonance inducing additional bands with Chern number 2. Thus, we call this impurity induced phase a genuine topological Anderson insulator. In seeming contradiction to the expectation that mass disorder is an irrelevant perturbation to the Dirac semimetal, the tricritical point separating these two Chern insulating phases and a thermal metal phase is located at zero impurity density and connected to the appearance of a zero energy bound state in the continuum that corresponds to a perfectly resonant mass impurity. Our conclusions based on the -matrix expansion are substantiated by large scale Chebyshev-polynomial Green’s function numerics. We discuss possible experimental platforms.}, archive = {J_PRL}, author = {Avedis Neehus and Frank Pollmann and Johannes Knolle}, doi = {10.1103/7p8y-2mp6}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126604}, shortjournal = {Phys. Rev. Lett.}, title = {Genuine topological anderson insulator from impurity induced chirality reversal}, volume = {135}, year = {2025}, }
• (2025). Topological valley transport in bilayer graphene induced by interlayer sliding. PRL, 135(12), 126603. (www)

  @article{ , abstract = {Interlayer sliding, together with twist angle, is a crucial parameter that defines the atomic registry and thus determines the properties of two-dimensional (2D) material homobilayers. Here, we theoretically demonstrate that controlled interlayer sliding in bilayer graphene induces Berry curvature reversals, leading to topological states confined within a one-dimensional moiré channel. We experimentally realize interlayer sliding by bending the bilayer graphene geometry across a nanoridge. Systematic electronic transport measurements reveal topological valley transport when the Fermi energy resides within the band gap, consistent with theoretical predictions of eight topological channels. Our findings establish interlayer sliding as a powerful tool for tuning the electronic properties of bilayer graphene and underscore its potential for broad application across 2D material systems.}, archive = {J_PRL}, author = {Jie Pan and Huanhuan Wang and Lin Zou and Xiaoyu Wang and Lihao Zhang and Xueyan Dong and Haibo Xie and Yi Ding and Yuze Zhang and Takashi Taniguchi and Kenji Watanabe and Shuxi Wang and Zhe Wang}, doi = {10.1103/26q7-dsm1}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126603}, shortjournal = {Phys. Rev. Lett.}, title = {Topological valley transport in bilayer graphene induced by interlayer sliding}, volume = {135}, year = {2025}, }
• (2025). Dimensional hierarchy of topological bound states in the continuum. PRL, 135(12), 126602. (www)

  @article{ , abstract = {Bound states in the continuum (BICs), with the ability of trapping and manipulating waves within the radiation continuum, have gained significant attention for their potential applications in optics and acoustics. However, challenges arise in reducing wave leakage and noise from fabrication imperfections. The emergence of robust wave manipulations based on topological BICs (TBICs) offers promising solutions. Traditionally, TBICs of different dimensions are observed separately in distinct systems. Here, we report the experimental discovery of the coexistence of two-dimensional surface TBICs and one-dimensional hinge TBICs in a single three-dimensional phononic crystal system. Such an unprecedented dimensional hierarchy of TBICs is triggered by the mechanism of separability and protected by the valley Chern numbers. Notably, these TBICs inherit dispersive propagation characteristics from valley topology and can propagate robustly against defects without leakage. Our findings offer an efficient approach to multidimensional TBICs and can be applied in designing highly efficient acoustic devices for wave trapping and manipulation in multidimensional environments.}, archive = {J_PRL}, author = {Shunda Yin and Zhenyu Wang and Liping Ye and Hailong He and Manzhu Ke and Weiyin Deng and Jiuyang Lu and Zhengyou Liu}, doi = {10.1103/lq9m-nngh}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126602}, shortjournal = {Phys. Rev. Lett.}, title = {Dimensional hierarchy of topological bound states in the continuum}, volume = {135}, year = {2025}, }
• (2025). Three-dimensional topological valley photonics. PRL, 135(12), 126601. (www)

  @article{ , abstract = {Topological valley photonics, which exploits valley degrees of freedom to manipulate electromagnetic waves, offers a practical and effective pathway for various classical and quantum photonic applications across the entire spectrum. Current valley photonics, however, has been limited to two dimensions, which typically suffer from out-of-plane losses and can only manipulate the flow of light in planar geometries. Here, we have theoretically and experimentally developed a framework of three-dimensional (3D) topological valley photonics with a complete photonic band gap and vectorial valley contrasting physics. Unlike the two-dimensional counterparts with a pair of valleys characterized by scalar valley Chern numbers, the 3D valley systems exhibit triple pairs of valleys characterized by valley Chern vectors, enabling the creation of vectorial bulk valley vortices and canalized chiral valley surface states. Notably, the valley Chern vectors and the circulating propagation direction of the valley surface states are intrinsically governed by the right-hand-thumb rule. Our findings reveal the vectorial nature of the 3D valley states and highlight their potential applications in 3D waveguiding, directional radiation, and imaging.}, archive = {J_PRL}, author = {Wenhao Li and Qiaolu Chen and Ning Han and Xinrui Li and Fujia Chen and Junyao Wu and Yuang Pan and Yudong Ren and Hongsheng Chen and Haoran Xue and Yihao Yang}, doi = {10.1103/kmsq-llfk}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126601}, shortjournal = {Phys. Rev. Lett.}, title = {Three-dimensional topological valley photonics}, volume = {135}, year = {2025}, }
• (2025). Phase transitions and remnants of fractionalization at finite temperature in the triangular lattice quantum loop model. PRL, 135(12), 126503. (www)

  @article{ , abstract = {The quantum loop and dimer models are archetypal correlated systems with local constraints. With natural foundations in statistical mechanics, they are of direct relevance to various important physical concepts and systems, such as topological order, lattice gauge theories, geometric frustrations, or more recently Rydberg array quantum simulators. However, how the thermal fluctuations interact with constraints has not been explored in the important class of nonbipartite geometries. Here we study, via unbiased quantum Monte Carlo simulations and field theoretical analysis, the finite-temperature phase diagram of the quantum loop model on the triangular lattice. We discover that the recently identified, “hidden” vison plaquette (VP) quantum crystal [X. Ran et al. , Hidden orders and phase transitions for the fully packed quantum loop model on the triangular lattice, Commun. Phys. 7 , 207 (2024) ] experiences a finite-temperature continuous transition, which smoothly connects to the Cubic* quantum critical point separating the VP and quantum spin liquid phases. This finite-temperature phase transition acquires a unique property of “remnants of fractionalization” at finite temperature, in that, both the cubic order parameter—the plaquette loop resonance—and its constituent—the vison field—exhibit independent criticality signatures. This phase transition is connected to a three-state Potts transition between the lattice nematic phase and the high-temperature disordered phase. We discuss the relevance of our results for current experiments on quantum simulation platforms.}, archive = {J_PRL}, author = {Xiaoxue Ran and Sylvain Capponi and Junchen Rong and Fabien Alet and Zi Yang Meng}, doi = {10.1103/tp8x-dscx}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126503}, shortjournal = {Phys. Rev. Lett.}, title = {Phase transitions and remnants of fractionalization at finite temperature in the triangular lattice quantum loop model}, volume = {135}, year = {2025}, }
• (2025). Spectral properties of fractionalized shiba states. PRL, 135(12), 126502. (www)

  @article{ , abstract = {A magnetic impurity in a BCS superconductor induces the formation of a Shiba state and drives a local quantum phase transition. We generalize this concept to a one-dimensional superconductor with fractionalized excitations, where the dominant instability is superconducting. In this framework, conduction electrons fractionalize into gapless charge and gapped spin excitations. We show that magnetic impurity interacts exclusively with the spin degrees of freedom and induces a quantum phase transition. Furthermore, charge excitations influence dynamical observables, giving rise to the phenomenon we term the “fractionalized Shiba state.” At zero temperature, the tunneling spectrum exhibits universal power-law scaling with an exponent of at half filling, stemming from the gapless charge modes that form a standard Luttinger liquid. Extending this analysis to finite temperatures reveals that the spectral features retain universal behavior at the critical point.}, archive = {J_PRL}, author = {Cătălin Paşcu Moca and Csanád Hajdú and Balázs Dóra and Gergely Zaránd}, doi = {10.1103/g4sp-t82d}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126502}, shortjournal = {Phys. Rev. Lett.}, title = {Spectral properties of fractionalized shiba states}, volume = {135}, year = {2025}, }
• (2025). Disorder-induced suppression of superconductivity in infinite-layer nickelates. PRL, 135(12), 126501. (www)

  @article{ , abstract = {The pairing symmetry of superconducting infinite-layer nickelates is a fundamental yet experimentally challenging question. We employ high-energy electron irradiation to induce disorder in superconducting thin films, examine the impact of pair-breaking defects on superconductivity, and elucidate the nature of the superconducting gap. Our measurements reveal a complete suppression of superconductivity with increasing disorder, suggesting an unconventional, sign-changing order parameter.}, archive = {J_PRL}, author = {Abhishek Ranna and Romain Grasset and Martin Gonzalez and Kyuho Lee and Bai Yang Wang and Edgar Abarca Morales and Florian Theuss and Zuzanna H. Filipiak and Michal Moravec and Marcin Konczykowski and Harold Y. Hwang and Andrew P. Mackenzie and Berit H. Goodge}, doi = {10.1103/7lqb-pjkm}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126501}, shortjournal = {Phys. Rev. Lett.}, title = {Disorder-induced suppression of superconductivity in infinite-layer nickelates}, volume = {135}, year = {2025}, }
• (2025). Quantum monte carlo pair orbital wave functions for periodic systems. PRL, 135(12), 126401. (www)

  @article{ , abstract = {We derive many-body single and multireference wave functions for quantum Monte Carlo of periodic systems with an antisymmetric portion that explicitly integrates over the Brillouin zone of one-particle Bloch states. The wave functions are BCS-like determinants for singlets and Pfaffians for polarized states built with appropriate pair orbitals. This ab initio formalism is broadly applicable, e.g., to description of quasiparticle band gaps and optical excitations and to systems with complicated Fermi surfaces. It generalizes to spin-dependent interactions using two-component spinor pairs.}, archive = {J_PRL}, author = {Lubos Mitas}, doi = {10.1103/9xqw-57cp}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum monte carlo pair orbital wave functions for periodic systems}, volume = {135}, year = {2025}, }
• (2025). Accurate ab initio method for charged defect scattering. PRL, 135(12), 126302. (www)

  @article{ , abstract = {Charged defect scattering of electrons plays a critical role in determining a wide range of material properties. However, there is a lack of an accurate method to calculate the scattering, as all the existing methods require assuming a specific distribution for unscreened (i.e., bare) excess charge carried by the defect, which limits their accuracy. Here we develop a first-principles method to determine the bare charge distribution, which thus enables accurate calculations of the scattering. Using this method, we accurately calculate the electron mobility of 2D under the scattering of charged sulfur vacancies and compare with that of charge-neutral oxygen substitutes of sulfur. Interestingly, we find that the charged defect-limited mobility exhibits a strong temperature dependence at low temperature and carrier concentration, in contrast to the neutral defect and the conventional belief that the defect-limited mobility is less sensitive to the temperature. This behavior arises from the free carrier screening of the long-range scattering potential of the charged defect. Our work offers new insights into the transport mechanism, and opens access to accurate calculation, understanding, and prediction of charged defect scattering and a broad range of associated properties.}, archive = {J_PRL}, author = {Rongjing Guo and Kwangrae Kim and Zhongcan Xiao and Yuanyue Liu}, doi = {10.1103/42pc-t2bx}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126302}, shortjournal = {Phys. Rev. Lett.}, title = {Accurate ab initio method for charged defect scattering}, volume = {135}, year = {2025}, }
• (2025). Twist-on-twist moiré elastic metasurfaces. PRL, 135(12), 126301. (www)

  @article{ , abstract = {The concepts of twistronics and magic angle have been widely applied beyond electrons, powering up new advancements in optics, acoustics, and heat transport. However, achieving a unidirectional or all-direction “magic angle” remains an established yet unresolved challenge in twisted bilayer metasurfaces across various disciplines. Our work proposes and validates a “twist-on-twist” paradigm to realizing unidirectional propagation and robust magic angle at arbitrary directions of the elastic out-of-plane wave. Our elastic metasurface not only exhibits a twisted configuration between the stacked bilayer but also significantly enhances out-of-plane symmetry breaking by further twisting meta-atoms in one constituent layer. Our twist-on-twist method unleashes versatile potentials of twisted thin composite materials to control the extreme propagation of topological elastic waves and even opens up new possibilities for photonic, phononic, and thermal moiré metamaterials.}, archive = {J_PRL}, author = {Menghan Li and Kuan He and Zhiwen Ren and Li-Qun Chen and Hao-Wen Dong and Chenglin Han and Tianzhi Yang and Cheng-Wei Qiu}, doi = {10.1103/qw7j-fj7b}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126301}, shortjournal = {Phys. Rev. Lett.}, title = {Twist-on-twist moiré elastic metasurfaces}, volume = {135}, year = {2025}, }
• (2025). Entropy spectroscopy of a bilayer graphene quantum dot. PRL, 135(12), 126202. (www)

  @article{ , abstract = {We measure the entropy change of charge transitions in an electrostatically defined quantum dot in bilayer graphene. Entropy provides insights into the equilibrium thermodynamic properties of both ground and excited states beyond transport measurements. For the one-carrier regime, the obtained entropy shows that the ground state has a twofold degeneracy lifted by an out-of-plane magnetic field. This observation is in agreement with previous direct transport measurements and confirms the applicability of this novel method. For the two-carrier regime, the extracted entropy indicates a nondegenerate ground state at zero magnetic field, contrary to previous studies suggesting a threefold degeneracy. We attribute the degeneracy lifting to the effect of Kane-Mele-type spin-orbit interaction on the two-carrier ground state, which has not been observed before. Our Letter demonstrates the validity and efficacy of entropy measurements as a unique, supplementary experimental tool to investigate the degeneracy of the ground state in quantum devices built in materials such as graphene. This technique, applied to exotic systems with fractional ground state entropies, will be a powerful tool in the study of quantum matter.}, archive = {J_PRL}, author = {C. Adam and H. Duprez and N. Lehmann and A. Yglesias and A. O. Denisov and S. Cances and M. J. Ruckriegel and M. Masseroni and C. Tong and W. Huang and D. Kealhofer and R. Garreis and K. Watanabe and T. Taniguchi and K. Ensslin and T. Ihn}, doi = {10.1103/vbbj-138r}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126202}, shortjournal = {Phys. Rev. Lett.}, title = {Entropy spectroscopy of a bilayer graphene quantum dot}, volume = {135}, year = {2025}, }
• (2025). Eliminating defect states in monolayer tungsten diselenide by coupling with a c-plane sapphire surface. PRL, 135(12), 126201. (www)

  @article{ , abstract = {Semiconducting transition metal dichalcogenides are promising platforms for exploring emergent two-dimensional (2D) exciton physics and constructing 2D optoelectronic devices. However, even in mechanically exfoliated and hexagonal boron nitride encapsulated samples that are expected to maintain the most intrinsic properties, shallow defect states are still unavoidable. Here, we reported a method for eliminating the defect states in monolayer WSe 2 by coupling it with a c-plane sapphire surface. We found that the defect-relevant photoluminescence peaks at cryogenic temperatures can be completely suppressed in WSe 2 on c-plane sapphire, resulting in intrinsic exciton radiation, prolonged lifetime, and increased diffusion length. Ab initio calculations revealed that the surface of c-plane sapphire is much more active than other planes, where oxygen atoms preferentially transfer to WSe 2 to repair selenium vacancy defects. Our Letter provides a new platform for defect engineering, which will promote the development of high-performance electronic and optoelectronic devices based on 2D materials.}, archive = {J_PRL}, author = {Chen Huang and Jinhuan Wang and Yilin Chen and Zuo Feng and Yuexing Xia and Guangjie Yao and Mengze Zhao and Guodong Xue and Si Zhou and Xiaozhi Xu and Xinfeng Liu and Enge Wang and Ji Chen and Kaihui Liu and Hao Hong}, doi = {10.1103/lswx-rxss}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126201}, shortjournal = {Phys. Rev. Lett.}, title = {Eliminating defect states in monolayer tungsten diselenide by coupling with a c-plane sapphire surface}, volume = {135}, year = {2025}, }
• (2025). Negative and positive anisotropic thermal expansion in 2D fullerene networks. PRL, 135(12), 126103. (www)

  @article{ , abstract = {We find a design principle for tailoring thermal expansion properties in nearly spherical molecular networks. Using 2D fullerene networks as a representative system, we realize positive thermal expansion along intermolecular [ 2 + 2 ] cycloaddition bonds and negative thermal expansion along intermolecular C-C single bonds by varying the structural frameworks of molecules. The microscopic mechanism originates from a combination of the framework’s geometric flexibility and its transverse vibrational characteristics. Based on this insight, we find molecular networks beyond C 60 with tunable thermal expansion. These findings shed light on the fundamental mechanisms governing thermal expansion in molecular networks towards rational materials design.}, archive = {J_PRL}, author = {Armaan Shaikh and Jiaqi Wu and Bo Peng}, doi = {10.1103/tck2-78dx}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126103}, shortjournal = {Phys. Rev. Lett.}, title = {Negative and positive anisotropic thermal expansion in 2D fullerene networks}, volume = {135}, year = {2025}, }
• (2025). Internal stresses as origin of the anomalous low-temperature specific heat in glasses. PRL, 135(12), 126102. (www)

  @article{ , abstract = {We apply a recently developed theory of the nonphononic vibrational density of states (DOS) in glasses to investigate the impact of local frozen-in stresses on the low-temperature specific heat. Using a completely harmonic description we show that the hybridization of the local nonphononic vibrational excitations with the waves leads to a low-frequency DOS, in excess to the Debye one, which varies linearly with frequency up to a certain crossover frequency, and then becomes constant. The actual value of the crossover depends of the ratio between the local stresses and the shear modulus. This excess DOS leads to a low-temperature specific heat with an apparent temperature exponent, which is between one and two, as observed experimentally. We discuss how these findings may be utilized for the characterization of glassy materials. We further compare our findings, which only rely on harmonic interactions, with the predictions of other theories, which invoke anharmonic interactions and tunneling for explaining the low-temperature behavior of the specific heat.}, archive = {J_PRL}, author = {Walter Schirmacher and Giancarlo Ruocco}, doi = {10.1103/p95w-9wjc}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126102}, shortjournal = {Phys. Rev. Lett.}, title = {Internal stresses as origin of the anomalous low-temperature specific heat in glasses}, volume = {135}, year = {2025}, }
• (2025). Tensor learning and compression of N-phonon interactions. PRL, 135(12), 126101. (www)

  @article{ , abstract = {Phonon interactions from lattice anharmonicity govern thermal properties and heat transport in materials. These interactions are described by th order interatomic force constants ( IFCs), which can be viewed as high-dimensional tensors correlating the motion of atoms, or equivalently encoding -phonon scattering processes in momentum space. Here, we introduce a tensor decomposition to efficiently compress IFCs for arbitrary order . Using tensor learning, we find optimal low-rank approximations of IFCs by solving the resulting optimization problem. Our approach reveals the inherent low dimensionality of phonon-phonon interactions and allows compression of the three- and four-IFC tensors by factors of up to while retaining high accuracy in calculations of phonon scattering rates and thermal conductivity. Calculations of thermal conductivity using the compressed IFCs achieve a speedup by nearly 3 orders of magnitude with accuracy relative to the reference uncompressed solution. These calculations include both three- and four-phonon scattering and are shown for a diverse range of materials (Si, HgTe, MgO, TiNiSn, and ). In addition to accelerating state-of-the-art thermal transport calculations, the method shown here paves the way for modeling strongly anharmonic materials and higher-order phonon interactions.}, archive = {J_PRL}, author = {Yao Luo and Dhruv Mangtani and Shiyu Peng and Jia Yao and Sergei Kliavinek and Marco Bernardi}, doi = {10.1103/nmgj-yq1g}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126101}, shortjournal = {Phys. Rev. Lett.}, title = {Tensor learning and compression of N-phonon interactions}, volume = {135}, year = {2025}, }
• (2025). Evidence for multiband gapless superconductivity in the topological superconductor candidate 4Hb−TaS2. PRL, 135(12), 126002. (www)

  @article{ , abstract = {We present the ultra-low-temperature thermal conductivity measurements on single crystals of the transition-metal dichalcogenide material , which has recently been proposed as a topological superconductor candidate. In zero field, a small residual linear term is observed, indicating the existence of a residual density of states in the superconducting state. The slow field dependence of at low fields rules out the presence of nodes in the superconducting gap, and the S-shaped field dependence across the full field range suggests multiple superconducting gaps in . Our results provide evidence for multiband gapless superconductivity in , and the residual density of states come from certain gapless Fermi surfaces.}, archive = {J_PRL}, author = {Hanru Wang and Yihan Jiao and Fanyu Meng and Xu Zhang and Dongzhe Dai and Chengpeng Tu and Chengcheng Zhao and Lu Xin and Sicheng Huang and Hechang Lei and Shiyan Li}, doi = {10.1103/d13p-mtbz}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126002}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for multiband gapless superconductivity in the topological superconductor candidate 4Hb−TaS2}, volume = {135}, year = {2025}, }
• (2025). Probing vortex dynamics in 2D superconductors with scanning quantum microscope. PRL, 135(12), 126001. (www)

  @article{ , abstract = {Magnetic dynamics at the nanoscale provide crucial insight into the behavior of superconductors. Using single-spin scanning quantum microscopy, we probe vortex dynamics in the two-dimensional superconductor . Our measurements reveal a disordered vortex glass phase that melts near the critical temperature and displays cooling-rate-dependent configurations. Surprisingly, magnetic noise persists well below , with a strength that increases at lower temperatures—contrary to expectations. This behavior, detected via spin decoherence, points to an intrinsic origin driven by competition between supercurrent density and thermal fluctuations. Our results establish single-spin microscopy as a powerful platform for investigating fluctuations in 2D superconductors.}, archive = {J_PRL}, author = {Sreehari Jayaram and Malik Lenger and Dong Zhao and Lucas Pupim and Takashi Taniguchi and Kenji Watanabe and Ruoming Peng and Marc Scheffler and Rainer Stöhr and Mathias S. Scheurer and Jurgen Smet and Jörg Wrachtrup}, doi = {10.1103/1fzm-pb1d}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {126001}, shortjournal = {Phys. Rev. Lett.}, title = {Probing vortex dynamics in 2D superconductors with scanning quantum microscope}, volume = {135}, year = {2025}, }
• (2025). TeV solar gamma rays as a probe for the solar internetwork magnetic fields. PRL, 135(12), 125201. (www)

  @article{ , abstract = {Recently, solar gamma rays produced by cosmic rays interacting with the solar atmosphere have been detected in the GeV to TeV energy range, revealing that cosmic rays are significantly affected by magnetic fields in the solar atmosphere. However, much of the observations remain unexplained by existing physical models. Using a semianalytic model, we demonstrate that magnetic fields at and below the photosphere with a large horizontal component could account for the approximately 1 TeV solar gamma rays observed by HAWC. This suggests that high-energy solar gamma rays could serve as a novel probe for magnetic fields beneath the photosphere, which in the future could help improve the understanding of solar magnetism, the key driver of space weather.}, archive = {J_PRL}, author = {Kenny C. Y. Ng and Andrew Hillier and Shin’ichiro Ando}, doi = {10.1103/l6qw-8c1h}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {125201}, shortjournal = {Phys. Rev. Lett.}, title = {TeV solar gamma rays as a probe for the solar internetwork magnetic fields}, volume = {135}, year = {2025}, }
• (2025). Influence of collisional effects on ion-acoustic wave properties in non-maxwellian laser-driven plasmas. PRL, 135(12), 125101. (www)

  @article{ , abstract = {Collisional effects significantly influence inertial confinement fusion hohlraum plasmas, where non-Maxwellian inverse bremsstrahlung heating and collision-induced anisotropy alter the kinetic plasma response. We derived the linear ion-acoustic wave (IAW) dispersion relation, revealing the necessity of accounting for binary collisions in both the isotropic and anisotropic parts of the electron distribution function, as well as in the anisotropic part of the light ion distribution function. This affects the IAW damping rate, either increasing or decreasing it depending on laser parameters and plasma composition. Our analytical model, validated against particle-in-cell simulations for single- and two-ion species plasmas, offers crucial insights for high-energy laser-driven implosion experiments. It can be applied to Thomson scattering analysis and integrated into wave mixing processes involving IAWs, such as cross-beam energy transfer and Brillouin scattering.}, archive = {J_PRL}, author = {R. Capdessus and C. Ruyer and A. Debayle and P. Loiseau and P. E. Masson-Laborde}, doi = {10.1103/yycm-f8l7}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {125101}, shortjournal = {Phys. Rev. Lett.}, title = {Influence of collisional effects on ion-acoustic wave properties in non-maxwellian laser-driven plasmas}, volume = {135}, year = {2025}, }
• (2025). Strong and weak dynamo regimes in taylor-couette flows. PRL, 135(12), 124001. (www)

  @article{ , abstract = {We reveal a nonlinear magnetic dynamo in a Taylor-Couette flow at small magnetic Prandtl numbers , which has been previously believed to exist only at higher in this flow. The amplitude of initial perturbations, and domain aspect ratio play a key role in the onset and evolution of the dynamo. It exists in two main states: a weak state dominated by large-scale modes and a strong, turbulent state with higher amplitude dominated by small-scale modes. These findings can be important for dynamo processes in various astrophysical objects with small .}, archive = {J_PRL}, author = {Ashish Mishra and George Mamatsashvili and Frank Stefani}, doi = {10.1103/fvv6-7pr2}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {124001}, shortjournal = {Phys. Rev. Lett.}, title = {Strong and weak dynamo regimes in taylor-couette flows}, volume = {135}, year = {2025}, }
• (2025). Genuine quantum effects in dicke-type models at large atom numbers. PRL, 135(12), 123602. (www)

  @article{ , abstract = {We investigate the occurrence of genuine quantum effects and beyond mean-field physics in the balanced and unbalanced open Dicke models with a large yet finite number of atoms . Such driven and dissipative quantum many-body systems have recently been realized in experiments involving ultracold gases inside optical cavities and are known to obey mean-field predictions in the thermodynamic limit . Here we show quantum effects that survive for large but finite , by employing a novel open-system dynamics method that allows us to obtain numerically exact quantum dynamical results for atom numbers up to a mesoscopic . While we find that beyond-mean-field effects vanish quickly with increasing in the balanced Dicke model, we are able to identify parameter regimes in the unbalanced Dicke model that allow genuine quantum effects to persist even for mesoscopic . They manifest themselves in a strong squeezing of the steady state and a modification of the steady-state phase diagram that cannot be seen in a mean-field description. This is due to the fact that the steady-state limit and thermodynamic limit do not commute.}, archive = {J_PRL}, author = {Kai Müller and Walter T. Strunz}, doi = {10.1103/42rz-xhxz}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {123602}, shortjournal = {Phys. Rev. Lett.}, title = {Genuine quantum effects in dicke-type models at large atom numbers}, volume = {135}, year = {2025}, }
• (2025). Correlated quasiparticle poisoning from phonon-only events in superconducting qubits. PRL, 135(12), 123601. (www)

  @article{ , abstract = {Errors that are correlated across a qubit array pose an obstacle to quantum error correction. We observe elevated correlated poisoning rates in superconducting qubit arrays at the start of a cooldown followed by power-law reductions in time, while the rate of offset charge shifts remains constant, evidence of nonionizing sources of pair-breaking phonon bursts. We also investigate different sample packages, with some exhibiting elevated poisoning due to mechanical impacts from the cryocooler. Possible sources include relaxation of built-up stress in device thin films, substrates, or packaging.}, archive = {J_PRL}, author = {E. Yelton and C. P. Larson and K. Dodge and K. Okubo and B. L. T. Plourde}, doi = {10.1103/h65v-ttbw}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {123601}, shortjournal = {Phys. Rev. Lett.}, title = {Correlated quasiparticle poisoning from phonon-only events in superconducting qubits}, volume = {135}, year = {2025}, }
• (2025). Efficiently measuring d-wave pairing and beyond in quantum gas microscopes. PRL, 135(12), 123402. (www)

  @article{ , abstract = {Understanding the mechanism of high-temperature superconductivity is among the most important problems in physics, one for which quantum simulation can provide new insights. However, it remains challenging to characterize superconductivity in existing cold-atom quantum simulation platforms. Here, we introduce a protocol for measuring a broad class of observables in fermionic quantum gas microscopes, including long-range superconducting pairing correlations (after a repulsive-to-attractive mapping). The protocol only requires global controls followed by site-resolved particle number measurements—capabilities that have been already demonstrated in multiple experiments—and is designed by analyzing the Hilbert space of fermions on two sites. The protocol is sample-efficient and we further optimize our pulses for robustness to experimental imperfections such as lattice inhomogeneity. Our Letter introduces a general tool for manipulating quantum states on optical lattices, enhancing their ability to tackle problems such as high-temperature superconductivity.}, archive = {J_PRL}, author = {Daniel K. Mark and Hong-Ye Hu and Joyce Kwan and Christian Kokail and Soonwon Choi and Susanne F. Yelin}, doi = {10.1103/dqyf-kl8x}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {123402}, shortjournal = {Phys. Rev. Lett.}, title = {Efficiently measuring d-wave pairing and beyond in quantum gas microscopes}, volume = {135}, year = {2025}, }
• (2025). Phase transitions in nonreciprocal driven-dissipative condensates. PRL, 135(12), 123401. (www)

  @article{ , abstract = {We investigate the influence of boundaries and spatial nonreciprocity on nonequilibrium driven-dissipative phase transitions. We focus on a one-dimensional lattice of nonlinear bosons described by a Lindblad master equation, where the interplay between coherent and incoherent dynamics generates nonreciprocal interactions between sites. Using a mean-field approach, we analyze the phase diagram under both periodic and open boundary conditions. For periodic boundaries, the system always forms a condensate at nonzero momentum and frequency, resulting in a time-dependent traveling wave pattern. In contrast, open boundaries reveal a far richer phase diagram, featuring multiple static and dynamical phases, as well as exotic phase transitions, including the spontaneous breaking of particle-hole symmetry associated with a critical exceptional point and phases with distinct bulk and edge behavior. Our model does not require postselection and is experimentally realizable in platforms such as superconducting circuits.}, archive = {J_PRL}, author = {Ron Belyansky and Cheyne Weis and Ryo Hanai and Peter B. Littlewood and Aashish A. Clerk}, doi = {10.1103/gphr-d1bc}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {123401}, shortjournal = {Phys. Rev. Lett.}, title = {Phase transitions in nonreciprocal driven-dissipative condensates}, volume = {135}, year = {2025}, }
• (2025). Host-dependent frequency offsets in th229 nuclear clockwork. PRL, 135(12), 123001. (www)

  @article{ , abstract = {Recent advances in laser excitation of the low-energy nuclear isomer transition in have opened avenues for developing nuclear clocks, a novel quantum technology with exceptional performance and sensitivity to exotic physics. Here, we explore the host dependence of the nuclear clock frequency, focusing on the isomer shift induced by the difference in the nuclear charge distribution between the ground and excited nuclear states. We combine relativistic many-body methods of atomic structure with periodic density functional theory to evaluate the isomer shifts in solid-state hosts. We elucidate the critical importance of the “relaxation” effect in evaluating the isomer shifts. Our analysis predicts nuclear clock frequencies for various solid-state and trapped ion platforms: , and . We also determine the nuclear transition energy for the bare nucleus to be . Our calculated valence band isomer shifts for different host materials constrain the nuclear transition frequencies to an 80-MHz-wide frequency window, aiding experimental searches for the nuclear transition in novel materials.}, archive = {J_PRL}, author = {U. C. Perera and H. W. T. Morgan and Eric R. Hudson and Andrei Derevianko}, doi = {10.1103/mhwc-4m14}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {123001}, shortjournal = {Phys. Rev. Lett.}, title = {Host-dependent frequency offsets in th229 nuclear clockwork}, volume = {135}, year = {2025}, }
• (2025). Study of χbJ(2P)→ωϒ(1S) at belle. PRL, 135(12), 121902. (www)

  @article{ , abstract = {We report a study of the hadronic transitions , with , using mesons recorded by the Belle detector. We present the first evidence for the near-threshold transition , the analog of the near-threshold charm sector decay , with a branching fraction of . We also obtain branching fractions of and , confirming the measurement of the transitions of the –wave states. The ratio for the to transitions is also measured and found to differ by 3.3 standard deviations from the expected value in the QCD multipole expansion.}, archive = {J_PRL}, author = {The Belle Collaboration and Z. S. Stottler and T. K. Pedlar and B. G. Fulsom and I. Adachi and K. Adamczyk and H. Aihara and S. Al Said and D. M. Asner and H. Atmacan and T. Aushev and R. Ayad and V. Babu and Sw. Banerjee and M. Bauer and P. Behera and K. Belous and J. Bennett and F. Bernlochner and M. Bessner and T. Bilka and D. Biswas and A. Bobrov and D. Bodrov and G. Bonvicini and J. Borah and A. Bozek and P. Branchini and T. E. Browder and A. Budano and M. Campajola and L. Cao and D. Červenkov and M.-C. Chang and B. G. Cheon and K. Chilikin and H. E. Cho and K. Cho and S.-K. Choi and Y. Choi and S. Choudhury and D. Cinabro and S. Das and G. De Nardo and G. De Pietro and R. Dhamija and F. Di Capua and Z. Doležal and T. V. Dong and S. Dubey and P. Ecker and D. Epifanov and T. Ferber and D. Ferlewicz and V. Gaur and A. Garmash and A. Giri and P. Goldenzweig and E. Graziani and T. Gu and Y. Guan and K. Gudkova and C. Hadjivasiliou and T. Hara and K. Hayasaka and S. Hazra and M. T. Hedges and D. Herrmann and W.-S. Hou and C.-L. Hsu and K. Inami and N. Ipsita and A. Ishikawa and R. Itoh and M. Iwasaki and Y. Iwasaki and W. W. Jacobs and S. Jia and Y. Jin and A. B. Kaliyar and T. Kawasaki and C. Kiesling and C. H. Kim and D. Y. Kim and K.-H. Kim and Y.-K. Kim and P. Kodyš and A. Korobov and S. Korpar and E. Kovalenko and P. Križan and P. Krokovny and T. Kuhr and M. Kumar and R. Kumar and K. Kumara and A. Kuzmin and Y.-J. Kwon and Y.-T. Lai and T. Lam and M. Laurenza and S. C. Lee and D. Levit and P. Lewis and L. K. Li and J. Libby and K. Lieret and D. Liventsev and T. Luo and Y. Ma and M. Masuda and S. K. Maurya and F. Meier and M. Merola and K. Miyabayashi and G. B. Mohanty and I. Nakamura and M. Nakao and A. Natochii and L. Nayak and N. K. Nisar and S. Nishida and K. Ogawa and S. Ogawa and H. Ono and P. Oskin and P. Pakhlov and G. Pakhlova and T. Pang and S. Pardi and J. Park and S.-H. Park and S. Patra and S. Paul and R. Pestotnik and L. E. Piilonen and T. Podobnik and E. Prencipe and M. T. Prim and N. Rout and G. Russo and S. Sandilya and A. Sangal and L. Santelj and V. Savinov and G. Schnell and C. Schwanda and Y. Seino and K. Senyo and W. Shan and M. Shapkin and C. Sharma and J.-G. Shiu and A. Sokolov and E. Solovieva and M. Starič and M. Sumihama and W. Sutcliffe and M. Takizawa and K. Tanida and F. Tenchini and R. Tiwary and M. Uchida and Y. Unno and S. Uno and S. E. Vahsen and G. Varner and D. Wang and E. Wang and M.-Z. Wang and S. Watanuki and O. Werbycka and E. Won and B. D. Yabsley and W. Yan and J. H. Yin and C. Z. Yuan and L. Yuan and Y. Yusa and Z. P. Zhang and V. Zhilich and V. Zhukova}, doi = {10.1103/dpb3-l6zc}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121902}, shortjournal = {Phys. Rev. Lett.}, title = {Study of χbJ(2P)→ωϒ(1S) at belle}, volume = {135}, year = {2025}, }
• (2025). Inclusive semileptonic decays of the ds meson: Lattice QCD confronts experiments. PRL, 135(12), 121901. (www)

  @article{ , abstract = {We present the results of a first-principles theoretical study of the inclusive semileptonic decays of the meson. We performed a state-of-the-art lattice QCD calculation by taking into account all sources of systematic errors. A detailed discussion of our lattice calculation, demonstrating that inclusive semileptonic decays can nowadays be studied on the lattice at a phenomenologically relevant level of accuracy, is the subject of a companion paper [A. De Santis et al. , Inclusive semileptonic decays of the meson: A first-principles lattice QCD calculation, Phys. Rev. D 112 , 054503 (2025)]. Here, we focus on the phenomenological implications of our results. Using the current best estimates of the relevant Cabibbo-Kobayashi-Maskawa (CKM) matrix elements, our theoretical predictions for the decay rate and for the first two lepton-energy moments are in very good agreement with the corresponding experimental measurements. We also argue that, while the inclusive channel is not yet competitive with the exclusive channels in the determination, the situation can be significantly improved in the near future.}, archive = {J_PRL}, author = {Alessandro De Santis and Antonio Evangelista and Roberto Frezzotti and Giuseppe Gagliardi and Paolo Gambino and Marco Garofalo and Christiane Franziska Groß and Bartosz Kostrzewa and Vittorio Lubicz and Francesca Margari and Marco Panero and Francesco Sanfilippo and Silvano Simula and Antonio Smecca and Nazario Tantalo and Carsten Urbach}, doi = {10.1103/snc6-cpz6}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121901}, shortjournal = {Phys. Rev. Lett.}, title = {Inclusive semileptonic decays of the ds meson: Lattice QCD confronts experiments}, volume = {135}, year = {2025}, }
• (2025). Search for millicharged particles in proton-proton collisions at s=13.6 TeV. PRL, 135(12), 121802. (www)

  @article{ , abstract = {We report on a search for elementary particles with charges much smaller than the electron charge using a data sample of proton-proton collisions provided by the CERN Large Hadron Collider in 2023–24, corresponding to an integrated luminosity of 124.7 fb − 1 at a center-of-mass energy of 13.6 TeV. The analysis presented uses the completed Run 3 milliQan bar detector to set the most stringent constraints to date for particles with charges ≤ 0.24 e and masses ≥ 0.45 GeV .}, archive = {J_PRL}, author = {S. Alcott and Z. Bhatti and J. Brooke and C. Campagnari and M. Carrigan and M. Citron and R. De Los Santos and A. De Roeck and C. Dorofeev and T. Du and M. Gastal and J. Goldstein and F. Golf and N. Gonzalez and A. Haas and J. Heymann and C. S. Hill and D. Imani and M. Joyce and K. Larina and R. Loos and S. Lowette and H. Mei and D. W. Miller and B. Peng and S. N. Santpur and I. Reed and E. Schaffer and R. Schmitz and J. Steenis and D. Stuart and J. S. Tafoya Vargas and D. Vannerom and T. Wybouw and Z. Xiao and H. Zaraket and G. Zecchinelli and C. Zheng}, doi = {10.1103/rtp1-679h}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121802}, shortjournal = {Phys. Rev. Lett.}, title = {Search for millicharged particles in proton-proton collisions at s=13.6 TeV}, volume = {135}, year = {2025}, }
• (2025). Measurement of reactor antineutrino oscillation at SNO+. PRL, 135(12), 121801. (www)

  @article{ , abstract = {Collaboration reports its second spectral analysis of reactor antineutrino oscillation using 286 ton-yr of new data. The measured energies of reactor antineutrino candidates were fitted to obtain the second-most precise determination of the neutrino mass-squared difference . Constraining and with measurements from long-baseline reactor antineutrino and solar neutrino experiments yields and . This fit also yields a first measurement of the flux of geoneutrinos in the Western Hemisphere, with TNU at .}, archive = {J_PRL}, author = {math xmlns="http://www.w3.org/1998/Math/MathML" display="inline">SNO+Collaboration</math and M. Abreu and V. Albanese and A. Allega and R. Alves and M. R. Anderson and S. Andringa and L. Anselmo and J. Antunes and E. Arushanova and S. Asahi and M. Askins and D. M. Asner and D. J. Auty and A. R. Back and S. Back and A. Bacon and T. Baltazar and F. Barão and Z. Barnard and A. Barr and N. Barros and D. Bartlett and R. Bayes and C. Beaudoin and E. W. Beier and G. Berardi and T. S. Bezerra and A. Bialek and S. D. Biller and E. Blucher and A. Boeltzig and R. Bonventre and M. Boulay and D. Braid and E. Caden and E. J. Callaghan and J. Caravaca and J. Carvalho and L. Cavalli and D. Chauhan and M. Chen and S. Cheng and O. Chkvorets and K. J. Clark and B. Cleveland and C. Connors and D. Cookman and J. Corning and I. T. Coulter and M. A. Cox and D. Cressy and X. Dai and C. Darrach and S. DeGraw and R. Dehghani and J. Deloye and M. M. Depatie and F. Descamps and C. Dima and J. Dittmer and K. H. Dixon and F. Di Lodovico and A. Doxtator and N. Duhaime and F. Duncan and J. Dunger and A. D. Earle and M. S. Esmaeilian and D. Fabris and E. Falk and A. Farrugia and N. Fatemighomi and C. Felber and V. Fischer and E. Fletcher and R. Ford and K. Frankiewicz and N. Gagnon and A. Gaur and J. Gauthier and A. Gibson-Foster and K. Gilje and O. I. González-Reina and D. Gooding and P. Gorel and K. Graham and C. Grant and J. Grove and S. Grullon and E. Guillian and R. L. Hahn and S. Hall and A. L. Hallin and D. Hallman and S. Hans and J. Hartnell and P. Harvey and C. Hearns and M. R. Hebert and M. Hedayatipour and W. J. Heintzelman and J. Heise and R. L. Helmer and C. Hewitt and B. Hodak and M. Hodak and M. Hood and D. Horne and M. Howe and B. Hreljac and J. Hu and P. Huang and R. Hunt-Stokes and T. Iida and A. S. Inácio and C. M. Jackson and N. A. Jelley and C. J. Jillings and C. Jones and P. G. Jones and S. Kaluzienski and K. Kamdin and T. Kaptanoglu and J. Kaspar and K. Keeter and C. Kefelian and P. Khaghani and L. Kippenbrock and J. Kladnik and J. R. Klein and R. Knapik and J. Kofron and L. L. Kormos and S. Korte and B. Krar and C. Kraus and C. B. Krauss and T. Kroupová and K. Labe and F. Lafleur and C. Lake and I. Lam and C. Lan and B. J. Land and R. Lane and S. Langrock and P. Larochelle and S. Larose and A. LaTorre and I. Lawson and L. Lebanowski and J. Lee and C. Lefebvre and G. M. Lefeuvre and E. J. Leming and A. Li and O. Li and J. Lidgard and B. Liggins and P. Liimatainen and Y. H. Lin and X. Liu and Y. Liu and V. Lozza and M. Luo and S. Maguire and A. Maio and K. Majumdar and S. Manecki and J. Maneira and R. D. Martin and E. Marzec and A. Mastbaum and A. Mathewson and N. McCauley and A. B. McDonald and K. McFarlane and P. Mekarski and M. Meyer and C. Miller and C. Mills and G. Milton and M. Mlejnek and E. Mony and B. Morissette and D. Morris and I. Morton-Blake and M. J. Mottram and M. Mubasher and S. Nae and S. Naugle and M. Newcomer and M. Nirkko and L. J. Nolan and V. M. Novikov and H. M. O’Keeffe and E. O’Sullivan and G. D. Orebi Gann and S. Ouyang and J. Page and S. Pal and K. Paleshi and W. Parker and M. J. Parnell and J. Paton and S. J. M. Peeters and T. Pershing and Z. Petriw and J. Petzoldt and L. J. Pickard and D. Pracsovics and G. Prior and J. C. Prouty and B. Quenallata and S. Quirk and P. Ravi and S. Read and A. Reichold and M. Reinhard and S. Riccetto and M. Rigan and I. Ritchie and A. Robertson and B. C. Robertson and J. Rose and R. Rosero and P. M. Rost and J. Rumleskie and A. Sörensen and P. Schrock and M. A. Schumaker and M. H. Schwendener and D. Scislowski and J. Secrest and M. Seddighin and L. Segui and S. Seibert and I. Semenec and F. Shaker and T. Shantz and M. K. Sharma and J. Shen and T. M. Shokair and L. Sibley and J. Simms and J. R. Sinclair and K. Singh and P. Skensved and M. Smiley and T. Sonley and M. St-Amant and R. Stainforth and S. Stankiewicz and M. Strait and M. I. Stringer and A. Stripay and R. Svoboda and S. Tacchino and R. Tafirout and B. Tam and C. Tanguay and J. Tatar and L. Tian and N. Tolich and J. Tseng and H. W. C. Tseung and E. Turner and E. Vázquez-Jáuregui and S. Valder and R. Van Berg and J. G. C. Veinot and C. J. Virtue and B. von Krosigk and J. M. G. Walker and M. Walker and J. Wallig and S. C. Walton and F. Wang and J. Wang and M. Ward and J. Waterfield and J. J. Weigand and R. F. White and J. F. Wilkerson and J. R. Wilson and J. D. Wilson and T. J. Winchester and P. Woosaree and A. Wright and S. Yang and K. Yazigi and Z. Ye and M. Yeh and S. Yu and T. Zhang and Y. Zhang and T. Zhao and K. Zuber and A. Zummo}, doi = {10.1103/gypt-lc9v}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121801}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of reactor antineutrino oscillation at SNO+}, volume = {135}, year = {2025}, }
• (2025). Modular-invariant random matrix theory and AdS3 wormholes. PRL, 135(12), 121602. (www)

  @article{ , abstract = {We develop a nonperturbative definition of : a generalization of random matrix theory that is compatible with the symmetries of two-dimensional conformal field theory. Given any random matrix ensemble, its -point spectral correlations admit a prescribed modular-invariant lift to , which moreover reduce to the original random matrix correlators in a near-extremal limit. Central to the prescription is a presentation of random matrix theory in Mellin space, which lifts to two dimensions via the spectral decomposition employed in previous work. As a demonstration we perform the explicit lift of two-point correlations of the GUE Airy model. We propose that in pure gravity, semiclassical amplitudes for off-shell -boundary torus wormholes with topology are given by the lift of JT gravity wormhole amplitudes. For the three-boundary case, we identify a gravity calculation which matches the result.}, archive = {J_PRL}, author = {Jan Boruch and Gabriele Di Ubaldo and Felix M. Haehl and Eric Perlmutter and Moshe Rozali}, doi = {10.1103/4hhn-c6mp}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121602}, shortjournal = {Phys. Rev. Lett.}, title = {Modular-invariant random matrix theory and AdS3 wormholes}, volume = {135}, year = {2025}, }
• (2025). Universality class of the first levels in low-dimensional gravity. PRL, 135(12), 121601. (www)

  @article{ , abstract = {We investigate the physics of a small group of quantum states defined above the sharply defined ground state of a chaotic ensemble. This “universality class of the first levels” is realized in the majority of “synthetic” random matrix models but, for all we know, in only one microscopically defined system: low-dimensional gravity. We discuss the physical properties of these states, notably their exceptional rigidity against external perturbations, as quantified by the so-called quantum state fidelity. Examining these structures through the lenses of random matrix and string theory, we highlight their relevance to the physics of low-dimensional holographic principles.}, archive = {J_PRL}, author = {Alexander Altland and Jeremy van der Heijden and Tobias Micklitz and Moshe Rozali and Joaquim Telles de Miranda}, doi = {10.1103/5tn7-knd7}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121601}, shortjournal = {Phys. Rev. Lett.}, title = {Universality class of the first levels in low-dimensional gravity}, volume = {135}, year = {2025}, }
• (2025). Ultrahigh-energy neutrinos from primordial black holes. PRL, 135(12), 121003. (www)

  @article{ , abstract = {The KM3NeT Collaboration recently announced the detection of a neutrino with energy 220 PeV. One possible source of such ultrahigh-energy particles is the rapid emission of energetic Hawking radiation from a primordial black hole (PBH) near the end of its evaporation lifetime. The mass distribution for PBHs features a power-law tail for small masses; a small subset of PBHs would be undergoing late-stage evaporation today. We find that recent high-energy neutrino events detected by the IceCube and KM3NeT Collaborations, with energies O ( 1 − 10 2 ) PeV , are consistent with event-rate expectations if a significant fraction of the dark matter consists of PBHs.}, archive = {J_PRL}, author = {Alexandra P. Klipfel and David I. Kaiser}, doi = {10.1103/vnm4-7wdc}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121003}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrahigh-energy neutrinos from primordial black holes}, volume = {135}, year = {2025}, }
• (2025). Combined annual modulation dark matter search with COSINE-100 and ANAIS-112. PRL, 135(12), 121002. (www)

  @article{ , abstract = {The annual modulation signal, claimed to be consistent with dark matter as observed by DAMA/LIBRA in a sodium-iodide based detector, has persisted for over two decades. COSINE-100 and ANAIS-112 were designed to test the claim directly using the same target material. COSINE-100, located at Yangyang Underground Laboratory in South Korea, and ANAIS-112, located at Canfranc Underground Laboratory in Spain, have been taking data since 2016 and 2017, respectively. Each experiment published its respective results independently. In this Letter, we present the results of an annual modulation search as a test of the signal observed by DAMA/LIBRA with the first three respective years of data from COSINE-100 and ANAIS-112. Using a Markov Chain Monte Carlo method, we find best fit values for modulation amplitude of − 0.0002 ± 0.0026 cpd / kg / keV in the 1–6 keV and 0.0021 ± 0.0028 cpd / kg / keV in the 2–6 keV energy regions. These results are not compatible with DAMA/LIBRA’s assertion for their observation of annual modulation at 3.7 σ and 2.6 σ , respectively. Performing a simple combination of the newly released 6-year datasets from both experiments finds values consistent with no modulation at 0.0005 ± 0.0019 cpd / kg / keV in the 1–6 keV and 0.0027 ± 0.0021 cpd / kg / keV in the 2–6 keV energy regions with 4.7 σ and 3.5 σ respective exclusions of the DAMA/LIBRA signal.}, archive = {J_PRL}, author = {COSINE-100 Collaboration and ANAIS-112 Collaboration and N. Carlin and J. Y. Cho and J. J. Choi and S. Choi and A. C. Ezeribe and L. E. França and C. Ha and I. S. Hahn and S. J. Hollick and S. B. Hong and E. J. Jeon and H. W. Joo and W. G. Kang and M. Kauer and B. H. Kim and H. J. Kim and J. Kim and K. W. Kim and S. H. Kim and S. K. Kim and W. K. Kim and Y. D. Kim and Y. H. Kim and Y. J. Ko and D. H. Lee and E. K. Lee and H. Lee and H. S. Lee and H. Y. Lee and I. S. Lee and J. Lee and J. Y. Lee and M. H. Lee and S. H. Lee and S. M. Lee and Y. J. Lee and D. S. Leonard and N. T. Luan and V. H. A. Machado and B. B. Manzato and R. H. Maruyama and R. J. Neal and S. L. Olsen and H. K. Park and H. S. Park and J. C. Park and J. S. Park and K. S. Park and K. Park and S. D. Park and R. L. C. Pitta and H. Prihtiadi and S. J. Ra and C. Rott and K. A. Shin and D. F. F. S. Cavalcante and M. K. Son and N. J. C. Spooner and L. T. Truc and L. Yang and G. H. Yu and J. Amaré and J. Apilluelo and S. Cebrián and D. Cintas and I. Coarasa and E. García and M. Martínez and Y. Ortigoza and A. Ortiz de Solórzano and T. Pardo and J. Puimedón and M. L. Sarsa and C. Seoane}, doi = {10.1103/9j7w-qp1c}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121002}, shortjournal = {Phys. Rev. Lett.}, title = {Combined annual modulation dark matter search with COSINE-100 and ANAIS-112}, volume = {135}, year = {2025}, }
• (2025). Illuminating black hole shadows with dark matter annihilation. PRL, 135(12), 121001. (www)

  @article{ , abstract = {The Event Horizon Telescope (EHT) has significantly advanced our ability to study black holes, achieving unprecedented spatial resolution and revealing horizon-scale structures. Notably, these observations feature a distinctive dark shadow—primarily arising from faint jet emissions—surrounded by a bright photon ring. Anticipated upgrades of the EHT promise substantial improvements in dynamic range, enabling deeper exploration of low-background regions, particularly the inner shadow defined by the lensed equatorial horizon. Our analysis shows that observations of these regions transform supermassive black holes into powerful probes for annihilating dark matter, which is expected to accumulate densely in their vicinity. By analyzing the black hole image morphology and performing electron-positron propagation calculations in realistic plasma backgrounds derived from general relativistic magnetohydrodynamic simulations, we set stringent constraints on dark matter annihilation, requiring contributions below the astrophysical emission. These constraints, derived from both current EHT observations and projections for future upgraded arrays, exclude a substantial region of previously unexplored parameter space and remain robust against astrophysical uncertainties, including black hole spin and plasma temperature variations.}, archive = {J_PRL}, author = {Yifan Chen and Ran Ding and Yuxin Liu and Yosuke Mizuno and Jing Shu and Haiyue Yu and Yanjie Zeng}, doi = {10.1103/yxqg-363n}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {121001}, shortjournal = {Phys. Rev. Lett.}, title = {Illuminating black hole shadows with dark matter annihilation}, volume = {135}, year = {2025}, }
• (2025). Enhanced gravity sensing by a levitated mesoscopic nanoparticle. PRL, 135(12), 120803. (www)

  @article{ , abstract = {The ground-state cooling and quantum control of levitated nanoparticles have become attainable, which makes the enhanced quantum sensing based on the large mass advantage of mesoscopic quantum systems accessible. Here, we propose an enhanced gravity-sensing protocol for a nanodiamond levitated in a linear ion trap, which improves the sensing sensitivity and further reduces device size. By introducing gravitational acceleration into the vibrational state through transient free fall, we achieve a square-accelerated relative phase accumulation, yielding higher sensitivity than the linear accumulation process. The sensitivity reaches the standard quantum limit for a nanodiamond containing multiple nitrogen-vacancy (N-V) centers. Besides, by using phonon-mediated one-axis twisting dynamics induced by magnetic field gradient to squeeze the initial spin state, the sensitivity can further surpass the standard quantum limit as a scaling law of . To fully assess the protocol performance, we further analyze the effects of decoherence and control errors, which are negligible under experimentally achievable conditions. Specifically, the sensitivity reaches for the nanodiamond containing only one N-V center over a free-fall distance of , while exceeds for 100 N-V centers. Our results will further facilitate research on compact and high-sensitivity gravimeters.}, archive = {J_PRL}, author = {L.-Y. Wang and J.-F. Wei and K.-F. Cui and S.-L. Su and L.-L. Yan and H.-Z. Guo and C.-X. Shan and Gang Chen}, doi = {10.1103/z8b4-sm79}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120803}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced gravity sensing by a levitated mesoscopic nanoparticle}, volume = {135}, year = {2025}, }
• (2025). Quantum stochastic communication via high-dimensional entanglement. PRL, 135(12), 120802. (www)

  @article{ , abstract = {Entanglement has the ability to enhance the transmission of classical information over a quantum channel. However, fully harvesting this advantage typically requires complex entangling measurements, which are challenging to implement and scale with the system’s size. In this Letter, we consider a natural quantum information primitive known as a random access code in which the message to be communicated is selected stochastically. We introduce a protocol that leverages high-dimensional entanglement to perform this task perfectly, without requiring quantum interference between particles at the measurement station. We experimentally demonstrate how this unlocks implementation in the high-dimensional regime through an optical setup using eight-dimensional entanglement and multioutcome detection, providing a practical solution for stochastic communication and a robust method for certifying the dimensionality of entanglement in communication experiments.}, archive = {J_PRL}, author = {Chao Zhang and Jia-Le Miao and Xiao-Min Hu and Jef Pauwels and Yu Guo and Chuan-Feng Li and Guang-Can Guo and Armin Tavakoli and Bi-Heng Liu}, doi = {10.1103/rq78-1qbh}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120802}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum stochastic communication via high-dimensional entanglement}, volume = {135}, year = {2025}, }
• (2025). Cavity-enhanced spin-wave solid-state quantum memory. PRL, 135(12), 120801. (www)

  @article{ , abstract = {We report on the realization of an efficient solid-state spin-wave quantum memory, with on-demand readout, using the full atomic frequency comb (AFC) scheme in a crystal embedded in an impedance-matched cavity. We demonstrate operation at the single-photon level by storing weak coherent states with an efficiency up to and a signal-to-noise ratio of 14 for an input photon number of 0.42 photons per pulse. We also investigated the enhancement of the incoherent noise due to the impedance-matched cavity and characterized the quantum memory performance, showing a two-way transfer from excited to spin states and back of up to 83%. Finally, we confirmed the quantum nature of our memory by storing nonclassical states of light, i.e., a heralded single photon from a nondegenerate spontaneous parametric down-conversion source, and achieved nonclassical correlations between the heralding and the stored-and-retrieved photon. These results demonstrate that impedance-matched AFC spin-wave quantum memories with on-demand readout can be used for experiments involving the storage of photonic quantum states. They also open the door to solid-state on-demand quantum memories with very high efficiencies, serving as a key resource for quantum networks and quantum repeaters.}, archive = {J_PRL}, author = {Leo Feldmann and Sören Wengerowsky and Antariksha Das and Stefano Duranti and Jonathan Hänni and Samuele Grandi and Hugues de Riedmatten}, doi = {10.1103/8l9k-12k2}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120801}, shortjournal = {Phys. Rev. Lett.}, title = {Cavity-enhanced spin-wave solid-state quantum memory}, volume = {135}, year = {2025}, }
• (2025). Designing a nearly optimal quantum algorithm for linear differential equations via lindbladians. PRL, 135(12), 120604. (www)

  @article{ , abstract = {Solving linear ordinary differential equations (ODEs) is one of the most promising applications for quantum computers to demonstrate exponential advantages. The challenge of designing a quantum ODE algorithm is how to embed nonunitary dynamics into intrinsically unitary quantum circuits. In this Letter, we propose a new quantum algorithm for solving ODEs by harnessing open quantum systems. Specifically, we propose a novel technique called nondiagonal density matrix encoding, which leverages the inherent nonunitary dynamics of Lindbladians to encode general linear ODEs into the nondiagonal blocks of density matrices. This framework enables us to design quantum algorithms with both theoretical simplicity and high performance. Combined with the state-of-the-art quantum Lindbladian simulation algorithms, our algorithm can outperform all existing quantum ODE algorithms and achieve near-optimal dependence on all parameters under a plausible input model. We also give applications of our algorithm including the Gibbs state preparations and the partition function estimations.}, archive = {J_PRL}, author = {Zhong-Xia Shang and Naixu Guo and Dong An and Qi Zhao}, doi = {10.1103/cvl9-97qg}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120604}, shortjournal = {Phys. Rev. Lett.}, title = {Designing a nearly optimal quantum algorithm for linear differential equations via lindbladians}, volume = {135}, year = {2025}, }
• (2025). Thresholds for postselected quantum error correction from statistical mechanics. PRL, 135(12), 120603. (www)

  @article{ , abstract = {We identify regimes where postselection can be used scalably in quantum error correction (QEC) to improve performance. We use statistical mechanical models to analytically quantify the performance and thresholds of postselected QEC, with a focus on the surface code. Based on the nonequilibrium magnetization of these models, we identify a simple heuristic technique for postselection that determines whether to abort without requiring a decoder. Along with performance gains, this heuristic allows us to derive analytic expressions for postselected conditional logical thresholds and abort thresholds of surface codes. We find that such postselected QEC is characterized by four distinct thermodynamic phases and detail the implications of this phase space for practical, scalable quantum computation.}, archive = {J_PRL}, author = {Lucas H. English and Dominic J. Williamson and Stephen D. Bartlett}, doi = {10.1103/nh49-52y2}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120603}, shortjournal = {Phys. Rev. Lett.}, title = {Thresholds for postselected quantum error correction from statistical mechanics}, volume = {135}, year = {2025}, }
• (2025). Structural dynamics and strong correlations in dynamical quantum optical lattices. PRL, 135(12), 120602. (www)

  @article{ , abstract = {When placing an ultracold atomic gas inside a cavity, the light-matter coupling is enhanced and nonlinear atomic dynamics is generated, offering a promising platform for quantum simulation of models with short- and long-range interactions. Recently, superradiant self-organized phases for ultracold atomic gases inside a cavity, pumped by a blue detuned optical lattice, have been observed. Here, we explore the formation of quantum many-body phases of bosonic atoms inside an optical cavity, subject to transverse blue detuned pumping. We investigate the strongly interacting regime, which can be reached by tuning the -wave scattering length using external fields. We analyze the interplay between superradiant self-organization with superfluid and Mott insulator phases, without the need of including higher lying bands, as the Wannier functions are dynamically linked to the cavity light via backaction. We observe different kinds of structural phase transitions driven by the light inside the cavity and the interplay with atomic collisions. We observe the mode softening at the critical points in the quantum phase transitions which can be measured in future experiments. We obtain our results within a full self-consistent theoretical framework, the light-matter density matrix renormalization group (DMRG), which employs the computation of light dependent Wannier functions for the full quantum optical lattice in combination with DMRG for the atomic dynamics. The methods introduced here can be used to analyze the effects of strong quantum correlations in strongly interacting light-matter systems.}, archive = {J_PRL}, author = {Adrián U. Ramírez-Barajas and Santiago F. Caballero-Benitez}, doi = {10.1103/gvm2-b46t}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120602}, shortjournal = {Phys. Rev. Lett.}, title = {Structural dynamics and strong correlations in dynamical quantum optical lattices}, volume = {135}, year = {2025}, }
• (2025). Geometric phase transition of the three-dimensional z2 lattice gauge model. PRL, 135(12), 120601. (www)

  @article{ , abstract = {After fifty years of lattice gauge theories (LGTs), the nature of the transition between their topological phases (confinement or deconfinement) remains challenging due to the absence of a local order parameter. In this work, we conduct a percolation analysis of Wegner’s three-dimensional lattice gauge model using intensive Monte Carlo simulations and finite-size scaling, offering fresh insights into the topological phase transitions of gauge-invariant systems. We demonstrate that, regardless of the connection rules, geometrical loops, constructed by piercing excited plaquettes percolate precisely at the thermal critical point , with critical exponents coinciding with those of the loop representation of the dual 3D Ising model. Further, we construct Fortuin-Kasteleyn (FK) clusters in a random-cluster representation, showing that they also percolate at , enabling access to all thermal critical exponents. Strikingly, the Binder cumulants of the percolation order parameters for both loops and FK clusters reveal a pseudo-first-order transition. This work sheds new light on the critical behavior of pure LGTs, with potential implications for condensed matter systems and quantum error correction.}, archive = {J_PRL}, author = {Ramgopal Agrawal and Leticia F. Cugliandolo and Lara Faoro and Lev B. Ioffe and Marco Picco}, doi = {10.1103/33q3-g68k}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120601}, shortjournal = {Phys. Rev. Lett.}, title = {Geometric phase transition of the three-dimensional z2 lattice gauge model}, volume = {135}, year = {2025}, }
• (2025). Quantum theory of the josephson junction between finite islands. PRL, 135(12), 120202. (www)

  @article{ , abstract = {Superconducting circuits comprising Josephson junctions have spurred significant research activity due to their promise to realize scalable quantum computers. Effective Hamiltonians for these systems have traditionally been derived assuming the junction connects superconducting islands of infinite size. We derive a quantized Hamiltonian for a Josephson junction between finite-sized islands and predict measurable corrections to the qubit frequency and charge susceptibility to test the theory.}, archive = {J_PRL}, author = {Thomas J. Maldonado and Alejandro W. Rodriguez and Hakan E. Türeci}, doi = {10.1103/mwvt-wlkj}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120202}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum theory of the josephson junction between finite islands}, volume = {135}, year = {2025}, }
• (2025). Limitations of gaussian measurements in quantum imaging. PRL, 135(12), 120201. (www)

  @article{ , abstract = {Imaging thermal sources naturally yields Gaussian states at the receiver, raising the question of whether Gaussian measurements can perform optimally in quantum imaging. In this Letter, we establish no-go theorems on the performance of Gaussian measurements for imaging thermal sources in the limit of mean photon number per temporal mode ε → 0 or source size L → 0 . We show that non-Gaussian measurements can outperform any Gaussian measurement in the scaling of the estimation variance with ε (or L ). We also present several examples to illustrate the no-go results.}, archive = {J_PRL}, author = {Yunkai Wang and Sisi Zhou}, doi = {10.1103/hnhp-jhr2}, journal = {Physical Review Letters}, month = {9}, number = {12}, pages = {120201}, shortjournal = {Phys. Rev. Lett.}, title = {Limitations of gaussian measurements in quantum imaging}, volume = {135}, year = {2025}, }
• (2025). Negative drag force on beating flagellar-shaped bodies in active fluids. PRL, 135(11), 118301. (www)

  @article{ , abstract = {We experimentally investigate the drag force exerted by a suspension of light-induced active particles (APs) on a translating and beating idealized flagellum-shaped object realized through negative phototactic interactions with the APs. We observe both positive and negative drag forces, depending on the beating frequency and translational velocity, driven by the dynamic redistribution of APs in response to the object’s motion. These findings are supported by numerical simulations and an analytical model, extendable to a range of slender geometries. Our results illustrate the complex interplay between geometric body changes and the density distribution in active baths, which may also be relevant for microrobotic applications.}, archive = {J_PRL}, author = {Timo Knippenberg and Robin Bebon and Thomas Speck and Clemens Bechinger}, doi = {10.1103/3xbk-sxhh}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {118301}, shortjournal = {Phys. Rev. Lett.}, title = {Negative drag force on beating flagellar-shaped bodies in active fluids}, volume = {135}, year = {2025}, }
• (2025). Magic sizes enable minimal-complexity high-fidelity assembly of programmable shells. PRL, 135(11), 118203. (www)

  @article{ , abstract = {Recent advances in synthetic methods enable designing subunits that self-assemble into structures with precise, finite sizes and well-defined architectures, but yields are frequently suppressed by the formation of off-target metastable structures. Increasing the complexity (the number of distinct subunit types) can inhibit off-target structures, but leads to slower kinetics and higher synthesis costs. Here, we study icosahedral shells formed of programmable triangular subunits as a model system, and identify design principles that produce the highest target yield at the lowest complexity. We use a symmetry-based construction to create a range of design complexities, starting from the maximal symmetry Caspar-Klug assembly up to the fully addressable, zero-symmetry assembly. Kinetic Monte Carlo simulations reveal that the most prominent defects leading to off-target assemblies are disclinations at sites of rotational symmetry. We derive symmetry-based rules for identifying the optimal (lowest complexity, highest symmetry) design that inhibits these disclinations, leading to robust high-fidelity assembly of targets with arbitrarily large, yet precise, finite sizes. The optimal complexity varies nonmonotonically with target size, with “magic” sizes appearing for high-symmetry designs in which symmetry axes do not intersect vertices of the triangular net. The optimal designs at magic sizes require 12 times fewer inequivalent interaction types than the (minimal symmetry) fully addressable construction, which greatly reduces the timescale and experimental cost required to achieve high-fidelity assembly of large targets. This symmetry-based principle for pruning off-target assembly generalizes to diverse architectures with different topologies.}, archive = {J_PRL}, author = {Botond Tyukodi and Fernando Caballero and Daichi Hayakawa and Douglas M. Hall and W. Benjamin Rogers and Gregory M. Grason and Michael F. Hagan}, doi = {10.1103/5yjp-kx2j}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {118203}, shortjournal = {Phys. Rev. Lett.}, title = {Magic sizes enable minimal-complexity high-fidelity assembly of programmable shells}, volume = {135}, year = {2025}, }
• (2025). Channel flows of deformable nematics. PRL, 135(11), 118202. (www)

  @article{ , abstract = {We describe channel flows in a continuum model of deformable nematic particles. In a simple shear flow, deformability leads to a nonlinear coupling of strain rate and vorticity, and results in shape oscillations or flow alignment. The final steady state can depend on initial conditions, and we explain this behavior by considering a phase space representation of the dynamics. In Poiseuille flow, particle deformability and nematic elasticity induce banding, where particles near the walls are aligned, and those near the center of the channel oscillate in direction and shape. Our results show that particle deformability can lead to complex behavior even in simple flows, suggesting new microfluidic experiments.}, archive = {J_PRL}, author = {Ioannis Hadjifrangiskou and Sumesh P. Thampi and Julia M. Yeomans}, doi = {10.1103/9mx1-1hk8}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {118202}, shortjournal = {Phys. Rev. Lett.}, title = {Channel flows of deformable nematics}, volume = {135}, year = {2025}, }
• (2025). Power spectra of velocity fluctuations in granular heap flow. PRL, 135(11), 118201. (www)

  @article{ , abstract = {This Letter used speckle visibility spectroscopy to probe velocity fluctuations in three-dimensional granular heap flow. The mean velocity profile comprises a fast-flowing surface layer over a creeping layer. In both layers, velocity fluctuations are scale invariant and self-similar, and the velocity spectra demonstrate power-law scaling, . In the surface layer, is between and , consistent with Hwa and Kardar’s “running” sandpile model, indicative of a dynamically self-organized critical state. In the creep layer, decreases with depth, reaching at a sufficiently deep layer; its theoretical basis remains unclear. Analysis of the fluctuation velocity distributions provides further insight into the microscopic origins of the spectrum. These findings may help resolve the long-standing puzzle of flow localization in gravity-driven granular flows, despite a uniform shear stress-to-pressure ratio.}, archive = {J_PRL}, author = {Shuchang Yu and Jin Shang and Yangrui Chen and Ran Li and Quan Chen and Hui Yang and Hu Zheng and Jie Zhang}, doi = {10.1103/c2w1-wjq6}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {118201}, shortjournal = {Phys. Rev. Lett.}, title = {Power spectra of velocity fluctuations in granular heap flow}, volume = {135}, year = {2025}, }
• (2025). Single-chain nanoparticles break the strength-toughness-processability trilemma in polymer glasses. PRL, 135(11), 118101. (www)

  @article{ , abstract = {The strength-toughness trade-off in polymer glasses presents a fundamental challenge, as enhancing one property typically compromises the other. Moreover, efforts to enhance mechanical performance often lead to increased melt viscosity, which in turn hinders processability. Here, we demonstrate that incorporating single-chain nanoparticles (SCNPs) breaks this trilemma by simultaneously enhancing strength, toughness, and processability. Through a combined experimental and molecular dynamics simulation approach, we reveal that SCNPs with higher glass transition temperature than the matrix not only increase yield strength but also delay and homogenize crazing, leading to dramatically improved toughness in the glassy state. Importantly, the SCNPs reduce melt viscosity in the molten state, countering the conventional trend of viscosity increase in nanocomposites. This triple enhancement establishes a universal framework for designing high-performance polymer glasses that transcend traditional material property limitations.}, archive = {J_PRL}, author = {Lei Zhang and Xu-Ze Zhang and Rui Shi and Shi-Long Wu and Chao-Hao Xu and Ji-Chun You and Yu Zhang and Ming-Yang Li and Wen-Yu Xu and Qing-Lin Li and Zhen-Zhong Yang and Zhong-Yuan Lu and Hu-Jun Qian}, doi = {10.1103/nm5z-2hxm}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {118101}, shortjournal = {Phys. Rev. Lett.}, title = {Single-chain nanoparticles break the strength-toughness-processability trilemma in polymer glasses}, volume = {135}, year = {2025}, }
• (2025). Picosecond expansion in LaAlO3 resonantly driven by infrared-active phonons. PRL, 135(11), 116906. (www)

  @article{ , abstract = {We investigate the ultrafast structural dynamics of thin films driven by short mid-infrared laser pulses at 20 THz. Time-resolved x-ray diffraction reveals an immediate lattice expansion and an acoustic breathing mode of the film. First-principles theory and a spring-mass model identify the direct coupling between coherently driven infrared-active phonons and strain as the underlying mechanism. Time-resolved optical birefringence measurements confirm that the amplitude of this acoustic mode scales linearly with the pump fluence, in agreement with theory. Furthermore, time-resolved x-ray diffuse scattering indicates that THz excitation enhances crystallinity by inducing a nonthermal increase in structural symmetry originating from preexisting defects. These findings highlight the potential of a multimodal approach—combining time-resolved x-ray and optical measurements and first-principles theory—to elucidate and control structural dynamics in nanoscale materials.}, archive = {J_PRL}, author = {Jakob Gollwitzer and Jeffrey Z. Kaaret and Y. Eren Suyolcu and Guru Khalsa and Rylan C. Fernandes and Oleg Gorobtsov and Sören Buchenau and ChanJu You and Jayanti Higgins and Ryan S. Russell and Ziming Shao and Yorick A. Birkhölzer and Takahiro Sato and Matthieu Chollet and Giacomo Coslovich and Mario Brützam and Christo Guguschev and John W. Harter and Ankit S. Disa and Darrell G. Schlom and Nicole A. Benedek and Andrej Singer}, doi = {10.1103/vzkw-n2bm}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116906}, shortjournal = {Phys. Rev. Lett.}, title = {Picosecond expansion in LaAlO3 resonantly driven by infrared-active phonons}, volume = {135}, year = {2025}, }
• (2025). Microwave negative refractive index enabled by anti-parity-time symmetry in a coupled photon-magnon hybrid system. PRL, 135(11), 116905. (www)

  @article{ , abstract = {We experimentally demonstrate that anti-parity-time (anti- ) symmetry can induce a negative refractive index (NRI) in a coupled photon-magnon hybrid system. Using an analytical circuit model, we show that the non-Hermitian dynamics originating from anti- symmetry give rise to antiphase propagation, reversing the phase velocity and resulting in an NRI. Furthermore, we identify cooperativity as the critical threshold parameter dictating the presence of an NRI in the anti- -symmetric regime. These findings provide an alternative framework for manipulating wave propagation and refractive properties in non-Hermitian hybrid quantum systems, opening avenues for advanced control of wave phenomena using magnetic materials.}, archive = {J_PRL}, author = {Junyoung Kim and Bojong Kim and Sang-Koog Kim}, doi = {10.1103/gz3k-7hpp}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116905}, shortjournal = {Phys. Rev. Lett.}, title = {Microwave negative refractive index enabled by anti-parity-time symmetry in a coupled photon-magnon hybrid system}, volume = {135}, year = {2025}, }
• (2025). Photoinduced dynamics and momentum distribution of chiral charge density waves in 1T−TiSe2. PRL, 135(11), 116904. (www)

  @article{ , abstract = {Exploring the photoinduced dynamics of chiral states offers promising avenues for advanced control of condensed matter systems. Photoinduced or photoenhanced chirality in 1 T − TiSe 2 has been suggested as a fascinating platform for optical manipulation of chiral states. However, the mechanisms underlying chirality training and its interplay with the charge density wave (CDW) phase remain elusive. Here, we use time-resolved x-ray diffraction (trXRD) with circularly polarized pump lasers to probe the photoinduced dynamics of chirality in 1 T − TiSe 2 . We observe a notable ( ∼ 20 % ) difference in CDW intensity suppression between left and right circularly polarized pumps. Additionally, we reveal momentum-resolved circular dichroism arising from domains of different chirality, providing a direct link between CDW and chirality. An immediate increase in CDW correlation length upon laser pumping is detected, suggesting the photoinduced expansion of chiral domains. These results both advance the potential of light-driven chirality by elucidating the mechanism driving chirality manipulation in TiSe 2 , and they demonstrate that trXRD with circularly polarized pumps is an effective tool for chirality detection in condensed matter systems.}, archive = {J_PRL}, author = {Qingzheng Qiu and Sae Hwan Chun and Jaeku Park and Dogeun Jang and Li Yue and Yeongkwan Kim and Yeojin Ahn and Mingi Jho and Kimoon Han and Xinyi Jiang and Qian Xiao and Tao Dong and Jia-Yi Ji and Nanlin Wang and Jeroen van den Brink and Jasper van Wezel and Yingying Peng}, doi = {10.1103/7ctk-h28x}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116904}, shortjournal = {Phys. Rev. Lett.}, title = {Photoinduced dynamics and momentum distribution of chiral charge density waves in 1T−TiSe2}, volume = {135}, year = {2025}, }
• (2025). Extended XY model for spinor polariton simulators. PRL, 135(11), 116903. (www)

  @article{ , abstract = {The classic lattice XY model is one of the universal models of statistical mechanics appearing in a broad variety of optical and condensed matter systems. One of its possible realizations is a system of tunnel-coupled spinor polariton condensates, where phases of individual condensates play a role of the two- dimensional spins. We show that the account of the polarization degree of freedom of cavity polaritons adds a new twist to the problem, modifying in particular the structure of the ground state. We formulate the corresponding classical spin Hamiltonian, which couples phase and polarization dynamics, and consider several particular geometries, demonstrating the principal differences between the scalar and spinor cases. Possible analog of spin Meissner effect for coupled condensates is discussed.}, archive = {J_PRL}, author = {A. Kudlis and D. Novokreschenov and I. A. Shelykh}, doi = {10.1103/41k6-yp2l}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116903}, shortjournal = {Phys. Rev. Lett.}, title = {Extended XY model for spinor polariton simulators}, volume = {135}, year = {2025}, }
• (2025). Inverse faraday effect in disordered two-dimensional electronic systems. PRL, 135(11), 116902. (www)

  @article{ , abstract = {I formulate a theory of the inverse Faraday effect in an impure two-dimensional metallic system with lifted spin degeneracy induced by Rashba spin-orbit coupling. Using the formalism of nonequilibrium quantum field theory, the static contributions to the current density up to the second order in powers of the external electromagnetic field are evaluated. For circularly polarized light one of the contributions describes the emergence of static magnetization. It is shown that the direction of induced magnetization may change depending on the frequency of the external radiation and disorder scattering rate. I also find that at large frequencies the leading contribution to the induced magnetization is proportional to the square of the spin-orbit interaction and is inversely proportional to the fifth power of the frequency of an external electromagnetic wave.}, archive = {J_PRL}, author = {Maxim Dzero}, doi = {10.1103/z5nw-9x7b}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116902}, shortjournal = {Phys. Rev. Lett.}, title = {Inverse faraday effect in disordered two-dimensional electronic systems}, volume = {135}, year = {2025}, }
• (2025). Near-field dynamical casimir effect. PRL, 135(11), 116901. (www)

  @article{ , abstract = {We propose the dynamical Casimir effect in a time-modulated near-field system at finite temperatures. The system consists of two bodies made of polaritonic materials that are brought in close proximity to each other, and the modulation frequency is approximately twice the relevant resonance frequencies of the system. We develop a rigorous fluctuational electrodynamics formalism to explore the produced Casimir flux, associated with the degenerate as well as the nondegenerate two-polariton emission processes. We have identified flux contributions from both quantum and thermal fluctuations at finite temperatures, with a dominant quantum contribution even at room temperature under the presence of a strong near-field effect. We have found that the Casimir flux can be generated with a smaller modulation frequency through the higher-order dynamical Casimir effect. We have conducted a nonclassicality test for the total radiative flux at finite temperatures, and we have shown that nonclassical states of emitted photons can be obtained for a high temperature up to . Our findings open an avenue for the exploration of the dynamical Casimir effect beyond cryogenic temperatures, and may be useful for creating tunable nanoscale nonclassical thermal states.}, archive = {J_PRL}, author = {Renwen Yu and Shanhui Fan}, doi = {10.1103/y261-8r5s}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116901}, shortjournal = {Phys. Rev. Lett.}, title = {Near-field dynamical casimir effect}, volume = {135}, year = {2025}, }
• (2025). Stabilization and observation of large-area ferromagnetic bimeron lattice. PRL, 135(11), 116703. (www)

  @article{ , abstract = {Symmetry engineering is an effective approach for generating emergent phases and quantum phenomena. In magnetic systems, the Dzyaloshinskii-Moriya (DM) interaction is essential for stabilizing chiral spin textures. The symmetry manipulation of DM vectors, described in three dimensions, could provide a strategy toward creating abundant topologically magnetic phases. Here, we have achieved breaking the rotational and mirror symmetries of the three-dimensional DM vectors in a strongly correlated ferromagnet, which were directly measured through the nonreciprocal spin-wave propagations in both in-plane and out-of-plane magnetic field geometries. Combining cryogenic magnetic force microscopy and micromagnetic simulations, we discover a bimeron phase that emerges between the spin spiral and skyrmion phases under an applied magnetic field. Such an artificially manipulated DM interaction is shown to play a critical role in the formation and evolution of the large-area bimeron lattice, a phenomenon that could be realized across a broad range of materials. Our findings demonstrate that symmetry engineering of the DM vectors can be practically achieved through epitaxial strain, paving the way for the creation of diverse spin topologies and the exploration of their emergent functionalities.}, archive = {J_PRL}, author = {Miming Cai and Shangyuan Wang and Yuelin Zhang and Xiaoqing Bao and Dekun Shen and Jinghua Ren and Lei Qiu and Haiming Yu and Zhenlin Luo and Mathias Kläui and Shilei Zhang and Nicolas Jaouen and Gerrit van der Laan and Thorsten Hesjedal and Ka Shen and Jinxing Zhang}, doi = {10.1103/587m-xvgv}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116703}, shortjournal = {Phys. Rev. Lett.}, title = {Stabilization and observation of large-area ferromagnetic bimeron lattice}, volume = {135}, year = {2025}, }
• (2025). Single-shot magnetization reversal in ferromagnetic spin valves via heat control. PRL, 135(11), 116702. (www)

  @article{ , abstract = {We study laser-induced ultrafast magnetization reversal in a ferromagnetic spin valve by comparing the effects of direct laser excitation and ultrashort hot-electron pulses. A wedged Cu layer is deposited atop the spin valve to tune energy transmission to the magnetic stack for both optical and hot-electron excitation. We demonstrate single-shot magnetization reversal of the free layer using hot-electron pulses. Moreover, such reversal is achieved even with picosecond laser pulses. The influence of laser fluence, Cu thickness ( ), and pulse duration is investigated in detail. Our results indicate that the key factor enabling magnetization reversal is full demagnetization of the free layer, driven by a rapid rise in its electronic temperature—achieved via either direct laser or hot-electron excitation. This work advances the understanding of ultrafast magnetization reversal via nonlocal heat and spin transport under strongly out-of-equilibrium conditions.}, archive = {J_PRL}, author = {Kazuaki Ishibashi and Junta Igarashi and Alberto Anadón and Michel Hehn and Yann Le Guen and Satoshi Iihama and Julius Hohlfeld and Jon Gorchon and Stéphane Mangin and Grégory Malinowski}, doi = {10.1103/h12x-tcwf}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116702}, shortjournal = {Phys. Rev. Lett.}, title = {Single-shot magnetization reversal in ferromagnetic spin valves via heat control}, volume = {135}, year = {2025}, }
• (2025). Inversion-asymmetric itinerant antiferromagnets by the space group symmetry. PRL, 135(11), 116701. (www)

  @article{ , abstract = {Antiferromagnetic states which break inversion symmetry are able to host odd-parity spin splittings, in analogy to altermagnets. Here we study the emergence of these inversion-asymmetric antiferromagnet (IA AFM) states via an itinerant mechanism in nonsymmorphic systems with two magnetic ions per unit cell. We identify the symmetries that allow mixed-parity irreducible representations for commensurate ordering vectors, and hence permit a continuous transition into the IA AFM. The Landau free energy which describes the transition is derived from a general microscopic model, from which we establish conditions favorable to the appearance of the IA AFM: inversion is not a site symmetry of a magnetic ion, and the nesting involves different bands. Moreover, the odd-parity spin splitting is negatively correlated with the stability of the IA AFM. We illustrate our conclusions with specific examples. The insight into the IA AFM provided by our work can guide the identification of candidate materials.}, archive = {J_PRL}, author = {Changhee Lee and P. M. R. Brydon}, doi = {10.1103/85fd-dmy8}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116701}, shortjournal = {Phys. Rev. Lett.}, title = {Inversion-asymmetric itinerant antiferromagnets by the space group symmetry}, volume = {135}, year = {2025}, }
• (2025). Observation of hybrid degenerate point in projected non-hermitian metasurfaces. PRL, 135(11), 116601. (www)

  @article{ , abstract = {Degeneracy appears ubiquitously in physical systems. Exceptional points, the non-Hermitian degeneracies, have unveiled numerous novel phenomena that have no counterparts in Hermitian degeneracies—diabolic points. Here, we observe a hybrid degenerate point (HP) in a projected non-Hermitian system, namely a subsystem obtained by projecting a metasurface characterized by a Hermitian scattering matrix. In the projected space, the metasurface is found naturally anchored at the merging point of two exceptional curves, each carrying opposite chirality. The HP exhibits a unique topology that encodes features of both Hermitian and non-Hermitian degeneracies, thereby exhibiting linear and square-root sensitivities simultaneously. We conceptually validate and experimentally confirm the projected HP using a passive and lossless acoustic metagrating, uncovering its unique singular behavior: the pronounced anisotropic sensitivity to perturbations. Our findings highlight the potential for exploring degenerate states via the projective Hilbert space and pave the way for extreme wave manipulation in open spaces.}, archive = {J_PRL}, author = {Jingyi Chen and Zhiling Zhou and Yu Xiao and Nengyin Wang and Xu Wang and Yong Li}, doi = {10.1103/9tdx-lcm5}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of hybrid degenerate point in projected non-hermitian metasurfaces}, volume = {135}, year = {2025}, }
• (2025). Unveiling stripe-shaped charge density modulations in doped mott insulators. PRL, 135(11), 116504. (www)

  @article{ , abstract = {Inspired by recent experimental findings, we investigate various scenarios of the doped Hubbard model with impurity potentials. We calculate the lattice Green’s function in a finite-size cluster and then map it to the continuum real space, which allows for a direct comparison with scanning tunneling microscopy measurements on the local density of states. Our simulations successfully reproduce experimental data, including the characteristic stripe- and ladder-shaped structures observed in cuprate systems. Moreover, our results establish a connection between previous numerical findings on stripe-ordered ground states and experimental observations, thus providing new insights into microscopic mechanisms of the Mott insulator to superconductor transition in cuprates.}, archive = {J_PRL}, author = {Ning Xia and Yuchen Guo and Shuo Yang}, doi = {10.1103/hmqb-9q91}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116504}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling stripe-shaped charge density modulations in doped mott insulators}, volume = {135}, year = {2025}, }
• (2025). Interlayer charge transfer induced by electronic instabilities in the natural van der waals heterostructure 4Hb−TaS2. PRL, 135(11), 116503. (www)

  @article{ , abstract = {The natural van der Waals heterostructure composed of alternating - and layers serves as a platform for investigating the electronic correlations and layer-dependent properties of novel quantum materials. The temperature evolution of the conductivity spectra obtained through infrared spectroscopy elucidates the influence of band modifications associated with the charge-density-wave (CDW) superlattice on the layer, resulting in a room-temperature energy gap, . Supported by density functional theory calculations, we attribute the behavior of interband transitions to the convergence of the layers, which amplifies the charge transfer from the to the layers, progressing as the temperature decreases. This phenomenon leads to an enhanced carrier density. The presence of an energy gap and the temperature-tunable charge transfer within the bulk of —driven by layer-dependent CDW states—contribute to a more comprehensive understanding of other complex compounds of transition-metal dichalcogenides.}, archive = {J_PRL}, author = {R. Mathew Roy and X. Feng and M. Wenzel and V. Hasse and C. Shekhar and M. G. Vergniory and C. Felser and A. V. Pronin and M. Dressel}, doi = {10.1103/sgz5-qj71}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116503}, shortjournal = {Phys. Rev. Lett.}, title = {Interlayer charge transfer induced by electronic instabilities in the natural van der waals heterostructure 4Hb−TaS2}, volume = {135}, year = {2025}, }
• (2025). Generalized peierls substitution for wannier obstructions: Response to disorder and interactions. PRL, 135(11), 116502. (www)

  @article{ , abstract = {We study the interplay between quantum geometry, interactions, and external fields in complex band systems. When Wannier obstructions preclude a description based solely on atomiclike orbitals, this complicates the prediction of electromagnetic responses, particularly in the presence of disorder and interactions. In this Letter, we introduce a generalized Peierls substitution framework based on Lagrange multipliers to enforce the constraints of the Wannier obstruction in the band of interest. Thus, we obtain effective descriptions of interactions and disorder in the presence of nontrivial quantum geometry of that band. We apply our approach to examples including the diamagnetic response in flat-band superconductors and delocalization effects in flat-band metals caused by interactions and disorder.}, archive = {J_PRL}, author = {Shuai A. Chen and Roderich Moessner and Tai Kai Ng}, doi = {10.1103/xkxw-1134}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116502}, shortjournal = {Phys. Rev. Lett.}, title = {Generalized peierls substitution for wannier obstructions: Response to disorder and interactions}, volume = {135}, year = {2025}, }
• (2025). Observation of electridelike s states coexisting with correlated d electrons in NdNiO2. PRL, 135(11), 116501. (www)

  @article{ , abstract = {Despite exhibiting a similar band character to cuprates, infinite-layer nickelates host additional electron pockets that distinguish them from single-band cuprates. The elusive orbital origin of these electron pockets has led to competing theoretical scenarios. Here, using polarization-dependent and resonant angle-resolved photoemission spectroscopy, we determine the orbital character of the Fermi surfaces in . Our data reveal that the electronlike pocket arises predominantly from interstitial states, with negligible contributions from rare-earth and orbitals near the Fermi level. The observation of well-defined quantum-well states indicates a uniform distribution of these interstitial electrons throughout the film thickness. By comparing with electronic structure of , we find that the rare-earth element modulates the Ni-derived bands and hopping integrals through a chemical pressure effect. These findings clarify the role of rare-earth elements in shaping the low-energy electronic structure and establish the presence of electridelike interstitial states in a correlated oxide system, where electrons occupy lattice voids rather than atomic orbitals. The electridelike character offers new insight into the self-doping and superconductivity in infinite-layer nickelates.}, archive = {J_PRL}, author = {Chihao Li and Yutong Chen and Xiang Ding and Yezhao Zhuang and Nan Guo and Zhihui Chen and Yu Fan and Jiahao Ye and Zhitong An and Suppanut Sangphet and Shenglin Tang and Xiaoxiao Wang and Hai Huang and Haichao Xu and Donglai Feng and Rui Peng}, doi = {10.1103/tptb-8hb4}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116501}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of electridelike s states coexisting with correlated d electrons in NdNiO2}, volume = {135}, year = {2025}, }
• (2025). Generalized neumann’s principle as a unified framework for fractional quantum and conventional ferroelectricity. PRL, 135(11), 116402. (www)

  @article{ , abstract = {Monolayer exhibits unexpected in-plane polarization, despite having symmetry, a feature that was traditionally considered forbidden by symmetry. To explain this remarkable behavior, Ji et al. proposed the concept of fractional quantum ferroelectricity (FQFE), in which polarization occurs in fractional multiples of a quantum, and argued that this phenomenon violates the conventional Neumann’s principle. In this Letter, we introduce a generalized form of Neumann’s principle and demonstrate that both FQFE and conventional ferroelectricity can be consistently described within this unified theoretical framework. We propose a method, based on the generalized Neumann’s principle, for the systematic identification of FQFE materials. This approach is straightforward to apply and offers a clear conceptual understanding and deep physical insight for FQFE. Using this method, we determine all symmetry-allowed FQFE cases across the 32 crystallographic point groups. Since practical applications rely on the ability to control polarization, we further show that FQFE can be effectively switched via coupling with conventional polarization. Using as an illustrative example, we reveal the underlying mechanism of this coupling and outline a strategy to identify other materials with similar switching behavior.}, archive = {J_PRL}, author = {Hongsheng Pang and Lixin He}, doi = {10.1103/trhd-kxm1}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116402}, shortjournal = {Phys. Rev. Lett.}, title = {Generalized neumann’s principle as a unified framework for fractional quantum and conventional ferroelectricity}, volume = {135}, year = {2025}, }
• (2025). Exciton photoemission from a ground state of a solid: Ta2Pd3Te5. PRL, 135(11), 116401. (www)

  @article{ , abstract = {Excitons are bosonic quasiparticles with a variety of applications in optoelectronics, photosynthesis, and dissipationless informatics, and their lifetime can become sufficiently long to form a quantum condensate. While exciton condensation has been predicted to occur as a ground state of a solid, so-called an excitonic insulator, whose material realization has been elusive. Here we report the observation of direct photoemission signals from excitons in a ground state of a very recent excitonic insulator candidate Ta 2 Pd 3 Te 5 below its metal-insulator transition temperature using orbital-selective angle-resolved photoemission spectroscopy. It is confirmed that the excitons have a lower energy than the valence band maximum to possibly drive the phase transition. This measurement further discloses the size and the unusual odd parity of the exciton wave function. The present finding opens an avenue toward applications of coherent excitons in solid systems and searching for exotic quantum phases of exciton condensates.}, archive = {J_PRL}, author = {Siwon Lee and Kyung-Hwan Jin and SeongJin Kwon and Hyunjin Jung and Choongjae Won and Sang-Wook Cheong and Gil Young Cho and Jaeyoung Kim and Han Woong Yeom}, doi = {10.1103/5kd3-trkg}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116401}, shortjournal = {Phys. Rev. Lett.}, title = {Exciton photoemission from a ground state of a solid: Ta2Pd3Te5}, volume = {135}, year = {2025}, }
• (2025). Thermally bianisotropic metamaterials induced by spatial asymmetry. PRL, 135(11), 116303. (www)

  @article{ , abstract = {Breaking spatial symmetries can induce interactions between disparate physical fields, which manifest in the macroscopic properties of materials as cross-coupling terms. Prominent examples include Willis terms in phononics and bianisotropic terms in photonics. However, the development of analogous cross-couplings in heat conduction remains limited and incomplete; here, we close this knowledge gap. To this end, we introduce an exact and universal homogenization method to capture the macroscopic dynamics of various physical processes in heterogeneous media. For heat conduction and thermodynamics, the method shows that thermal bianisotropy emerges through the intentional design of spatial asymmetry. In certain conditions, the resulting macroscopic description is free from the infinite heat speed paradox inherent in Fourier’s law of conduction. We support the exact theory with examples based on heuristic homogenization of a canonical scattering problem. These results may benefit the design of thermal metamaterials with asymmetric response.}, archive = {J_PRL}, author = {Gal Shmuel and John R. Willis}, doi = {10.1103/tx76-hshd}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116303}, shortjournal = {Phys. Rev. Lett.}, title = {Thermally bianisotropic metamaterials induced by spatial asymmetry}, volume = {135}, year = {2025}, }
• (2025). Universal transport at lifshitz metal-insulator transitions in two dimensions. PRL, 135(11), 116302. (www)

  @article{ , abstract = {We study the charge transport across a band-tuned metal-insulator transition in two dimensions. For high temperatures and chemical potentials far from the transition point, conduction is ballistic and the resistance verifies a simple one-parameter scaling relation. Here, we explore the limits of this semiclassical behavior and study the quantum regime beyond, where scaling breaks down. We analytically evaluate the simplest Feynman diagram of the linear-response conductivity of a parabolic band endowed with a finite lifetime. Our formula shows excellent agreement for experiments for a field-tuned moiré bilayer, and can capture the quantum effects responsible for breaking the one-parameter scaling. We go on to discuss a fascinating prediction of our model: The resistance at the quantum-critical band-tuned Lifshitz point ( ) has the universal value , per degree of freedom, in congruence with experiment. Furthermore, we investigate whether two-dimensional metal-insulator transitions driven by strong electron correlations or disorder can also be classified by their quantum-critical resistance and come up with an, in principle, complete assignment of the transition mechanism.}, archive = {J_PRL}, author = {Harry Tomlins and Jan M. Tomczak}, doi = {10.1103/kc4r-72vj}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116302}, shortjournal = {Phys. Rev. Lett.}, title = {Universal transport at lifshitz metal-insulator transitions in two dimensions}, volume = {135}, year = {2025}, }
• (2025). Electric hall effect and quantum electric hall effect. PRL, 135(11), 116301. (www)

  @article{ , abstract = {Exploring new Hall effect is always a fascinating research topic. The ordinary Hall effect and the quantum Hall effect, initially discovered in two-dimensional (2D) nonmagnetic systems, are the phenomena that a transverse current is generated when a system carrying an electron current is placed in a magnetic field perpendicular to the currents. In this Letter, we propose the electric counterparts of these two Hall effects, termed the “electric Hall effect” (EHE) and the “quantum electric Hall effect” (QEHE). The EHE and QEHE emerge in 2D magnetic systems, where the transverse current is generated by applying an electric gate field instead of a magnetic field. We present a symmetry requirement for both intrinsic EHE and QEHE. Besides, we establish an analytical expression for the intrinsic EHE coefficient when the gate field is weak. We show that it is determined by two band geometric quantities: Berry curvature polarization and Berry curvature polarizability. Via first-principles calculations, we investigate the EHE in the monolayer , where significant EHE coefficient is observed around band crossings. Furthermore, we demonstrate that the QEHE can appear in the semiconductor monolayer , of which the Hall conductivity exhibits steps that take on the quantized values 0 and in the unit of by varying the gate field within the experimentally achievable range. Because of the great tunability of the electric gate field, the EHE and QEHE proposed here can be easily controlled, and should have significant potential applications.}, archive = {J_PRL}, author = {Chaoxi Cui and Run-Wu Zhang and Yuhui Qiu and Yilin Han and Zhi-Ming Yu and Yugui Yao}, doi = {10.1103/5yxp-djy9}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116301}, shortjournal = {Phys. Rev. Lett.}, title = {Electric hall effect and quantum electric hall effect}, volume = {135}, year = {2025}, }
• (2025). Design of frictionless interfaces for moiré layers. PRL, 135(11), 116202. (www)

  @article{ , abstract = {Ultralow friction offers great potential for energy-efficient applications. However, the superlubric sliding of a flake is often plagued by persistent finite friction arising from incomplete moiré tiles at flake edges. To tackle this challenge, we develop a theory of structural frictionless interface based on moiré geometry. Our theory predicts the existence of a directional frictionless interface, which can further evolve to two kinds of all-direction frictionless interfaces, even when the total flake area is not a multiple of the size of a complete moiré tile. Before reaching the frictionless state, friction scales with flake area via a geometry-dependent proportionality factor that encodes frictionless directions, agreeing with large-scale molecular dynamics simulations for both homogeneous or heterogeneous interfaces. Our theory further paves the way for designing frictionless motions in double-interface nanoconfinement channels. Our work provides insights into the creation of structural frictionless interfaces for future advancements in nanoscale tribology and nanoconfinement transport.}, archive = {J_PRL}, author = {Zichong Zhang and Shuze Zhu}, doi = {10.1103/zqw2-sgfq}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116202}, shortjournal = {Phys. Rev. Lett.}, title = {Design of frictionless interfaces for moiré layers}, volume = {135}, year = {2025}, }
• (2025). Hydrophobic versus hydrophilic nature of the gold-water interface determined by fluctuating local water orientation. PRL, 135(11), 116201. (www)

  @article{ , abstract = {The interactions between water molecules and gold surfaces are central to biocompatibility and electrocatalysis, yet their fundamental nature remains highly controversial. Recent findings indicating a molecular-level hydrophobicity have challenged the classical view of gold being hydrophilic. Using surface-specific spectroscopy and ab initio simulations, we demonstrate that gold is neither hydrophobic nor hydrophilic in the classical sense, but exhibits strong electronic interactions with water, resulting in an orientation-dependent electronic heterogeneity. These findings are important for the properties of metal-aqueous interfaces with broad applications.}, archive = {J_PRL}, author = {Tadneem Tabassum and Banshi Das and Chanbum Park and Soumya Ghosh and Dennis Naujoks and Stefan M. Piontek and Alfred Ludwig and Dominik Marx and Poul B. Petersen}, doi = {10.1103/7ht1-xv82}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116201}, shortjournal = {Phys. Rev. Lett.}, title = {Hydrophobic versus hydrophilic nature of the gold-water interface determined by fluctuating local water orientation}, volume = {135}, year = {2025}, }
• (2025). Fast crystallization driven by quasiatomic electrons at ultralow temperatures. PRL, 135(11), 116101. (www)

  @article{ , abstract = {In electride liquids, electrons detach from atomic orbitals and freely occupy the interstitial regions, forming quasiatomic electrons. Here, using dense electride potassium liquid as an example, we uncover a fast crystallization behavior at ultralow temperatures. By combining machine-learned molecular dynamic simulations and ab initio calculations, we demonstrate that this rapid crystallization is attributed to quasiatomic electron flexibility, i.e., self-accommodation of atom size with the help of the change of quasiatomic electrons, particularly the population of involved quasiatomic electrons that is enhanced at low temperatures. This effect not only accelerates atomic mobility but also softens the stiffness of the solid-liquid interface, triggering supercollective atomic motion and enabling rapid crystallization. Our findings challenge conventional views of crystallization kinetics and reveal a previously unrecognized mechanism where electronic contributions play a dominant role in dictating metallic solidification.}, archive = {J_PRL}, author = {Long Zhao and Hongxiang Zong and Artem R. Oganov and Xiangdong Ding and Jun Sun and Graeme J. Ackland}, doi = {10.1103/lp46-x2wy}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116101}, shortjournal = {Phys. Rev. Lett.}, title = {Fast crystallization driven by quasiatomic electrons at ultralow temperatures}, volume = {135}, year = {2025}, }
• (2025). Berezinskii-kosterlitz-thouless renormalization group flow at a quantum phase transition. PRL, 135(11), 116002. (www)

  @article{ , abstract = {We present a controlled numerical study of the Berezinskii-Kosterlitz-Thouless (BKT) transition in the one-dimensional Bose-Hubbard model at unit filling, providing evidence of the characteristic logarithmic finite-size scaling of the BKT transition. Employing density matrix renormalization group and quantum Monte Carlo simulations under periodic boundary conditions, together with a systematic finite-size scaling analysis of bipartite particle number fluctuations, we resolve boundary-induced complications that previously obscured critical scaling. We demonstrate that a suitably chosen central region under open boundaries reproduces universal renormalization group signatures, reconciling earlier discrepancies. Finally, leveraging a nonparametric Bayesian analysis, we determine the critical interaction strength with high precision to be , establishing a benchmark for BKT physics in one-dimensional quantum models.}, archive = {J_PRL}, author = {Matthias Thamm and Harini Radhakrishnan and Hatem Barghathi and C. M. Herdman and Arpan Biswas and Bernd Rosenow and Adrian Del Maestro}, doi = {10.1103/4xdz-5vq7}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116002}, shortjournal = {Phys. Rev. Lett.}, title = {Berezinskii-kosterlitz-thouless renormalization group flow at a quantum phase transition}, volume = {135}, year = {2025}, }
• (2025). Spontaneous vortex-antivortex lattice and majorana fermions in rhombohedral graphene. PRL, 135(11), 116001. (www)

  @article{ , abstract = {The discovery of superconducting states in multilayer rhombohedral graphene with spin and valley polarization [1] has raised an interesting question: how does superconductivity cope with time-reversal symmetry breaking? In this Letter, using Ginzburg-Landau theory and microscopic calculation, we predict the existence of a new superconducting state at low electron density, which exhibits a spontaneously formed lattice of vortices and antivortices hosting Majorana zero modes in their cores. We further identify this vortex-antivortex lattice state in the experimental phase diagram and describe its experimental manifestations.}, archive = {J_PRL}, author = {Filippo Gaggioli and Daniele Guerci and Liang Fu}, doi = {10.1103/k8sb-rqxf}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {116001}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous vortex-antivortex lattice and majorana fermions in rhombohedral graphene}, volume = {135}, year = {2025}, }
• (2025). Theory and experimental observation of scattering by a space-time corner. PRL, 135(11), 113802. (www)

  @article{ , abstract = {The corner problem is a century-old canonical scattering problem describing wave diffraction at a quarter-plane spatial discontinuity. Here, we study its space-time analog: wave scattering at a corner in space-time, arising at a time-switched spatial interface. We highlight and resolve an inconsistency between spatial and temporal boundary conditions arising in this problem, and analytically demonstrate the emergence of shock waves launched by the scattering process. After numerically verifying our theory, we realize and experimentally probe the scattering at a space-time corner arising at the edge of a time-switched waveguide. Our results unveil and efficiently model the unusual phenomena arising at the spatial interface between time-modulated and static media, of great relevance for the growing field of spatiotemporal metamaterials.}, archive = {J_PRL}, author = {Luca Stefanini and Emanuele Galiffi and Shixiong Yin and Sahitya Singh and Diego M. Solís and Nader Engheta and Alessandro Toscano and Davide Ramaccia and Filiberto Bilotti and Andrea Alù}, doi = {10.1103/1p4g-wt7h}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113802}, shortjournal = {Phys. Rev. Lett.}, title = {Theory and experimental observation of scattering by a space-time corner}, volume = {135}, year = {2025}, }
• (2025). Ultraflat soliton microcombs in driven quadratic-kerr nonlinear microresonators. PRL, 135(11), 113801. (www)

  @article{ , abstract = {We predict the generation of ultraflat broadband soliton microcombs in a driven quadratic-Kerr nonlinear microring resonator via phase-matched second-harmonic generation. The unprecedented spectral flatness arises from a novel cavity mechanism of symmetric dispersive wave generation, enabled by opposite group-velocity dispersions—anomalous at the fundamental frequency and normal at the second harmonic—without requiring higher-order dispersion engineering. This mechanism manifests itself as a characteristic long-rippled-wing bright soliton at the second harmonic, thereby generating the ultraflat spectrum. We develop analytical criteria for predicting the radiated frequencies, and show that, under proper control of relative cavity losses, the resulting combs exhibit nearly vanishing ( ) comb-line power variations over a broad spectral range, at variance with platicon microcombs that operate at normal dispersions. Our results offer a pathway to realize octave-spanning, highly efficient, coherent ultraflat combs without needing external phase or intensity modulators, enabling applications such as high-capacity telecommunications, precision metrology, and astrophysical spectrograph calibration.}, archive = {J_PRL}, author = {Gangzhou Wu and Yating Wei and Lingfang Li and Shihua Chen and Lili Bu and Fabio Baronio and Tong Lin and Min Zhu and Stefano Trillo and Zhenhua Ni}, doi = {10.1103/cf1p-k6v6}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113801}, shortjournal = {Phys. Rev. Lett.}, title = {Ultraflat soliton microcombs in driven quadratic-kerr nonlinear microresonators}, volume = {135}, year = {2025}, }
• (2025). Optimal diffractive focusing of matter and light waves. PRL, 135(11), 113604. (www)

  @article{ , abstract = {Following the familiar analogy between the optical paraxial wave equation and the Schrödinger equation, we derive the optimal, real-valued wave function for focusing in one- and two-space dimensions without the use of any phase component. We compare and contrast the focusing parameters of the optimal waves with those of other diffractive focusing approaches, such as Fresnel zones. Moreover, we experimentally demonstrate these focusing properties on optical beams using both reflective and transmissive liquid crystal devices. Our results provide an alternative direction for focusing waves where phase elements are challenging to implement, such as for x-rays, THz radiation, and electron beams.}, archive = {J_PRL}, author = {Maxim A. Efremov and Felix Hufnagel and Hugo Larocque and Wolfgang P. Schleich and Ebrahim Karimi}, doi = {10.1103/h6yy-vvmf}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113604}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal diffractive focusing of matter and light waves}, volume = {135}, year = {2025}, }
• (2025). Floquet engineering of interactions and entanglement in periodically driven rydberg chains. PRL, 135(11), 113603. (www)

  @article{ , abstract = {Neutral atom arrays driven into Rydberg states constitute a promising approach for realizing programmable quantum systems. Enabled by strong interactions associated with Rydberg blockade, they allow for simulation of complex spin models and quantum dynamics. We introduce a new Floquet engineering technique for systems in the blockade regime that provides control over novel forms of interactions and entanglement dynamics in such systems. Our approach is based on time-dependent control of Rydberg laser detuning and leverages perturbations around periodic many-body trajectories as resources for operator spreading. These time-evolved operators are utilized as a basis for engineering interactions in the effective Hamiltonian describing the stroboscopic evolution. As an example, we show how our method can be used to engineer strong spin exchange, consistent with the blockade, in a one-dimensional chain, enabling the exploration of gapless Luttinger liquid phases. In addition, we demonstrate that combining gapless excitations with Rydberg blockade can lead to dynamic generation of large-scale multipartite entanglement. Experimental feasibility and possible generalizations are discussed.}, archive = {J_PRL}, author = {Nazli Ugur Koyluoglu and Nishad Maskara and Johannes Feldmeier and Mikhail D. Lukin}, doi = {10.1103/5qhh-322q}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113603}, shortjournal = {Phys. Rev. Lett.}, title = {Floquet engineering of interactions and entanglement in periodically driven rydberg chains}, volume = {135}, year = {2025}, }
• (2025). Temporally localized quantum operations on continuous-wave thermal light. PRL, 135(11), 113602. (www)

  @article{ , abstract = {Previous work showed that thermal light with a blackbody spectrum cannot be decomposed into a mixture of independent localized pulses. However, we find that in the weak-source limit and under the assumption of a flat spectrum, the first nonvacuum term in the state expansion does form a mixture of such pulses. This decomposition is essential for quantum-enhanced astronomical interferometry, which typically operates on localized pulses even though stellar light is inherently continuous-wave. We present a quantum derivation of the van Cittert–Zernike theorem that incorporates finite bandwidth, thereby justifying the operations on localized pulses while processing continuous-wave thermal light. For general spectra in the weak-source limit, we establish a criterion under which correlations between pulses can be safely neglected. When this criterion is not met, we provide a corrected strategy that accurately accounts for both the spectral profile and the detector-defined pulse shape.}, archive = {J_PRL}, author = {Yunkai Wang and Yujie Zhang and Virginia O. Lorenz}, doi = {10.1103/y4v8-1wgm}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113602}, shortjournal = {Phys. Rev. Lett.}, title = {Temporally localized quantum operations on continuous-wave thermal light}, volume = {135}, year = {2025}, }
• (2025). Selective collective emission from a dense atomic ensemble coupled to a nanophotonic resonator. PRL, 135(11), 113601. (www)

  @article{ , abstract = {We experimentally and theoretically study collective emission of a dense atomic ensemble coupled to a single mode in a nanophotonic microring resonator. Because many cold atoms are localized in a small volume, these trapped atoms collectively couple not only to the guided resonator mode but also to the nonguided modes in free space. Through tuning the atom-photon coupling and by adjusting the number of trapped atoms, we demonstrate superradiant emission to the microring resonator. For photon emission via the nonguided modes, our study reveals signatures of subradiance and superradiance when the system is driven to the steady state and to the timed-Dicke state, respectively. Our experimental platform thus presents the first atom-light interface with selective collective emission behavior into a guided mode and the environment. Our observation and methodology could shed light on future explorations of collective emission with densely packed quantum emitters coupled to nanophotonic light-matter interfaces.}, archive = {J_PRL}, author = {Xinchao Zhou and Deepak A. Suresh and F. Robicheaux and Chen-Lung Hung}, doi = {10.1103/cdd5-r7h4}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113601}, shortjournal = {Phys. Rev. Lett.}, title = {Selective collective emission from a dense atomic ensemble coupled to a nanophotonic resonator}, volume = {135}, year = {2025}, }
• (2025). Medium-enhanced polaron repulsion in a dilute bose mixture. PRL, 135(11), 113402. (www)

  @article{ , abstract = {We investigate the fundamental problem of a small density of bosonic impurities immersed in a dilute Bose gas at zero temperature. Using a rigorous perturbative expansion, we show that the presence of the surrounding medium enhances the repulsion between dressed bosonic impurities (polarons) in the regime of weak interactions. Crucially, this differs from prevailing theories based on Landau quasiparticles, which neglect the possibility of quantum degenerate impurities and predict an exchange-induced attraction. We furthermore show that the polaron-polaron interactions are strongly modified if the medium chemical potential rather than the density is held fixed, such that the medium-induced attraction between thermal impurities becomes twice the expected Landau effective interaction. Our work provides a possible explanation for the differing signs of the polaron-polaron interactions observed in experiments across cold atomic gases and two-dimensional semiconductors, and it has important implications for theories of quasiparticles and quantum mixtures in general.}, archive = {J_PRL}, author = {Jesper Levinsen and Olivier Bleu and Meera M. Parish}, doi = {10.1103/x2xb-6hzv}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113402}, shortjournal = {Phys. Rev. Lett.}, title = {Medium-enhanced polaron repulsion in a dilute bose mixture}, volume = {135}, year = {2025}, }
• (2025). Nonlinear stage of modulational instability in repulsive two-component bose-einstein condensates. PRL, 135(11), 113401. (www)

  @article{ , abstract = {Modulational instability (MI) is a fundamental phenomenon in the study of nonlinear dynamics, spanning diverse areas such as shallow water waves, optics, and ultracold atomic gases. In particular, the nonlinear stage of MI has recently been a topic of intense exploration and has been shown to manifest, in many cases, in the generation of dispersive shock waves (DSWs). In this Letter, we experimentally probe the MI dynamics in an immiscible two-component ultracold atomic gas with exclusively repulsive interactions, catalyzed by a hard-wall-like boundary produced by a repulsive optical barrier. We analytically describe the expansion rate of the DSWs in this system, generalized to arbitrary intercomponent interaction strengths and species ratios. We observe excellent agreement among the analytical results, an effective 1D numerical model, full 3D numerical simulations, and experimental data. Additionally, we extend this scenario to the interaction between two counterpropagating DSWs, which leads to the production of Peregrine soliton structures. These results further demonstrate the versatility of atomic platforms toward the controlled realization of DSWs and rogue waves.}, archive = {J_PRL}, author = {S. Mossman and S. I. Mistakidis and G. C. Katsimiga and A. Romero-Ros and G. Biondini and P. Schmelcher and P. Engels and P. G. Kevrekidis}, doi = {10.1103/6jsr-f8q1}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113401}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear stage of modulational instability in repulsive two-component bose-einstein condensates}, volume = {135}, year = {2025}, }
• (2025). Molecular wave plate for the control of ultrashort pulses carrying orbital angular momentum. PRL, 135(11), 113201. (www)

  @article{ , abstract = {Ultrashort laser pulses carrying orbital angular momentum (OAM) have become essential tools in atomic, molecular, and optical studies, particularly for investigating strong-field light-matter interactions. However, controlling and generating ultrashort vortex pulses presents significant challenges, since their broad spectral content complicates manipulation with conventional optical elements, while the high peak power inherent in short-duration pulses risks damaging optical components. To address these challenges, we demonstrate a “molecular wave plate” as a promising way for generating and controlling broadband ultrashort vortex beams. By exploiting the nonadiabatic alignment of linear gas-phase molecules induced by vector beams, the interaction between the vector beam and the gas-phase molecules results in spatially varying polarizability, imparting a phase modulation to a probe laser. This process effectively creates a tunable molecular wave plate that adapts naturally to a broad spectral range. By leveraging this approach, we can generate ultrashort vortex pulses across a wide range of wavelengths. Under optimized gas pressure and interaction length conditions, this method allows for highly efficient, near unity, conversion of circularly polarized light into the desired OAM pulse, thus enabling the generation of few-cycle, high-intensity vortex beams. This molecular wave plate, which overcomes the limitations imposed by conventional optical elements, opens up new possibilities for exploring strong-field physics, ultrafast science, and other applications that require high-intensity vortex beams.}, archive = {J_PRL}, author = {Chengqing Xu and Lixin He and Wanchen Tao and Xiaosong Zhu and Feng Wang and Long Xu and Lu Xu and Pengfei Lan and Ilya Averbukh and Yehiam Prior and Peixiang Lu}, doi = {10.1103/j2jj-1jns}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113201}, shortjournal = {Phys. Rev. Lett.}, title = {Molecular wave plate for the control of ultrashort pulses carrying orbital angular momentum}, volume = {135}, year = {2025}, }
• (2025). Selective bond breaking in CO22+ induced by photoelectron recoil. PRL, 135(11), 113002. (www)

  @article{ , abstract = {After core ionization of , typically an Auger-Meitner decay takes place, leading to the formation of a dicationic molecule that may dissociate into and . We demonstrate experimentally that the recoil momentum of the photoelectron determines which of the two equivalent bonds breaks during dissociation. At 20 keV photon energy, we observe an asymmetry of up to 25% for bond cleavage that depends on the emission direction of the photoelectron. Furthermore, we show that this effect leads to a significant nondipole effect in molecular dissociation in the laboratory frame: fragments are more likely to be emitted in the direction opposite to the light propagation than along it.}, archive = {J_PRL}, author = {J. Weiherer and N. Melzer and M. Kircher and A. Pier and L. Kaiser and J. Kruse and N. Anders and J. Stindl and L. Sommerlad and O. D. McGinnis and M. Schmidt and J. Drnec and F. Trinter and M. S. Schöffler and L. Ph. H. Schmidt and N. Sisourat and S. Eckart and T. Jahnke and R. Dörner}, doi = {10.1103/qxk7-jt72}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113002}, shortjournal = {Phys. Rev. Lett.}, title = {Selective bond breaking in CO22+ induced by photoelectron recoil}, volume = {135}, year = {2025}, }
• (2025). Testing strong-field QED to second order in the highly correlated atomic system berylliumlike pb78+ by electron-ion collision spectroscopy. PRL, 135(11), 113001. (www)

  @article{ , abstract = {A low-energy storage ring with an ultracold electron cooler has been coupled with a heavy-ion accelerator facilitating high-resolution electron-ion collision spectroscopy of the heaviest few-electron ions. In the present Letter resonant electron-ion recombination of berylliumlike ions was measured in the collision-energy range 9.3–16.5 eV and a value of 244.937(30) eV is derived for the excitation energy. This result agrees with the most recent (less accurate) theoretical value of 244.942(52) eV [Malyshev et al. , Phys. Rev. A 110 , 062824 (2024) ], which has been calculated by applying strong-field QED rigorously up to the second order. The present investigation suggests that further technical improvements can potentially increase the experimental accuracy by an order of magnitude.}, archive = {J_PRL}, author = {S. Schippers and C. Brandau and S. Fuchs and M. Lestinsky and S. X. Wang and C. Y. Zhang and N. R. Badnell and A. Borovik, Jr and M. Fogle and V. Hannen and Z. Harman and P.-M. Hillenbrand and E. B. Menz and Y. Zhang and Z. Andelkovic and F. Herfurth and R. Heß and A. Kalinin and C. Kozhuharov and C. Krantz and S. Litvinov and B. Lorentz and U. Spillmann and M. Steck and G. Vorobyev and D. Banaś and S. Fritzsche and E. Lindroth and X. Ma and A. Müller and R. Schuch and A. Surzhykov and M. Trassinelli and K. Ueberholz and C. Weinheimer and Th. Stöhlker}, doi = {10.1103/6j3v-lwxj}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {113001}, shortjournal = {Phys. Rev. Lett.}, title = {Testing strong-field QED to second order in the highly correlated atomic system berylliumlike pb78+ by electron-ion collision spectroscopy}, volume = {135}, year = {2025}, }
• (2025). Contribution of subthreshold states to the residual energy distribution of dy159. PRL, 135(11), 112502. (www)

  @article{ , abstract = {We investigate the residual energy distribution in the electron capture (EC) process of , emphasizing the role of subthreshold atomic states, which have typically been omitted in conventional spectral analyses. By incorporating these energetically forbidden hole states into the spectral function , we demonstrate a significant enhancement—over an order of magnitude—in the EC rate near the zero-momentum neutrino emission region. This enhancement increases further with larger values, contrary to standard expectations. Our analysis shows that can be experimentally determined, resolving ambiguities near the end point and enabling new approaches to “ultralow value” EC reactions for neutrino mass studies.}, archive = {J_PRL}, author = {Tadafumi Kishimoto and Toru Sato}, doi = {10.1103/l8mm-33m7}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {112502}, shortjournal = {Phys. Rev. Lett.}, title = {Contribution of subthreshold states to the residual energy distribution of dy159}, volume = {135}, year = {2025}, }
• (2025). Evidence of oscillating neutron-capture cross sections. PRL, 135(11), 112501. (www)

  @article{ , abstract = {Analysis of neutron-capture cross sections in the resolved resonance range reveals that a large fraction of them (13 of 21, or 62%) exhibit highly significant ( confidence level) oscillations about their average value. Oscillations exceed a significance level of in nine cases (43%). Oscillations comprise of the average cross section with periods ranging from 68.2 to 2380 eV. This contradicts random matrix theory (RMT), which predicts that fluctuations about the average cross section should be entirely random and demonstrates that deviations from RMT are common and widespread in neutron-capture data. These facts suggest there is a widespread physical mechanism that is missing from current nuclear physics models describing neutron-capture cross sections.}, archive = {J_PRL}, author = {P. E. Koehler and A. Stamatopoulos}, doi = {10.1103/bh31-4qq6}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {112501}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence of oscillating neutron-capture cross sections}, volume = {135}, year = {2025}, }
• (2025). Modification of the jet energy-energy correlator in cold nuclear matter. PRL, 135(11), 112302. (www)

  @article{ , abstract = {We compute medium corrections to the energy-energy correlator (EEC) for jets in electron-nucleus collisions at leading order in the QCD coupling and the interaction of the jet with the medium. We derive an analytical expression for the modification of the EEC as a function of the opening angle and show that the modification is strongest at large angles within the jet cone. We obtain explicit results for the dependence of the modification on the jet energy, the scattering power of cold nuclear matter, and the path length within the medium. We extend our calculations to gluon jets in proton-nucleus collisions and compare our results with recent preliminary data for proton-lead collisions at the LHC. We also discuss the role of comovers on the EEC in p + Pb collisions.}, archive = {J_PRL}, author = {Yu Fu and Berndt Müller and Chathuranga Sirimanna}, doi = {10.1103/qxdv-cmrg}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {112302}, shortjournal = {Phys. Rev. Lett.}, title = {Modification of the jet energy-energy correlator in cold nuclear matter}, volume = {135}, year = {2025}, }
• (2025). Probing gluon fluctuations in nuclei with the first energy-dependent measurement of incoherent j/ψ photoproduction in ultraperipheral PbPb collisions. PRL, 135(11), 112301. (www)

  @article{ , abstract = {Incoherent photoproduction in heavy ion ultraperipheral collisions (UPCs) provides a sensitive probe of localized, fluctuating gluonic structures within heavy nuclei. This Letter reports the first measurement of the photon-nucleon center-of-mass energy ( ) dependence of this process in PbPb UPCs at a nucleon-nucleon center-of-mass energy of 5.02 TeV, using of data recorded by the CMS experiment. The measurement covers a wide range of , probing gluons carrying a fraction of nucleon momentum down to an unexplored regime of . Compared to baseline predictions neglecting nuclear effects, the measured cross sections exhibit significantly greater suppression at lower . Additionally, the ratio of incoherent to coherent photoproduction is found to be constant across the probed and range, disfavoring the establishment of the black disk limit. This Letter provides critical insights into the -dependent evolution of fluctuating gluonic structures within nuclei and calls for further advancements in theoretical models incorporating nuclear shadowing and gluon saturation.}, archive = {J_PRL}, author = {CMS Collaboration and V. Chekhovsky and A. Hayrapetyan and V. Makarenko and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and H. Kwon and T. Van Laer and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and Y. Hong and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and A. Khalilzadeh and F. A. Khan and K. Lee and A. Malara and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and J. Knolle and L. Lambrecht and D. Marckx and K. Skovpen and N. Van Den Bossche and J. van der Linden and J. Vandenbroeck and L. Wezenbeek and S. Bein and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and S. Turkcapar and G. A. Alves and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and E. J. Tonelli Manganote and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and T. Laux Kuhn and M. Macedo and J. Martins and K. Mota Amarilo and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and V. Scheurer and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and D. Laroze and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and Y. Zhao and C. Zhou and S. Yang and Z. Ye and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and H. Wang and K. Yi and J. Zhang and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and J. Jaramillo and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and R. Aly and Y. Assran and S. Elgammal and M. Abdullah Al-Mashad and M. A. Mahmoud and K. Ehataht and M. Kadastik and T. Lange and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and K. Osterberg and M. Voutilainen and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Myllymäki and M. m. Rantanen and J. Tuominiemi and H. Kirschenmann and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and A. Cappati and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Nguyen and S. Obraztsov and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and G. Sokmen and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and I. Lomidze and T. Toriashvili and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and A. Cardini and F. Colombina and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and S. Zakharov and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and T. Chwalek and A. Dierlamm and G. G. Dincer and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and O. Lavoryk and J. M. Lawhorn and M. Link and A. Lintuluoto and S. Maier and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and R. Schmieder and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and B. Topko and N. Trevisani and T. Voigtländer and R. F. Von Cube and J. Von Den Driesch and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and G. Melachroinos and Z. Painesis and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and P. Major and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Baradia and S. Barman and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and T. Mishra and B. Parida and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and S. Bhowmik and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and B. M. Joshi and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and K. Naskar and A. Nayak and S. Nayak and K. Pal and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and G. Lavizzari and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and D. Bisello and P. Bortignon and G. Bortolato and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and F. Gasparini and U. Gasparini and S. Giorgetti and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and F. Montecassiano and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and M. Tosi and A. Triossi and S. Ventura and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and V. K. Muraleedharan Nair Bindhu and M. Musich and S. Nandan and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and P. Barria and C. Basile and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and R. Gargiulo and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and J. Yoo and J. Goh and Y. Kang and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and K. Hwang and B. Kim and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and F. E. Neri Huerta and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and A. Bellora and L. Forthomme and L. Grzanka and M. Malawski and K. Piotrzkowski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and M. Stojanovic and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and C. Martin Perez and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and E. Palencia Cortezon and J. Prado Pico and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and A. A. Bin Anuar and A. Bocci and L. Borgonovi and C. Botta and A. Bragagnolo and E. Brondolin and C. E. Brown and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and M. Glowacki and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and G. Karathanasis and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and M. Magherini and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and M. Pitt and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and Y. Maghrbi and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and Y. Komurcu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and E. Uslan and I. S. Zorbakir and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and V. J. Smith and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and O. Buchmuller and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and V. Hegde and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and C. Cosby and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and L. Gouskos and M. Hadley and U. Heintz and K. W. Ho and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and J. Luo and S. Mondal and T. Russell and S. Sagir and X. Shen and M. Stamenkovic and N. Venkatasubramanian and S. Abbott and B. Barton and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and S. Yoo and F. Zhang and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and D. Primosch and M. Quinnan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and M. M. Hussain and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and X. Yan and D. Zhang and A. Bornheim and O. Cerri and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and M. Kanemura and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and N. Manganelli and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and X. Chen and D. J. Cranshaw and J. Dickinson and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and I. Dutta and V. D. Elvira and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and K. Maeshima and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and P. Roy and T. Roy and S. Rudrabhatla and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and S. Popescu and C. Rogan and C. Royon and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Wang and L. Zhang and C. Baldenegro Barrera and J. Bendavid and S. Bright-Thonney and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and A. Rohilla and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and P. Levchenko and J. Li and M. Lu and R. Mccarthy and D. M. Morse and T. Orimoto and A. Parker and L. Skinnari and E. Tsai and D. Wood and S. Dittmer and K. A. Hahn and D. Li and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and P. Fackeldey and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and F. Simpson and D. Stickland and C. Tully and L. H. Vage and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and J. F. Schulte and A. K. Virdi and F. Wang and A. Wildridge and W. Xie and Y. Yao and J. Dolen and N. Parashar and A. Pathak and D. Acosta and A. Agrawal and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and X. Huang and I. Krommydas and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and J. Reichert and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and A. Safonov and N. Akchurin and J. Damgov and Y. Feng and N. Gogate and Y. Kazhykarim and K. Lamichhane and C. Madrid and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and D. Rathjens and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Mantilla and C. Neu and C. Ramón Álvarez and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and D. Budkouski and I. Golutvin and I. Gorbunov and V. Karjavine and O. Kodolova and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and A. Nikitenko and V. Palichik and V. Perelygin and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and V. Smirnov and O. Teryaev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and Yu. Andreev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and I. Tlisova and A. Toropin and T. Aushev and K. Ivanov and V. Gavrilov and N. Lychkovskaya and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and A. Ershov and A. Gribushin and L. Khein and V. Korotkikh and O. Lukina and S. Petrushanko and V. Savrin and A. Snigirev and I. Vardanyan and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and Y. Skovpen and V. Kachanov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin}, doi = {10.1103/w9kp-f8xr}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {112301}, shortjournal = {Phys. Rev. Lett.}, title = {Probing gluon fluctuations in nuclei with the first energy-dependent measurement of incoherent j/ψ photoproduction in ultraperipheral PbPb collisions}, volume = {135}, year = {2025}, }
• (2025). Bayesian inferring nucleon gravitational form factors via near-threshold j/ψ photoproduction. PRL, 135(11), 111902. (www)

  @article{ , abstract = {With Bayesian inference, we investigate the impact of recent near-threshold 𝐽 / 𝜓 production measurements by the 𝐽 / 𝜓 ⁢ 0 0 7 experiment and GlueX Collaboration on the extraction of proton gravitational form factors. We apply the generalized parton distribution framework at the next to leading order and demonstrate a stable expansion for the near-threshold kinematics. We find that the experimental constraints are in good agreement with the state-of-the-art lattice simulations, where negative 𝐶 𝑞 ⁡ ( 𝑡 ) and 𝐶 𝑔 ⁡ ( 𝑡 ) are strongly preferred. This highlights a great potential to extract them from future high-precision experiments.}, archive = {J_PRL}, author = {Yuxun Guo and Feng Yuan and Wenbin Zhao}, doi = {10.1103/3x7r-ythq}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111902}, shortjournal = {Phys. Rev. Lett.}, title = {Bayesian inferring nucleon gravitational form factors via near-threshold j/ψ photoproduction}, volume = {135}, year = {2025}, }
• (2025). Measurement of two-point energy correlators within jets in p+p collisions at s=200 GeV. PRL, 135(11), 111901. (www)

  @article{ , abstract = {Hard-scattered partons ejected from high-energy proton-proton collisions undergo parton shower and hadronization, resulting in collimated collections of particles that are clustered into jets. A substructure observable that highlights the transition between the perturbative and nonperturbative regimes of jet evolution in terms of the angle between two particles is the two-point energy correlator (EEC). In this Letter, the first measurement of the EEC at RHIC is presented, using data taken from 200 GeV collisions by the STAR experiment. The EEC is measured both for all the pairs of particles in jets and separately for pairs with like and opposite electric charges. These measurements demonstrate that the transition between perturbative and nonperturbative effects occurs within an angular region that is consistent with expectations of a universal hadronization regime that scales with jet momentum for a given initiator flavor. Additionally, a deviation from Monte Carlo predictions at small angles in the charge-selected sample could result from mechanics of hadronization not fully captured by current models.}, archive = {J_PRL}, author = {STAR Collaboration and B. E. Aboona and J. Adam and G. Agakishiev and I. Aggarwal and M. M. Aggarwal and Z. Ahammed and A. Aitbayev and I. Alekseev and E. Alpatov and A. K. Alshammri and A. Aparin and S. Aslam and J. Atchison and G. S. Averichev and V. Bairathi and X. Bao and K. Barish and S. Behera and P. Bhagat and A. Bhasin and S. Bhatta and J. Bielcik and J. Bielcikova and I. G. Bordyuzhin and J. D. Brandenburg and A. V. Brandin and C. Broodo and X. Z. Cai and H. Caines and M. Calderón de la Barca Sánchez and D. Cebra and J. Ceska and I. Chakaberia and Y. S. Chang and Z. Chang and A. Chatterjee and D. Chen and J. H. Chen and Q. Chen and Z. Chen and J. Cheng and Y. Cheng and W. Christie and X. Chu and S. Corey and H. J. Crawford and G. Dale-Gau and A. Das and T. G. Dedovich and I. M. Deppner and A. A. Derevschikov and A. Deshpande and A. Dhamija and A. Dimri and P. Dixit and X. Dong and J. L. Drachenberg and E. Duckworth and J. C. Dunlop and J. Engelage and G. Eppley and S. Esumi and O. Evdokimov and O. Eyser and R. Fatemi and S. Fazio and Y. Feng and E. Finch and Y. Fisyak and F. A. Flor and C. Fu and T. Fu and T. Gao and F. Geurts and A. Gibson and K. Gopal and X. Gou and D. Grosnick and A. Gu and A. Gupta and A. Hamed and R. J. Hamilton and X. Han and M. D. Harasty and J. W. Harris and H. Harrison-Smith and L. B. Havener and X. H. He and Y. He and C. Hu and Q. Hu and Y. Hu and H. Huang and H. Z. Huang and S. L. Huang and T. Huang and Y. Huang and M. Isshiki and W. W. Jacobs and A. Jalotra and C. Jena and Y. Ji and J. JJia and C. Jin and N. Jindal and X. Ju and E. G. Judd and S. Kabana and D. Kalinkin and K. Kang and D. Kapukchyan and K. Kauder and D. Keane and A. Kechechyan and M. Kesler and A. Khanal and J. Kim and A. Kiselev and A. G. Knospe and L. Kochenda and A. A. Korobitsin and B. Korodi and A. Yu. Kraeva and P. Kravtsov and L. Kumar and M. C. Labonte and R. Lacey and J. M. Landgraf and C. Larson and A. Lebedev and R. Lednicky and J. H. Lee and Y. H. Leung and D. Li and H-S. Li and H. Li and W. Li and X. Li and Y. Li and Z. Li and X. Liang and T. Lin and Y. Lin and C. Liu and G. Liu and H. Liu and L. Liu and Z. Liu and T. Ljubicic and O. Lomicky and R. S. Longacre and E. M. Loyd and T. Lu and J. Luo and X. F. Luo and V. B. Luong and Ma and R. Ma and Y. G. Ma and N. Magdy and R. Manikandhan and S. Margetis and O. Matonoha and O. Mezhanska and K. Mi and N. G. Minaev and B. Mohanty and B. Mondal and M. M. Mondal and I. Mooney and D. A. Morozov and M. I. Nagy and C. J. Naim and A. S. Nain and J. D. Nam and M. Nasim and H. Nasrulloh and E. Nedorezov and J. M. Nelson and M. Nie and G. Nigmatkulov and T. Niida and L. V. Nogach and T. Nonaka and G. Odyniec and A. Ogawa and S. Oh and V. A. Okorokov and K. Okubo and B. S. Page and S. Pal and A. Pandav and A. Panday and A. K. Pandey and Y. Panebratsev and T. Pani and P. Parfenov and A. Paul and S. Paul and C. Perkins and B. R. Pokhrel and I. D. Ponce Pinto and M. Posik and E. Pottebaum and A. Povarov and S. Prodhan and T. L. Protzman and N. K. Pruthi and J. Putschke and Z. Qin and H. Qiu and C. Racz and S. K. Radhakrishnan and A. Rana and R. L. Ray and C. W. Robertson and O. V. Rogachevsky and M. A. Rosales Aguilar and D. Roy and L. Ruan and A. K. Sahoo and N. R. Sahoo and H. Sako and S. Salur and S. S. Sambyal and E. Samigullin and J. K. Sandhu and S. Sato and B. C. Schaefer and N. Schmitz and J. Seger and R. Seto and P. Seyboth and N. Shah and E. Shahaliev and P. V. Shanmuganathan and T. Shao and M. Sharma and N. Sharma and R. Sharma and S. R. Sharma and A. I. Sheikh and D. Shen and D. Y. Shen and K. Shen and S. Shi and Y. Shi and F. Si and J. Singh and S. Singha and P. Sinha and M. J. Skoby and Y. Söhngen and Y. Song and T. D. S. Stanislaus and M. Strikhanov and Y. Su and X. Sun and Y. Sun and B. Surrow and D. N. Svirida and Z. W. Sweger and A. C. Tamis and A. H. Tang and Z. Tang and A. Taranenko and T. Tarnowsky and J. H. Thomas and D. Tlusty and M. V. Tokarev and D. Torres Valladares and S. Trentalange and P. Tribedy and B. Trzeciak and O. D. Tsai and C. Y. Tsang and Z. Tu and J. E. Tyler and T. Ullrich and D. G. Underwood and G. Van Buren and A. N. Vasiliev and F. Videbæk and S. Vokal and S. A. Voloshin and G. Wang and J. S. Wang and J. Wang and K. Wang and X. Wang and Y. Wang and Z. Wang and J. C. Webb and P. C. Weidenkaff and G. D. Westfall and H. Wieman and G. Wilks and S. W. Wissink and C. P. Wong and J. Wu and X. Wu and B. Xi and Z. G. Xiao and G. Xie and W. Xie and H. Xu and N. Xu and Q. H. Xu and Y. Xu and Z. Xu and G. Yan and Z. Yan and C. Yang and Q. Yang and S. Yang and Y. Yang and Z. Ye and L. Yi and Y. Yu and W. Zha and C. Zhang and D. Zhang and J. Zhang and S. Zhang and W. Zhang and X. Zhang and Y. Zhang and Z. Zhang and F. Zhao and J. Zhao and S. Zhou and Y. Zhou and X. Zhu and M. Zurek and M. Zyzak}, doi = {10.1103/wv2t-dkgn}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111901}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of two-point energy correlators within jets in p+p collisions at s=200 GeV}, volume = {135}, year = {2025}, }
• (2025). Nucleon decays into light new particles in neutrino detectors. PRL, 135(11), 111804. (www)

  @article{ , abstract = {Proton and neutron decays into light new particles X can drastically change the experimental signatures and benefit from the complementarity of large water-Cherenkov neutrino detectors such as Super- and Hyper-Kamiokande and tracking detectors such as JUNO and DUNE. The proton decays p → ℓ + X and p → π + X with m X near phase-space closure lead to charged particles below the Cherenkov threshold, rendering them practically invisible in Super- and Hyper-Kamiokande but not in JUNO and DUNE, which are therefore uniquely positioned for these baryon-number-violating signatures despite their smaller size. As an additional signature, such nucleon decays in the Earth can produce a sizable flux of X particles in underground detectors. We present a simple model in which nucleons decay into sub-GeV sterile neutrinos that subsequently decay through active-sterile neutrino mixing, with a promisingly large number of events in Super-Kamiokande even in the seesaw-motivated parameter space.}, archive = {J_PRL}, author = {Julian Heeck and Ian M. Shoemaker}, doi = {10.1103/cxvm-p412}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111804}, shortjournal = {Phys. Rev. Lett.}, title = {Nucleon decays into light new particles in neutrino detectors}, volume = {135}, year = {2025}, }
• (2025). Precise measurement of the form factors in D0→K*(892)−μ+νμ, and test of lepton universality with D0→K*(892)−ℓ+νℓ decays. PRL, 135(11), 111803. (www)

  @article{ , abstract = {We report a study of the semileptonic decay based on a sample of of annihilation data collected at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider. The branching fraction of the decay is measured for the first time to be , where the first uncertainty is statistical and the second is systematic. Based on the investigation of the decay dynamics, we find that the decay is dominated by the resonance with the branching fraction measured to be . We also determine the hadronic form factors for the decay to be , and , where is the vector form factor and are the axial-vector form factors evaluated at . The is measured for the first time in decay. Averaging the form factor parameters that we reported previously in and decays, we obtain , and . This is the most precise determination of the form factor parameters to date measured in transitions, which provide the most stringent test on various theoretical models.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. Q. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. Gao and Y. N. Gao and Y. Y. Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Q. A. Malik and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. J. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and L. Q. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Y. P. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/zfxr-dlzg}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111803}, shortjournal = {Phys. Rev. Lett.}, title = {Precise measurement of the form factors in D0→K*(892)−μ+νμ, and test of lepton universality with D0→K*(892)−ℓ+νℓ decays}, volume = {135}, year = {2025}, }
• (2025). Evidence for longitudinally polarized w bosons in the electroweak production of same-sign w boson pairs in association with two jets in pp collisions at s=13 TeV with the ATLAS detector. PRL, 135(11), 111802. (www)

  @article{ , abstract = {This Letter reports the first evidence of electroweak production of same-sign boson pairs where at least one of the bosons is longitudinally polarized and the most stringent constraint to date for the production of two longitudinally polarized same-sign bosons. The dataset used corresponds to an integrated luminosity of of proton-proton collisions at a center-of-mass energy of 13 TeV, collected with the ATLAS detector during run 2 of the Large Hadron Collider. The study is performed in final states including two same-sign leptons (electrons or muons), missing transverse momentum, and at least two jets with a large invariant mass and a large rapidity difference. Two independent fits are performed targeting the production of same-sign bosons with at least one, or two longitudinally polarized bosons. The observed (expected) significance of the production with at least one longitudinally polarized boson is 3.3 (4.0) standard deviations. An observed (expected) 95% confidence level upper limit of 0.45 (0.70) fb is reported on the fiducial production cross section of two longitudinally polarized same-sign bosons.}, archive = {J_PRL}, author = {ATLAS Collaboration and G. Aad and E. Aakvaag and B. Abbott and S. Abdelhameed and K. Abeling and N. J. Abicht and S. H. Abidi and M. Aboelela and A. Aboulhorma and H. Abramowicz and Y. Abulaiti and B. S. Acharya and A. Ackermann and C. Adam Bourdarios and L. Adamczyk and S. V. Addepalli and M. J. Addison and J. Adelman and A. Adiguzel and T. Adye and A. A. Affolder and Y. Afik and M. N. Agaras and A. Aggarwal and C. Agheorghiesei and F. Ahmadov and S. Ahuja and X. Ai and G. Aielli and A. Aikot and M. Ait Tamlihat and B. Aitbenchikh and M. Akbiyik and T. P. A. Åkesson and A. V. Akimov and D. Akiyama and N. N. Akolkar and S. Aktas and G. L. Alberghi and J. Albert and P. Albicocco and G. L. Albouy and S. Alderweireldt and Z. L. Alegria and M. Aleksa and I. N. Aleksandrov and C. Alexa and T. Alexopoulos and F. Alfonsi and M. Algren and M. Alhroob and B. Ali and H. M. J. Ali and S. Ali and S. W. Alibocus and M. Aliev and G. Alimonti and W. Alkakhi and C. Allaire and B. M. M. Allbrooke and J. S. Allen and J. F. Allen and P. P. Allport and A. Aloisio and F. Alonso and C. Alpigiani and Z. M. K. Alsolami and A. Alvarez Fernandez and M. Alves Cardoso and M. G. Alviggi and M. Aly and Y. Amaral Coutinho and A. Ambler and C. Amelung and M. Amerl and C. G. Ames and T. Amezza and D. Amidei and B. Amini and K. Amirie and A. Amirkhanov and S. P. Amor Dos Santos and K. R. Amos and D. Amperiadou and S. An and C. Anastopoulos and T. Andeen and J. K. Anders and A. C. Anderson and A. Andreazza and S. Angelidakis and A. Angerami and A. V. Anisenkov and A. Annovi and C. Antel and E. Antipov and M. Antonelli and F. Anulli and M. Aoki and T. Aoki and M. A. Aparo and L. Aperio Bella and M. Apicella and C. Appelt and A. Apyan and S. J. Arbiol Val and C. Arcangeletti and A. T. H. Arce and J-F. Arguin and S. Argyropoulos and J.-H. Arling and O. Arnaez and H. Arnold and G. Artoni and H. Asada and K. Asai and S. Asai and S. Asatryan and N. A. Asbah and R. A. Ashby Pickering and A. M. Aslam and K. Assamagan and R. Astalos and K. S. V. Astrand and S. Atashi and R. J. Atkin and H. Atmani and P. A. Atmasiddha and K. Augsten and A. D. Auriol and V. A. Austrup and G. Avolio and K. Axiotis and G. Azuelos and D. Babal and H. Bachacou and K. Bachas and A. Bachiu and E. Bachmann and M. J. Backes and A. Badea and T. M. Baer and P. Bagnaia and M. Bahmani and D. Bahner and K. Bai and J. T. Baines and L. Baines and O. K. Baker and E. Bakos and D. Bakshi Gupta and L. E. Balabram Filho and V. Balakrishnan and R. Balasubramanian and E. M. Baldin and P. Balek and E. Ballabene and F. Balli and L. M. Baltes and W. K. Balunas and J. Balz and I. Bamwidhi and E. Banas and M. Bandieramonte and A. Bandyopadhyay and S. Bansal and L. Barak and M. Barakat and E. L. Barberio and D. Barberis and M. Barbero and M. Z. Barel and T. Barillari and M-S. Barisits and T. Barklow and P. Baron and D. A. Baron Moreno and A. Baroncelli and A. J. Barr and J. D. Barr and F. Barreiro and J. Barreiro Guimarães da Costa and M. G. Barros Teixeira and S. Barsov and F. Bartels and R. Bartoldus and A. E. Barton and P. Bartos and A. Basan and M. Baselga and S. Bashiri and A. Bassalat and M. J. Basso and S. Bataju and R. Bate and R. L. Bates and S. Batlamous and M. Battaglia and D. Battulga and M. Bauce and M. Bauer and P. Bauer and L. T. Bayer and L. T. Bazzano Hurrell and J. B. Beacham and T. Beau and J. Y. Beaucamp and P. H. Beauchemin and P. Bechtle and H. P. Beck and K. Becker and A. J. Beddall and V. A. Bednyakov and C. P. Bee and L. J. Beemster and M. Begalli and M. Begel and J. K. Behr and J. F. Beirer and F. Beisiegel and M. Belfkir and G. Bella and L. Bellagamba and A. Bellerive and C. D. Bellgraph and P. Bellos and K. Beloborodov and D. Benchekroun and F. Bendebba and Y. Benhammou and K. C. Benkendorfer and L. Beresford and M. Beretta and E. Bergeaas Kuutmann and N. Berger and B. Bergmann and J. Beringer and G. Bernardi and C. Bernius and F. U. Bernlochner and F. Bernon and A. Berrocal Guardia and T. Berry and P. Berta and A. Berthold and A. Berti and R. Bertrand and S. Bethke and A. Betti and A. J. Bevan and L. Bezio and N. K. Bhalla and S. Bharthuar and S. Bhatta and P. Bhattarai and Z. M. Bhatti and K. D. Bhide and V. S. Bhopatkar and R. M. Bianchi and G. Bianco and O. Biebel and M. Biglietti and C. S. Billingsley and Y. Bimgdi and M. Bindi and A. Bingham and A. Bingul and C. Bini and G. A. Bird and M. Birman and M. Biros and S. Biryukov and T. Bisanz and E. Bisceglie and J. P. Biswal and D. Biswas and I. Bloch and A. Blue and U. Blumenschein and J. Blumenthal and V. S. Bobrovnikov and L. Boccardo and M. Boehler and B. Boehm and D. Bogavac and A. G. Bogdanchikov and L. S. Boggia and V. Boisvert and P. Bokan and T. Bold and M. Bomben and M. Bona and M. Boonekamp and A. G. Borbély and I. S. Bordulev and G. Borissov and D. Bortoletto and D. Boscherini and M. Bosman and K. Bouaouda and N. Bouchhar and L. Boudet and J. Boudreau and E. V. Bouhova-Thacker and D. Boumediene and R. Bouquet and A. Boveia and J. Boyd and D. Boye and I. R. Boyko and L. Bozianu and J. Bracinik and N. Brahimi and G. Brandt and O. Brandt and B. Brau and J. E. Brau and R. Brener and L. Brenner and R. Brenner and S. Bressler and G. Brianti and D. Britton and D. Britzger and I. Brock and R. Brock and G. Brooijmans and A. J. Brooks and E. M. Brooks and E. Brost and L. M. Brown and L. E. Bruce and T. L. Bruckler and P. A. Bruckman de Renstrom and B. Brüers and A. Bruni and G. Bruni and D. Brunner and M. Bruschi and N. Bruscino and T. Buanes and Q. Buat and D. Buchin and A. G. Buckley and O. Bulekov and B. A. Bullard and S. Burdin and C. D. Burgard and A. M. Burger and B. Burghgrave and O. Burlayenko and J. Burleson and J. C. Burzynski and E. L. Busch and V. Büscher and P. J. Bussey and J. M. Butler and C. M. Buttar and J. M. Butterworth and W. Buttinger and C. J. Buxo Vazquez and A. R. Buzykaev and S. Cabrera Urbán and L. Cadamuro and D. Caforio and H. Cai and Y. Cai and V. M. M. Cairo and O. Cakir and N. Calace and P. Calafiura and G. Calderini and P. Calfayan and G. Callea and L. P. Caloba and D. Calvet and S. Calvet and R. Camacho Toro and S. Camarda and D. Camarero Munoz and P. Camarri and C. Camincher and M. Campanelli and A. Camplani and V. Canale and A. C. Canbay and E. Canonero and J. Cantero and Y. Cao and F. Capocasa and M. Capua and A. Carbone and R. Cardarelli and J. C. J. Cardenas and M. P. Cardiff and G. Carducci and T. Carli and G. Carlino and J. I. Carlotto and B. T. Carlson and E. M. Carlson and J. Carmignani and L. Carminati and A. Carnelli and M. Carnesale and S. Caron and E. Carquin and I. B. Carr and S. Carrá and G. Carratta and A. M. Carroll and M. P. Casado and P. Casolaro and M. Caspar and F. L. Castillo and L. Castillo Garcia and V. Castillo Gimenez and N. F. Castro and A. Catinaccio and J. R. Catmore and T. Cavaliere and V. Cavaliere and L. J. Caviedes Betancourt and E. Celebi and S. Cella and V. Cepaitis and K. Cerny and A. S. Cerqueira and A. Cerri and L. Cerrito and F. Cerutti and B. Cervato and A. Cervelli and G. Cesarini and S. A. Cetin and P. M. Chabrillat and R. Chakkappai and S. Chakraborty and J. Chan and W. Y. Chan and J. D. Chapman and E. Chapon and B. Chargeishvili and D. G. Charlton and C. Chauhan and Y. Che and S. Chekanov and S. V. Chekulaev and G. A. Chelkov and B. Chen and H. Chen and J. Chen and M. Chen and S. Chen and S. J. Chen and X. Chen and Z. Chen and C. L. Cheng and H. C. Cheng and S. Cheong and A. Cheplakov and E. Cherepanova and R. Cherkaoui El Moursli and E. Cheu and K. Cheung and L. Chevalier and V. Chiarella and G. Chiarelli and G. Chiodini and A. S. Chisholm and A. Chitan and M. Chitishvili and M. V. Chizhov and K. Choi and Y. Chou and E. Y. S. Chow and K. L. Chu and M. C. Chu and X. Chu and Z. Chubinidze and J. Chudoba and J. J. Chwastowski and D. Cieri and K. M. Ciesla and V. Cindro and A. Ciocio and F. Cirotto and Z. H. Citron and M. Citterio and D. A. Ciubotaru and A. Clark and P. J. Clark and N. Clarke Hall and C. Clarry and S. E. Clawson and C. Clement and Y. Coadou and M. Cobal and A. Coccaro and R. F. Coelho Barrue and R. Coelho Lopes De Sa and S. Coelli and L. S. Colangeli and B. Cole and P. Collado Soto and J. Collot and R. Coluccia and P. Conde Muiño and M. P. Connell and S. H. Connell and E. I. Conroy and M. Contreras Cossio and F. Conventi and H. G. Cooke and A. M. Cooper-Sarkar and L. Corazzina and F. A. Corchia and A. Cordeiro Oudot Choi and L. D. Corpe and M. Corradi and F. Corriveau and A. Cortes-Gonzalez and M. J. Costa and F. Costanza and D. Costanzo and B. M. Cote and J. Couthures and G. Cowan and K. Cranmer and L. Cremer and D. Cremonini and S. Crépé-Renaudin and F. Crescioli and T. Cresta and M. Cristinziani and M. Cristoforetti and V. Croft and J. E. Crosby and G. Crosetti and A. Cueto and H. Cui and Z. Cui and W. R. Cunningham and F. Curcio and J. R. Curran and M. J. Da Cunha Sargedas De Sousa and J. V. Da Fonseca Pinto and C. Da Via and W. Dabrowski and T. Dado and S. Dahbi and T. Dai and D. Dal Santo and C. Dallapiccola and M. Dam and G. D’amen and V. D’Amico and J. Damp and J. R. Dandoy and D. Dannheim and G. D’anniballe and M. Danninger and V. Dao and G. Darbo and S. J. Das and F. Dattola and S. D’Auria and A. D’Avanzo and T. Davidek and J. Davidson and I. Dawson and K. De and C. De Almeida Rossi and R. De Asmundis and N. De Biase and S. De Castro and N. De Groot and P. de Jong and H. De la Torre and A. De Maria and A. De Salvo and U. De Sanctis and F. De Santis and A. De Santo and J. B. De Vivie De Regie and J. Debevc and D. V. Dedovich and J. Degens and A. M. Deiana and J. Del Peso and L. Delagrange and F. Deliot and C. M. Delitzsch and M. Della Pietra and D. Della Volpe and A. Dell’Acqua and L. Dell’Asta and M. Delmastro and C. C. Delogu and P. A. Delsart and S. Demers and M. Demichev and S. P. Denisov and H. Denizli and L. D’Eramo and D. Derendarz and F. Derue and P. Dervan and A. M. Desai and K. Desch and F. A. Di Bello and A. Di Ciaccio and L. Di Ciaccio and A. Di Domenico and C. Di Donato and A. Di Girolamo and G. Di Gregorio and A. Di Luca and B. Di Micco and R. Di Nardo and K. F. Di Petrillo and M. Diamantopoulou and F. A. Dias and M. A. Diaz and A. R. Didenko and M. Didenko and S. D. Diefenbacher and E. B. Diehl and S. Díez Cornell and C. Diez Pardos and C. Dimitriadi and A. Dimitrievska and A. Dimri and J. Dingfelder and T. Dingley and I-M. Dinu and S. J. Dittmeier and F. Dittus and M. Divisek and B. Dixit and F. Djama and T. Djobava and C. Doglioni and A. Dohnalova and Z. Dolezal and K. Domijan and K. M. Dona and M. Donadelli and B. Dong and J. Donini and A. D’Onofrio and M. D’Onofrio and J. Dopke and A. Doria and N. Dos Santos Fernandes and P. Dougan and M. T. Dova and A. T. Doyle and M. A. Draguet and M. P. Drescher and E. Dreyer and I. Drivas-koulouris and M. Drnevich and M. Drozdova and D. Du and T. A. du Pree and Z. Duan and M. Dubau and F. Dubinin and M. Dubovsky and E. Duchovni and G. Duckeck and P. K. Duckett and O. A. Ducu and D. Duda and A. Dudarev and E. R. Duden and M. D’uffizi and L. Duflot and M. Dührssen and I. Duminica and A. E. Dumitriu and M. Dunford and S. Dungs and K. Dunne and A. Duperrin and H. Duran Yildiz and M. Düren and A. Durglishvili and D. Duvnjak and G. I. Dyckes and M. Dyndal and B. S. Dziedzic and Z. O. Earnshaw and G. H. Eberwein and B. Eckerova and S. Eggebrecht and E. Egidio Purcino De Souza and G. Eigen and K. Einsweiler and T. Ekelof and P. A. Ekman and S. El Farkh and Y. El Ghazali and H. El Jarrari and A. El Moussaouy and V. Ellajosyula and M. Ellert and F. Ellinghaus and N. Ellis and J. Elmsheuser and M. Elsawy and M. Elsing and D. Emeliyanov and Y. Enari and I. Ene and S. Epari and D. Ernani Martins Neto and F. Ernst and M. Errenst and M. Escalier and C. Escobar and E. Etzion and G. Evans and H. Evans and L. S. Evans and A. Ezhilov and S. Ezzarqtouni and F. Fabbri and L. Fabbri and G. Facini and V. Fadeyev and R. M. Fakhrutdinov and D. Fakoudis and S. Falciano and L. F. Falda Ulhoa Coelho and F. Fallavollita and G. Falsetti and J. Faltova and C. Fan and K. Y. Fan and Y. Fan and Y. Fang and M. Fanti and M. Faraj and Z. Farazpay and A. Farbin and A. Farilla and T. Farooque and J. N. Farr and S. M. Farrington and F. Fassi and D. Fassouliotis and L. Fayard and P. Federic and P. Federicova and O. L. Fedin and M. Feickert and L. Feligioni and D. E. Fellers and C. Feng and Z. Feng and M. J. Fenton and L. Ferencz and B. Fernandez Barbadillo and P. Fernandez Martinez and M. J. V. Fernoux and J. Ferrando and A. Ferrari and P. Ferrari and R. Ferrari and D. Ferrere and C. Ferretti and M. P. Fewell and D. Fiacco and F. Fiedler and P. Fiedler and S. Filimonov and M. S. Filip and A. Filipčič and E. K. Filmer and F. Filthaut and M. C. N. Fiolhais and L. Fiorini and W. C. Fisher and T. Fitschen and P. M. Fitzhugh and I. Fleck and P. Fleischmann and T. Flick and M. Flores and L. R. Flores Castillo and L. Flores Sanz De Acedo and F. M. Follega and N. Fomin and J. H. Foo and A. Formica and A. C. Forti and E. Fortin and A. W. Fortman and L. Foster and L. Fountas and D. Fournier and H. Fox and P. Francavilla and S. Francescato and S. Franchellucci and M. Franchini and S. Franchino and D. Francis and L. Franco and V. Franco Lima and L. Franconi and M. Franklin and G. Frattari and Y. Y. Frid and J. Friend and N. Fritzsche and A. Froch and D. Froidevaux and J. A. Frost and Y. Fu and S. Fuenzalida Garrido and M. Fujimoto and K. Y. Fung and E. Furtado De Simas Filho and M. Furukawa and J. Fuster and A. Gaa and A. Gabrielli and P. Gadow and G. Gagliardi and L. G. Gagnon and S. Gaid and S. Galantzan and J. Gallagher and E. J. Gallas and A. L. Gallen and B. J. Gallop and K. K. Gan and S. Ganguly and Y. Gao and A. Garabaglu and F. M. Garay Walls and C. García and A. Garcia Alonso and A. G. Garcia Caffaro and J. E. García Navarro and M. Garcia-Sciveres and G. L. Gardner and R. W. Gardner and N. Garelli and R. B. Garg and J. M. Gargan and C. A. Garner and C. M. Garvey and V. K. Gassmann and G. Gaudio and V. Gautam and P. Gauzzi and J. Gavranovic and I. L. Gavrilenko and A. Gavrilyuk and C. Gay and G. Gaycken and E. N. Gazis and A. Gekow and C. Gemme and M. H. Genest and A. D. Gentry and S. George and T. Geralis and A. A. Gerwin and P. Gessinger-Befurt and M. E. Geyik and M. Ghani and K. Ghorbanian and A. Ghosal and A. Ghosh and B. Giacobbe and S. Giagu and T. Giani and A. Giannini and S. M. Gibson and M. Gignac and D. T. Gil and A. K. Gilbert and B. J. Gilbert and D. Gillberg and G. Gilles and D. M. Gingrich and M. P. Giordani and P. F. Giraud and G. Giugliarelli and D. Giugni and F. Giuli and I. Gkialas and L. K. Gladilin and C. Glasman and M. Glazewska and R. M. Gleason and G. Glemža and M. Glisic and I. Gnesi and Y. Go and M. Goblirsch-Kolb and B. Gocke and D. Godin and B. Gokturk and S. Goldfarb and T. Golling and M. G. D. Gololo and D. Golubkov and J. P. Gombas and A. Gomes and G. Gomes Da Silva and A. J. Gomez Delegido and R. Gonçalo and L. Gonella and A. Gongadze and F. Gonnella and J. L. Gonski and R. Y. González Andana and S. González de la Hoz and M. V. Gonzalez Rodrigues and R. Gonzalez Suarez and S. Gonzalez-Sevilla and L. Goossens and B. Gorini and E. Gorini and A. Gorišek and T. C. Gosart and A. T. Goshaw and M. I. Gostkin and S. Goswami and C. A. Gottardo and S. A. Gotz and M. Gouighri and A. G. Goussiou and N. Govender and R. P. Grabarczyk and I. Grabowska-Bold and K. Graham and E. Gramstad and S. Grancagnolo and C. M. Grant and P. M. Gravila and F. G. Gravili and H. M. Gray and M. Greco and M. J. Green and C. Grefe and A. S. Grefsrud and I. M. Gregor and K. T. Greif and P. Grenier and S. G. Grewe and A. A. Grillo and K. Grimm and S. Grinstein and J.-F. Grivaz and E. Gross and J. Grosse-Knetter and L. Guan and G. Guerrieri and R. Guevara and R. Gugel and J. A. M. Guhit and A. Guida and E. Guilloton and S. Guindon and F. Guo and J. Guo and L. Guo and Y. Guo and A. Gupta and R. Gupta and S. Gupta and S. Gurbuz and S. S. Gurdasani and G. Gustavino and P. Gutierrez and L. F. Gutierrez Zagazeta and M. Gutsche and C. Gutschow and C. Gwenlan and C. B. Gwilliam and E. S. Haaland and A. Haas and M. Habedank and C. Haber and H. K. Hadavand and A. Haddad and A. Hadef and A. I. Hagan and J. J. Hahn and E. H. Haines and M. Haleem and J. Haley and G. D. Hallewell and L. Halser and K. Hamano and M. Hamer and S. E. D. Hammoud and E. J. Hampshire and J. Han and L. Han and S. Han and K. Hanagaki and M. Hance and D. A. Hangal and H. Hanif and M. D. Hank and J. B. Hansen and P. H. Hansen and D. Harada and T. Harenberg and S. Harkusha and M. L. Harris and Y. T. Harris and J. Harrison and N. M. Harrison and P. F. Harrison and M. L. E. Hart and N. M. Hartman and N. M. Hartmann and R. Z. Hasan and Y. Hasegawa and F. Haslbeck and S. Hassan and R. Hauser and M. Haviernik and C. M. Hawkes and R. J. Hawkings and Y. Hayashi and D. Hayden and C. Hayes and R. L. Hayes and C. P. Hays and J. M. Hays and H. S. Hayward and M. He and Y. He and N. B. Heatley and V. Hedberg and C. Heidegger and K. K. Heidegger and J. Heilman and S. Heim and T. Heim and J. G. Heinlein and J. J. Heinrich and L. Heinrich and J. Hejbal and M. Helbig and A. Held and S. Hellesund and C. M. Helling and S. Hellman and A. M. Henriques Correia and H. Herde and Y. Hernández Jiménez and L. M. Herrmann and T. Herrmann and G. Herten and R. Hertenberger and L. Hervas and M. E. Hesping and N. P. Hessey and J. Hessler and M. Hidaoui and N. Hidic and E. Hill and T. S. Hillersoy and S. J. Hillier and J. R. Hinds and F. Hinterkeuser and M. Hirose and S. Hirose and D. Hirschbuehl and T. G. Hitchings and B. Hiti and J. Hobbs and R. Hobincu and N. Hod and A. M. Hodges and M. C. Hodgkinson and B. H. Hodkinson and A. Hoecker and D. D. Hofer and J. Hofer and M. Holzbock and L. B. A. H. Hommels and V. Homsak and B. P. Honan and J. J. Hong and T. M. Hong and B. H. Hooberman and W. H. Hopkins and M. C. Hoppesch and Y. Horii and M. E. Horstmann and S. Hou and M. R. Housenga and A. S. Howard and J. Howarth and J. Hoya and M. Hrabovsky and T. Hryn’ova and P. J. Hsu and S.-C. Hsu and T. Hsu and M. Hu and Q. Hu and S. Huang and X. Huang and Y. Huang and Z. Huang and Z. Hubacek and M. Huebner and F. Huegging and T. B. Huffman and M. Hufnagel Maranha De Faria and C. A. Hugli and M. Huhtinen and S. K. Huiberts and R. Hulsken and C. E. Hultquist and N. Huseynov and J. Huston and J. Huth and R. Hyneman and G. Iacobucci and G. Iakovidis and L. Iconomidou-Fayard and J. P. Iddon and P. Iengo and R. Iguchi and Y. Iiyama and T. Iizawa and Y. Ikegami and D. Iliadis and N. Ilic and H. Imam and G. Inacio Goncalves and S. A. Infante Cabanas and T. Ingebretsen Carlson and J. M. Inglis and G. Introzzi and M. Iodice and V. Ippolito and R. K. Irwin and M. Ishino and W. Islam and C. Issever and S. Istin and K. Itabashi and H. Ito and R. Iuppa and A. Ivina and V. Izzo and P. Jacka and P. Jackson and P. Jain and K. Jakobs and T. Jakoubek and J. Jamieson and W. Jang and S. Jankovych and M. Javurkova and P. Jawahar and L. Jeanty and J. Jejelava and P. Jenni and C. E. Jessiman and C. Jia and H. Jia and J. Jia and X. Jia and Z. Jia and C. Jiang and Q. Jiang and S. Jiggins and M. Jimenez Ortega and J. Jimenez Pena and S. Jin and A. Jinaru and O. Jinnouchi and P. Johansson and K. A. Johns and J. W. Johnson and F. A. Jolly and D. M. Jones and E. Jones and K. S. Jones and P. Jones and R. W. L. Jones and T. J. Jones and H. L. Joos and R. Joshi and J. Jovicevic and X. Ju and J. J. Junggeburth and T. Junkermann and A. Juste Rozas and M. K. Juzek and S. Kabana and A. Kaczmarska and M. Kado and H. Kagan and M. Kagan and A. Kahn and C. Kahra and T. Kaji and E. Kajomovitz and N. Kakati and N. Kakoty and I. Kalaitzidou and S. Kandel and N. J. Kang and D. Kar and K. Karava and E. Karentzos and O. Karkout and S. N. Karpov and Z. M. Karpova and V. Kartvelishvili and A. N. Karyukhin and E. Kasimi and J. Katzy and S. Kaur and K. Kawade and M. P. Kawale and C. Kawamoto and T. Kawamoto and E. F. Kay and F. I. Kaya and S. Kazakos and V. F. Kazanin and J. M. Keaveney and R. Keeler and G. V. Kehris and J. S. Keller and J. J. Kempster and O. Kepka and J. Kerr and B. P. Kerridge and B. P. Kerševan and L. Keszeghova and R. A. Khan and A. Khanov and A. G. Kharlamov and T. Kharlamova and E. E. Khoda and M. Kholodenko and T. J. Khoo and G. Khoriauli and Y. Khoulaki and J. Khubua and Y. A. R. Khwaira and B. Kibirige and D. Kim and D. W. Kim and Y. K. Kim and N. Kimura and M. K. Kingston and A. Kirchhoff and C. Kirfel and F. Kirfel and J. Kirk and A. E. Kiryunin and S. Kita and O. Kivernyk and M. Klassen and C. Klein and L. Klein and M. H. Klein and S. B. Klein and U. Klein and A. Klimentov and T. Klioutchnikova and P. Kluit and S. Kluth and E. Kneringer and T. M. Knight and A. Knue and M. Kobel and D. Kobylianskii and S. F. Koch and M. Kocian and P. Kodyš and D. M. Koeck and T. Koffas and O. Kolay and I. Koletsou and T. Komarek and K. Köneke and A. X. Y. Kong and T. Kono and N. Konstantinidis and P. Kontaxakis and B. Konya and R. Kopeliansky and S. Koperny and K. Korcyl and K. Kordas and A. Korn and S. Korn and I. Korolkov and N. Korotkova and B. Kortman and O. Kortner and S. Kortner and W. H. Kostecka and M. Kostov and V. V. Kostyukhin and A. Kotsokechagia and A. Kotwal and A. Koulouris and A. Kourkoumeli-Charalampidi and C. Kourkoumelis and E. Kourlitis and O. Kovanda and R. Kowalewski and W. Kozanecki and A. S. Kozhin and V. A. Kramarenko and G. Kramberger and P. Kramer and M. W. Krasny and A. Krasznahorkay and A. C. Kraus and J. W. Kraus and J. A. Kremer and N. B. Krengel and T. Kresse and L. Kretschmann and J. Kretzschmar and K. Kreul and P. Krieger and K. Krizka and K. Kroeninger and H. Kroha and J. Kroll and K. S. Krowpman and U. Kruchonak and H. Krüger and N. Krumnack and M. C. Kruse and O. Kuchinskaia and S. Kuday and S. Kuehn and R. Kuesters and T. Kuhl and V. Kukhtin and Y. Kulchitsky and S. Kuleshov and J. Kull and E. V. Kumar and M. Kumar and N. Kumari and P. Kumari and A. Kupco and T. Kupfer and A. Kupich and O. Kuprash and H. Kurashige and L. L. Kurchaninov and O. Kurdysh and Y. A. Kurochkin and A. Kurova and M. Kuze and A. K. Kvam and J. Kvita and N. G. Kyriacou and C. Lacasta and F. Lacava and H. Lacker and D. Lacour and N. N. Lad and E. Ladygin and A. Lafarge and B. Laforge and T. Lagouri and F. Z. Lahbabi and S. Lai and J. E. Lambert and S. Lammers and W. Lampl and C. Lampoudis and G. Lamprinoudis and A. N. Lancaster and E. Lançon and U. Landgraf and M. P. J. Landon and V. S. Lang and O. K. B. Langrekken and A. J. Lankford and F. Lanni and K. Lantzsch and A. Lanza and M. Lanzac Berrocal and J. F. Laporte and T. Lari and D. Larsen and L. Larson and F. Lasagni Manghi and M. Lassnig and S. D. Lawlor and R. Lazaridou and M. Lazzaroni and H. D. M. Le and E. M. Le Boulicaut and L. T. Le Pottier and B. Leban and F. Ledroit-Guillon and T. F. Lee and L. L. Leeuw and M. Lefebvre and C. Leggett and G. Lehmann Miotto and M. Leigh and W. A. Leight and W. Leinonen and A. Leisos and M. A. L. Leite and C. E. Leitgeb and R. Leitner and K. J. C. Leney and T. Lenz and S. Leone and C. Leonidopoulos and A. Leopold and J. H. Lepage Bourbonnais and R. Les and C. G. Lester and M. Levchenko and J. Levêque and L. J. Levinson and G. Levrini and M. P. Lewicki and C. Lewis and D. J. Lewis and L. Lewitt and A. Li and B. Li and C. Li and C-Q. Li and H. Li and J. Li and K. Li and L. Li and R. Li and S. Li and T. Li and X. Li and Z. Li and S. Liang and Z. Liang and M. Liberatore and B. Liberti and K. Lie and J. Lieber Marin and H. Lien and H. Lin and S. F. Lin and L. Linden and R. E. Lindley and J. H. Lindon and J. Ling and E. Lipeles and A. Lipniacka and A. Lister and J. D. Little and B. Liu and B. X. Liu and D. Liu and E. H. L. Liu and J. K. K. Liu and K. Liu and M. Liu and M. Y. Liu and P. Liu and Q. Liu and X. Liu and Y. Liu and Y. L. Liu and Y. W. Liu and Z. Liu and S. L. Lloyd and E. M. Lobodzinska and P. Loch and E. Lodhi and T. Lohse and K. Lohwasser and E. Loiacono and J. D. Lomas and J. D. Long and I. Longarini and R. Longo and A. Lopez Solis and N. A. Lopez-canelas and N. Lorenzo Martinez and A. M. Lory and M. Losada and G. Löschcke Centeno and X. Lou and A. Lounis and P. A. Love and M. Lu and S. Lu and Y. J. Lu and H. J. Lubatti and C. Luci and F. L. Lucio Alves and F. Luehring and B. S. Lunday and O. Lundberg and J. Lunde and N. A. Luongo and M. S. Lutz and A. B. Lux and D. Lynn and R. Lysak and V. Lysenko and E. Lytken and V. Lyubushkin and T. Lyubushkina and M. M. Lyukova and M. Firdaus M. Soberi and H. Ma and K. Ma and L. L. Ma and W. Ma and Y. Ma and J. C. MacDonald and P. C. Machado De Abreu Farias and R. Madar and T. Madula and J. Maeda and T. Maeno and P. T. Mafa and H. Maguire and V. Maiboroda and A. Maio and K. Maj and O. Majersky and S. Majewski and R. Makhmanazarov and N. Makovec and V. Maksimovic and B. Malaescu and J. Malamant and Pa. Malecki and V. P. Maleev and F. Malek and M. Mali and D. Malito and U. Mallik and A. Maloizel and S. Maltezos and A. Malvezzi Lopes and S. Malyukov and J. Mamuzic and G. Mancini and M. N. Mancini and G. Manco and J. P. Mandalia and S. S. Mandarry and I. Mandić and L. Manhaes de Andrade Filho and I. M. Maniatis and J. Manjarres Ramos and D. C. Mankad and A. Mann and T. Manoussos and M. N. Mantinan and S. Manzoni and L. Mao and X. Mapekula and A. Marantis and R. R. Marcelo Gregorio and G. Marchiori and M. Marcisovsky and C. Marcon and E. Maricic and M. Marinescu and S. Marium and M. Marjanovic and A. Markhoos and M. Markovitch and M. K. Maroun and G. T. Marsden and E. J. Marshall and Z. Marshall and S. Marti-Garcia and J. Martin and T. A. Martin and V. J. Martin and B. Martin dit Latour and L. Martinelli and M. Martinez and P. Martinez Agullo and V. I. Martinez Outschoorn and P. Martinez Suarez and S. Martin-Haugh and G. Martinovicova and V. S. Martoiu and A. C. Martyniuk and A. Marzin and D. Mascione and L. Masetti and J. Masik and A. L. Maslennikov and S. L. Mason and P. Massarotti and P. Mastrandrea and A. Mastroberardino and T. Masubuchi and T. T. Mathew and J. Matousek and D. M. Mattern and J. Maurer and T. Maurin and A. J. Maury and B. Maček and C. Mavungu Tsava and D. A. Maximov and A. E. May and E. Mayer and R. Mazini and I. Maznas and S. M. Mazza and E. Mazzeo and J. P. Mc Gowan and S. P. Mc Kee and C. A. Mc Lean and C. C. McCracken and E. F. McDonald and A. E. McDougall and L. F. Mcelhinney and J. A. Mcfayden and R. P. McGovern and R. P. Mckenzie and T. C. Mclachlan and D. J. Mclaughlin and S. J. McMahon and C. M. Mcpartland and R. A. McPherson and S. Mehlhase and A. Mehta and D. Melini and B. R. Mellado Garcia and A. H. Melo and F. Meloni and A. M. Mendes Jacques Da Costa and L. Meng and S. Menke and M. Mentink and E. Meoni and G. Mercado and S. Merianos and C. Merlassino and C. Meroni and J. Metcalfe and A. S. Mete and E. Meuser and C. Meyer and J-P. Meyer and Y. Miao and R. P. Middleton and M. Mihovilovic and L. Mijović and G. Mikenberg and M. Mikestikova and M. Mikuž and H. Mildner and A. Milic and D. W. Miller and E. H. Miller and L. S. Miller and A. Milov and D. A. Milstead and T. Min and A. A. Minaenko and I. A. Minashvili and A. I. Mincer and B. Mindur and M. Mineev and Y. Mino and L. M. Mir and M. Miralles Lopez and M. Mironova and M. C. Missio and A. Mitra and V. A. Mitsou and Y. Mitsumori and O. Miu and P. S. Miyagawa and T. Mkrtchyan and M. Mlinarevic and T. Mlinarevic and M. Mlynarikova and S. Mobius and M. H. Mohamed Farook and S. Mohapatra and S. Mohiuddin and G. Mokgatitswane and L. Moleri and U. Molinatti and L. G. Mollier and B. Mondal and S. Mondal and K. Mönig and E. Monnier and L. Monsonis Romero and J. Montejo Berlingen and A. Montella and M. Montella and F. Montereali and F. Monticelli and S. Monzani and A. Morancho Tarda and N. Morange and A. L. Moreira De Carvalho and M. Moreno Llácer and C. Moreno Martinez and J. M. Moreno Perez and P. Morettini and S. Morgenstern and M. Morii and M. Morinaga and M. Moritsu and F. Morodei and P. Moschovakos and B. Moser and M. Mosidze and T. Moskalets and P. Moskvitina and J. Moss and P. Moszkowicz and A. Moussa and Y. Moyal and H. Moyano Gomez and E. J. W. Moyse and O. Mtintsilana and S. Muanza and M. Mucha and J. Mueller and R. Müller and G. A. Mullier and A. J. Mullin and J. J. Mullin and A. C. Mullins and A. E. Mulski and D. P. Mungo and D. Munoz Perez and F. J. Munoz Sanchez and W. J. Murray and M. Muškinja and C. Mwewa and A. G. Myagkov and A. J. Myers and G. Myers and M. Myska and B. P. Nachman and K. Nagai and K. Nagano and R. Nagasaka and J. L. Nagle and E. Nagy and A. M. Nairz and Y. Nakahama and K. Nakamura and K. Nakkalil and A. Nandi and H. Nanjo and E. A. Narayanan and Y. Narukawa and I. Naryshkin and L. Nasella and S. Nasri and C. Nass and G. Navarro and J. Navarro-Gonzalez and A. Nayaz and P. Y. Nechaeva and S. Nechaeva and F. Nechansky and L. Nedic and T. J. Neep and A. Negri and M. Negrini and C. Nellist and C. Nelson and K. Nelson and S. Nemecek and M. Nessi and M. S. Neubauer and J. Newell and P. R. Newman and Y. W. Y. Ng and B. Ngair and H. D. N. Nguyen and J. D. Nichols and R. B. Nickerson and R. Nicolaidou and J. Nielsen and M. Niemeyer and J. Niermann and N. Nikiforou and V. Nikolaenko and I. Nikolic-Audit and P. Nilsson and I. Ninca and G. Ninio and A. Nisati and N. Nishu and R. Nisius and N. Nitika and J-E. Nitschke and E. K. Nkadimeng and T. Nobe and T. Nommensen and M. B. Norfolk and B. J. Norman and M. Noury and J. Novak and T. Novak and R. Novotny and L. Nozka and K. Ntekas and N. M. J. Nunes De Moura Junior and J. Ocariz and A. Ochi and I. Ochoa and S. Oerdek and J. T. Offermann and A. Ogrodnik and A. Oh and C. C. Ohm and H. Oide and M. L. Ojeda and Y. Okumura and L. F. Oleiro Seabra and I. Oleksiyuk and G. Oliveira Correa and D. Oliveira Damazio and J. L. Oliver and Ö. O. Öncel and A. P. O’Neill and A. Onofre and P. U. E. Onyisi and M. J. Oreglia and D. Orestano and R. Orlandini and R. S. Orr and L. M. Osojnak and Y. Osumi and G. Otero y Garzon and H. Otono and G. J. Ottino and M. Ouchrif and F. Ould-Saada and T. Ovsiannikova and M. Owen and R. E. Owen and V. E. Ozcan and F. Ozturk and N. Ozturk and S. Ozturk and H. A. Pacey and K. Pachal and A. Pacheco Pages and C. Padilla Aranda and G. Padovano and S. Pagan Griso and G. Palacino and A. Palazzo and J. Pampel and J. Pan and T. Pan and D. K. Panchal and C. E. Pandini and J. G. Panduro Vazquez and H. D. Pandya and H. Pang and P. Pani and G. Panizzo and L. Panwar and L. Paolozzi and S. Parajuli and A. Paramonov and C. Paraskevopoulos and D. Paredes Hernandez and A. Pareti and K. R. Park and T. H. Park and F. Parodi and J. A. Parsons and U. Parzefall and B. Pascual Dias and L. Pascual Dominguez and E. Pasqualucci and S. Passaggio and F. Pastore and P. Patel and U. M. Patel and J. R. Pater and T. Pauly and F. Pauwels and C. I. Pazos and M. Pedersen and R. Pedro and S. V. Peleganchuk and O. Penc and E. A. Pender and S. Peng and G. D. Penn and K. E. Penski and M. Penzin and B. S. Peralva and A. P. Pereira Peixoto and L. Pereira Sanchez and D. V. Perepelitsa and G. Perera and E. Perez Codina and M. Perganti and H. Pernegger and S. Perrella and O. Perrin and K. Peters and R. F. Y. Peters and B. A. Petersen and T. C. Petersen and E. Petit and V. Petousis and A. R. Petri and C. Petridou and T. Petru and A. Petrukhin and M. Pettee and A. Petukhov and K. Petukhova and R. Pezoa and L. Pezzotti and G. Pezzullo and L. Pfaffenbichler and A. J. Pfleger and T. M. Pham and T. Pham and P. W. Phillips and G. Piacquadio and E. Pianori and F. Piazza and R. Piegaia and D. Pietreanu and A. D. Pilkington and M. Pinamonti and J. L. Pinfold and B. C. Pinheiro Pereira and J. Pinol Bel and A. E. Pinto Pinoargote and L. Pintucci and K. M. Piper and A. Pirttikoski and D. A. Pizzi and L. Pizzimento and A. Plebani and M.-A. Pleier and V. Pleskot and E. Plotnikova and G. Poddar and R. Poettgen and L. Poggioli and S. Polacek and G. Polesello and A. Poley and A. Polini and C. S. Pollard and Z. B. Pollock and E. Pompa Pacchi and N. I. Pond and D. Ponomarenko and L. Pontecorvo and S. Popa and G. A. Popeneciu and A. Poreba and D. M. Portillo Quintero and S. Pospisil and M. A. Postill and P. Postolache and K. Potamianos and P. A. Potepa and I. N. Potrap and C. J. Potter and H. Potti and J. Poveda and M. E. Pozo Astigarraga and R. Pozzi and A. Prades Ibanez and J. Pretel and D. Price and M. Primavera and L. Primomo and M. A. Principe Martin and R. Privara and T. Procter and M. L. Proffitt and N. Proklova and K. Prokofiev and G. Proto and J. Proudfoot and M. Przybycien and W. W. Przygoda and A. Psallidas and J. E. Puddefoot and D. Pudzha and D. Pyatiizbyantseva and J. Qian and R. Qian and D. Qichen and Y. Qin and T. Qiu and A. Quadt and M. Queitsch-Maitland and G. Quetant and R. P. Quinn and G. Rabanal Bolanos and D. Rafanoharana and F. Raffaeli and F. Ragusa and J. L. Rainbolt and J. A. Raine and S. Rajagopalan and E. Ramakoti and L. Rambelli and I. A. Ramirez-Berend and K. Ran and D. S. Rankin and N. P. Rapheeha and H. Rasheed and D. F. Rassloff and A. Rastogi and S. Rave and S. Ravera and B. Ravina and I. Ravinovich and M. Raymond and A. L. Read and N. P. Readioff and D. M. Rebuzzi and A. S. Reed and K. Reeves and J. A. Reidelsturz and D. Reikher and A. Rej and C. Rembser and H. Ren and M. Renda and F. Renner and A. G. Rennie and A. L. Rescia and S. Resconi and M. Ressegotti and S. Rettie and W. F. Rettie and E. Reynolds and O. L. Rezanova and P. Reznicek and H. Riani and N. Ribaric and E. Ricci and R. Richter and S. Richter and E. Richter-Was and M. Ridel and S. Ridouani and P. Rieck and P. Riedler and E. M. Riefel and J. O. Rieger and M. Rijssenbeek and M. Rimoldi and L. Rinaldi and P. Rincke and G. Ripellino and I. Riu and J. C. Rivera Vergara and F. Rizatdinova and E. Rizvi and B. R. Roberts and S. S. Roberts and D. Robinson and M. Robles Manzano and A. Robson and A. Rocchi and C. Roda and S. Rodriguez Bosca and Y. Rodriguez Garcia and A. M. Rodríguez Vera and S. Roe and J. T. Roemer and O. Røhne and R. A. Rojas and C. P. A. Roland and A. Romaniouk and E. Romano and M. Romano and A. C. Romero Hernandez and N. Rompotis and L. Roos and S. Rosati and B. J. Rosser and E. Rossi and L. P. Rossi and L. Rossini and R. Rosten and M. Rotaru and B. Rottler and D. Rousseau and D. Rousso and S. Roy-Garand and A. Rozanov and Z. M. A. Rozario and Y. Rozen and A. Rubio Jimenez and V. H. Ruelas Rivera and T. A. Ruggeri and A. Ruggiero and A. Ruiz-Martinez and A. Rummler and Z. Rurikova and N. A. Rusakovich and H. L. Russell and G. Russo and J. P. Rutherfoord and S. Rutherford Colmenares and M. Rybar and P. Rybczynski and A. Ryzhov and J. A. Sabater Iglesias and H. F-W. Sadrozinski and F. Safai Tehrani and S. Saha and M. Sahinsoy and B. Sahoo and A. Saibel and B. T. Saifuddin and M. Saimpert and G. T. Saito and M. Saito and T. Saito and A. Sala and A. Salnikov and J. Salt and A. Salvador Salas and F. Salvatore and A. Salzburger and D. Sammel and E. Sampson and D. Sampsonidis and D. Sampsonidou and J. Sánchez and V. Sanchez Sebastian and H. Sandaker and C. O. Sander and J. A. Sandesara and M. Sandhoff and C. Sandoval and L. Sanfilippo and D. P. C. Sankey and T. Sano and A. Sansoni and L. Santi and C. Santoni and H. Santos and A. Santra and E. Sanzani and K. A. Saoucha and J. G. Saraiva and J. Sardain and O. Sasaki and K. Sato and C. Sauer and E. Sauvan and P. Savard and R. Sawada and C. Sawyer and L. Sawyer and C. Sbarra and A. Sbrizzi and T. Scanlon and J. Schaarschmidt and U. Schäfer and A. C. Schaffer and D. Schaile and R. D. Schamberger and C. Scharf and M. M. Schefer and V. A. Schegelsky and D. Scheirich and M. Schernau and C. Scheulen and C. Schiavi and M. Schioppa and B. Schlag and S. Schlenker and J. Schmeing and E. Schmidt and M. A. Schmidt and K. Schmieden and C. Schmitt and N. Schmitt and S. Schmitt and N. A. Schneider and L. Schoeffel and A. Schoening and P. G. Scholer and E. Schopf and M. Schott and S. Schramm and T. Schroer and H-C. Schultz-Coulon and M. Schumacher and B. A. Schumm and Ph. Schune and H. R. Schwartz and A. Schwartzman and T. A. Schwarz and Ph. Schwemling and R. Schwienhorst and F. G. Sciacca and A. Sciandra and G. Sciolla and F. Scuri and C. D. Sebastiani and K. Sedlaczek and S. C. Seidel and A. Seiden and B. D. Seidlitz and C. Seitz and J. M. Seixas and G. Sekhniaidze and L. Selem and N. Semprini-Cesari and A. Semushin and D. Sengupta and V. Senthilkumar and L. Serin and M. Sessa and H. Severini and F. Sforza and A. Sfyrla and Q. Sha and E. Shabalina and H. Shaddix and A. H. Shah and R. Shaheen and J. D. Shahinian and M. Shamim and L. Y. Shan and M. Shapiro and A. Sharma and A. S. Sharma and P. Sharma and P. B. Shatalov and K. Shaw and S. M. Shaw and Q. Shen and D. J. Sheppard and P. Sherwood and L. Shi and X. Shi and S. Shimizu and C. O. Shimmin and I. P. J. Shipsey and S. Shirabe and M. Shiyakova and M. J. Shochet and D. R. Shope and B. Shrestha and S. Shrestha and I. Shreyber and M. J. Shroff and P. Sicho and A. M. Sickles and E. Sideras Haddad and A. C. Sidley and A. Sidoti and F. Siegert and Dj. Sijacki and F. Sili and J. M. Silva and I. Silva Ferreira and M. V. Silva Oliveira and S. B. Silverstein and S. Simion and R. Simoniello and E. L. Simpson and H. Simpson and L. R. Simpson and S. Simsek and S. Sindhu and P. Sinervo and S. N. Singh and S. Singh and S. Sinha and M. Sioli and K. Sioulas and I. Siral and E. Sitnikova and J. Sjölin and A. Skaf and E. Skorda and P. Skubic and M. Slawinska and I. Slazyk and I. Sliusar and V. Smakhtin and B. H. Smart and S. Yu. Smirnov and Y. Smirnov and L. N. Smirnova and O. Smirnova and A. C. Smith and D. R. Smith and J. L. Smith and M. B. Smith and R. Smith and H. Smitmanns and M. Smizanska and K. Smolek and P. Smolyanskiy and A. A. Snesarev and H. L. Snoek and S. Snyder and R. Sobie and A. Soffer and C. A. Solans Sanchez and E. Yu. Soldatov and U. Soldevila and A. A. Solodkov and S. Solomon and A. Soloshenko and K. Solovieva and O. V. Solovyanov and P. Sommer and A. Sonay and A. Sopczak and A. L. Sopio and F. Sopkova and J. D. Sorenson and I. R. Sotarriva Alvarez and V. Sothilingam and O. J. Soto Sandoval and S. Sottocornola and R. Soualah and Z. Soumaimi and D. South and N. Soybelman and S. Spagnolo and M. Spalla and D. Sperlich and B. Spisso and D. P. Spiteri and L. Splendori and M. Spousta and E. J. Staats and R. Stamen and E. Stanecka and W. Stanek-Maslouska and M. V. Stange and B. Stanislaus and M. M. Stanitzki and B. Stapf and E. A. Starchenko and G. H. Stark and J. Stark and P. Staroba and P. Starovoitov and R. Staszewski and G. Stavropoulos and A. Stefl and P. Steinberg and B. Stelzer and H. J. Stelzer and O. Stelzer-Chilton and H. Stenzel and T. J. Stevenson and G. A. Stewart and J. R. Stewart and M. C. Stockton and G. Stoicea and M. Stolarski and S. Stonjek and A. Straessner and J. Strandberg and S. Strandberg and M. Stratmann and M. Strauss and T. Strebler and P. Strizenec and R. Ströhmer and D. M. Strom and R. Stroynowski and A. Strubig and S. A. Stucci and B. Stugu and J. Stupak and N. A. Styles and D. Su and S. Su and X. Su and D. Suchy and K. Sugizaki and V. V. Sulin and M. J. Sullivan and D. M. S. Sultan and L. Sultanaliyeva and S. Sultansoy and S. Sun and W. Sun and O. Sunneborn Gudnadottir and N. Sur and M. R. Sutton and H. Suzuki and M. Svatos and P. N. Swallow and M. Swiatlowski and T. Swirski and A. Swoboda and I. Sykora and M. Sykora and T. Sykora and D. Ta and K. Tackmann and A. Taffard and R. Tafirout and Y. Takubo and M. Talby and A. A. Talyshev and K. C. Tam and N. M. Tamir and A. Tanaka and J. Tanaka and R. Tanaka and M. Tanasini and Z. Tao and S. Tapia Araya and S. Tapprogge and A. Tarek Abouelfadl Mohamed and S. Tarem and K. Tariq and G. Tarna and G. F. Tartarelli and M. J. Tartarin and P. Tas and M. Tasevsky and E. Tassi and A. C. Tate and G. Tateno and Y. Tayalati and G. N. Taylor and W. Taylor and A. S. Tegetmeier and P. Teixeira-Dias and J. J. Teoh and K. Terashi and J. Terron and S. Terzo and M. Testa and R. J. Teuscher and A. Thaler and O. Theiner and T. Theveneaux-Pelzer and D. W. Thomas and J. P. Thomas and E. A. Thompson and P. D. Thompson and E. Thomson and R. E. Thornberry and C. Tian and Y. Tian and V. Tikhomirov and Yu. A. Tikhonov and S. Timoshenko and D. Timoshyn and E. X. L. Ting and P. Tipton and A. Tishelman-Charny and K. Todome and S. Todorova-Nova and S. Todt and L. Toffolin and M. Togawa and J. Tojo and S. Tokár and O. Toldaiev and G. Tolkachev and M. Tomoto and L. Tompkins and E. Torrence and H. Torres and E. Torró Pastor and M. Toscani and C. Tosciri and M. Tost and D. R. Tovey and T. Trefzger and P. M. Tricarico and A. Tricoli and I. M. Trigger and S. Trincaz-Duvoid and D. A. Trischuk and A. Tropina and L. Truong and M. Trzebinski and A. Trzupek and F. Tsai and M. Tsai and A. Tsiamis and P. V. Tsiareshka and S. Tsigaridas and A. Tsirigotis and V. Tsiskaridze and E. G. Tskhadadze and M. Tsopoulou and Y. Tsujikawa and I. I. Tsukerman and V. Tsulaia and S. Tsuno and K. Tsuri and D. Tsybychev and Y. Tu and A. Tudorache and V. Tudorache and S. B. Tuncay and S. Turchikhin and I. Turk Cakir and R. Turra and T. Turtuvshin and P. M. Tuts and S. Tzamarias and E. Tzovara and Y. Uematsu and F. Ukegawa and P. A. Ulloa Poblete and E. N. Umaka and G. Unal and A. Undrus and G. Unel and J. Urban and P. Urrejola and G. Usai and R. Ushioda and M. Usman and F. Ustuner and Z. Uysal and V. Vacek and B. Vachon and T. Vafeiadis and A. Vaitkus and C. Valderanis and E. Valdes Santurio and M. Valente and S. Valentinetti and A. Valero and E. Valiente Moreno and A. Vallier and J. A. Valls Ferrer and D. R. Van Arneman and T. R. Van Daalen and A. Van Der Graaf and H. Z. Van Der Schyf and P. Van Gemmeren and M. Van Rijnbach and S. Van Stroud and I. Van Vulpen and P. Vana and M. Vanadia and U. M. Vande Voorde and W. Vandelli and E. R. Vandewall and D. Vannicola and L. Vannoli and R. Vari and M. Varma and E. W. Varnes and C. Varni and D. Varouchas and L. Varriale and K. E. Varvell and M. E. Vasile and L. Vaslin and M. D. Vassilev and A. Vasyukov and L. M. Vaughan and R. Vavricka and T. Vazquez Schroeder and J. Veatch and V. Vecchio and M. J. Veen and I. Veliscek and I. Velkovska and L. M. Veloce and F. Veloso and S. Veneziano and A. Ventura and S. Ventura Gonzalez and A. Verbytskyi and M. Verducci and C. Vergis and M. Verissimo De Araujo and W. Verkerke and J. C. Vermeulen and C. Vernieri and M. Vessella and M. C. Vetterli and A. Vgenopoulos and N. Viaux Maira and T. Vickey and O. E. Vickey Boeriu and G. H. A. Viehhauser and L. Vigani and M. Vigl and M. Villa and M. Villaplana Perez and E. M. Villhauer and E. Vilucchi and M. Vincent and M. G. Vincter and A. Visibile and C. Vittori and I. Vivarelli and E. Voevodina and F. Vogel and J. C. Voigt and P. Vokac and Yu. Volkotrub and E. Von Toerne and B. Vormwald and K. Vorobev and M. Vos and K. Voss and M. Vozak and L. Vozdecky and N. Vranjes and M. Vranjes Milosavljevic and M. Vreeswijk and N. K. Vu and R. Vuillermet and O. Vujinovic and I. Vukotic and I. K. Vyas and J. F. Wack and S. Wada and C. Wagner and J. M. Wagner and W. Wagner and S. Wahdan and H. Wahlberg and C. H. Waits and J. Walder and R. Walker and K. Walkingshaw Pass and W. Walkowiak and A. Wall and E. J. Wallin and T. Wamorkar and A. Wang and A. Z. Wang and C. Wang and H. Wang and J. Wang and P. Wang and R. Wang and S. M. Wang and S. Wang and T. Wang and W. T. Wang and W. Wang and X. Wang and Y. Wang and Z. Wang and C. Wanotayaroj and A. Warburton and A. L. Warnerbring and N. Warrack and S. Waterhouse and A. T. Watson and H. Watson and M. F. Watson and E. Watton and G. Watts and B. M. Waugh and J. M. Webb and C. Weber and H. A. Weber and M. S. Weber and S. M. Weber and C. Wei and Y. Wei and A. R. Weidberg and E. J. Weik and J. Weingarten and C. Weiser and C. J. Wells and T. Wenaus and B. Wendland and T. Wengler and N. S. Wenke and N. Wermes and M. Wessels and A. M. Wharton and A. S. White and A. White and M. J. White and D. Whiteson and L. Wickremasinghe and W. Wiedenmann and M. Wielers and R. Wierda and C. Wiglesworth and H. G. Wilkens and J. J. H. Wilkinson and D. M. Williams and H. H. Williams and S. Williams and S. Willocq and B. J. Wilson and D. J. Wilson and P. J. Windischhofer and F. I. Winkel and F. Winklmeier and B. T. Winter and M. Wittgen and M. Wobisch and T. Wojtkowski and Z. Wolffs and J. Wollrath and M. W. Wolter and H. Wolters and M. C. Wong and E. L. Woodward and S. D. Worm and B. K. Wosiek and K. W. Woźniak and S. Wozniewski and K. Wraight and C. Wu and J. Wu and M. Wu and S. L. Wu and S. Wu and X. Wu and Y. Wu and Z. Wu and J. Wuerzinger and T. R. Wyatt and B. M. Wynne and S. Xella and L. Xia and M. Xia and M. Xie and A. Xiong and J. Xiong and D. Xu and H. Xu and L. Xu and R. Xu and T. Xu and Y. Xu and Z. Xu and B. Yabsley and S. Yacoob and Y. Yamaguchi and E. Yamashita and H. Yamauchi and T. Yamazaki and Y. Yamazaki and S. Yan and Z. Yan and H. J. Yang and H. T. Yang and S. Yang and T. Yang and X. Yang and Y. Yang and W-M. Yao and C. L. Yardley and J. Ye and S. Ye and X. Ye and Y. Yeh and I. Yeletskikh and B. Yeo and M. R. Yexley and T. P. Yildirim and P. Yin and K. Yorita and C. J. S. Young and C. Young and N. D. Young and Y. Yu and J. Yuan and M. Yuan and R. Yuan and L. Yue and M. Zaazoua and B. Zabinski and I. Zahir and A. Zaio and Z. K. Zak and T. Zakareishvili and S. Zambito and J. A. Zamora Saa and J. Zang and R. Zanzottera and O. Zaplatilek and C. Zeitnitz and H. Zeng and J. C. Zeng and D. T. Zenger, Jr and O. Zenin and T. Ženiš and S. Zenz and D. Zerwas and M. Zhai and D. F. Zhang and G. Zhang and J. Zhang and K. Zhang and L. Zhang and P. Zhang and R. Zhang and S. Zhang and T. Zhang and Y. Zhang and Z. Zhang and H. Zhao and T. Zhao and Y. Zhao and Z. Zhao and A. Zhemchugov and J. Zheng and K. Zheng and X. Zheng and Z. Zheng and D. Zhong and B. Zhou and H. Zhou and N. Zhou and Y. Zhou and C. G. Zhu and J. Zhu and X. Zhu and Y. Zhu and X. Zhuang and K. Zhukov and N. I. Zimine and J. Zinsser and M. Ziolkowski and L. Živković and A. Zoccoli and K. Zoch and A. Zografos and T. G. Zorbas and O. Zormpa and L. Zwalinski}, doi = {10.1103/bpln-ccql}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111802}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for longitudinally polarized w bosons in the electroweak production of same-sign w boson pairs in association with two jets in pp collisions at s=13 TeV with the ATLAS detector}, volume = {135}, year = {2025}, }
• (2025). Superradiant neutrino lasers from radioactive condensates. PRL, 135(11), 111801. (www)

  @article{ , abstract = {Superradiance emerges from collective spontaneous emission in optically pumped gases, and is characterized by photon emission enhancements of up to in an atom system. The gain mechanism derives from correlations developed within the decay medium rather than from stimulated emission as in lasing, so an analog of this process should be possible for fermionic final states. We introduce here the concept of superradiant neutrino emission from a radioactive Bose Einstein condensate, which can form the basis for a superradiant neutrino laser. A plausible experimental realization based on a condensate of electron-capture isotope could exhibit effective radioactive decay rates accelerated from 86.2 days to minutes in viably sized rubidium condensates of atoms.}, archive = {J_PRL}, author = {B. J. P. Jones and J. A. Formaggio}, doi = {10.1103/l3c1-yg2l}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111801}, shortjournal = {Phys. Rev. Lett.}, title = {Superradiant neutrino lasers from radioactive condensates}, volume = {135}, year = {2025}, }
• (2025). GW250114: Testing hawking’s area law and the kerr nature of black holes. PRL, 135(11), 111403. (www)

  @article{ , abstract = {The gravitational-wave signal GW250114 was observed by the two LIGO detectors with a network matched-filter signal-to-noise ratio of 80. The signal was emitted by the coalescence of two black holes with near-equal masses and , and small spins (90% credibility) and negligible eccentricity . Postmerger data excluding the peak region are consistent with the dominant quadrupolar mode of a Kerr black hole and its first overtone. We constrain the modes’ frequencies to of the Kerr spectrum, providing a test of the remnant’s Kerr nature. We also examine Hawking’s area law, also known as the second law of black hole mechanics, which states that the total area of the black hole event horizons cannot decrease with time. A range of analyses that exclude up to five of the strongest merger cycles confirm that the remnant area is larger than the sum of the initial areas to high credibility.}, archive = {J_PRL}, author = {LIGO Scientific, Virgo, and KAGRA Collaborations and A. G. Abac and I. Abouelfettouh and F. Acernese and K. Ackley and C. Adamcewicz and S. Adhicary and D. Adhikari and N. Adhikari and R. X. Adhikari and V. K. Adkins and S. Afroz and A. Agapito and D. Agarwal and M. Agathos and N. Aggarwal and S. Aggarwal and O. D. Aguiar and I.-L. Ahrend and L. Aiello and A. Ain and P. Ajith and T. Akutsu and S. Al-Kershi and S. Al-Shammari and S. Albanesi and W. Ali and C. Alléné and A. Allocca and P. A. Altin and S. Alvarez-Lopez and W. Amar and O. Amarasinghe and A. Amato and F. Amicucci and C. Amra and A. Ananyeva and S. B. Anderson and W. G. Anderson and M. Andia and M. Ando and M. Andrés-Carcasona and T. Andrić and J. Anglin and S. Ansoldi and J. M. Antelis and S. Antier and M. Aoumi and E. Z. Appavuravther and S. Appert and S. K. Apple and K. Arai and A. Araya and M. C. Araya and M. Arca Sedda and J. S. Areeda and N. Aritomi and F. Armato and S. Armstrong and N. Arnaud and M. Arogeti and S. M. Aronson and G. Ashton and Y. Aso and L. Asprea and M. Assiduo and S. Assis de Souza Melo and S. M. Aston and P. Astone and F. Attadio and F. Aubin and K. AultONeal and G. Avallone and E. A. Avila and S. Babak and C. Badger and S. Bae and S. Bagnasco and L. Baiotti and R. Bajpai and T. Baka and A. M. Baker and K. A. Baker and T. Baker and G. Baldi and N. Baldicchi and M. Ball and G. Ballardin and S. W. Ballmer and S. Banagiri and B. Banerjee and D. Bankar and T. M. Baptiste and P. Baral and M. Baratti and J. C. Barayoga and B. C. Barish and D. Barker and N. Barman and P. Barneo and F. Barone and B. Barr and L. Barsotti and M. Barsuglia and D. Barta and A. M. Bartoletti and M. A. Barton and I. Bartos and A. Basalaev and R. Bassiri and A. Basti and M. Bawaj and P. Baxi and J. C. Bayley and A. C. Baylor and P. A. Baynard, II and M. Bazzan and V. M. Bedakihale and F. Beirnaert and M. Bejger and D. Belardinelli and A. S. Bell and D. S. Bellie and L. Bellizzi and W. Benoit and I. Bentara and J. D. Bentley and M. Ben Yaala and S. Bera and F. Bergamin and B. K. Berger and S. Bernuzzi and M. Beroiz and C. P. L. Berry and D. Bersanetti and T. Bertheas and A. Bertolini and J. Betzwieser and D. Beveridge and G. Bevilacqua and N. Bevins and S. Bhagwat and R. Bhandare and R. Bhatt and D. Bhattacharjee and S. Bhattacharyya and S. Bhaumik and V. Biancalana and A. Bianchi and I. A. Bilenko and G. Billingsley and A. Binetti and S. Bini and C. Binu and S. Biot and O. Birnholtz and S. Biscoveanu and A. Bisht and M. Bitossi and M.-A. Bizouard and S. Blaber and J. K. Blackburn and L. A. Blagg and C. D. Blair and D. G. Blair and N. Bode and N. Boettner and G. Boileau and M. Boldrini and G. N. Bolingbroke and A. Bolliand and L. D. Bonavena and R. Bondarescu and F. Bondu and E. Bonilla and M. S. Bonilla and A. Bonino and R. Bonnand and A. Borchers and S. Borhanian and V. Boschi and S. Bose and V. Bossilkov and Y. Bothra and A. Boudon and L. Bourg and M. Boyle and A. Bozzi and C. Bradaschia and P. R. Brady and A. Branch and M. Branchesi and I. Braun and T. Briant and A. Brillet and M. Brinkmann and P. Brockill and E. Brockmueller and A. F. Brooks and B. C. Brown and D. D. Brown and M. L. Brozzetti and S. Brunett and G. Bruno and R. Bruntz and J. Bryant and Y. Bu and F. Bucci and J. Buchanan and O. Bulashenko and T. Bulik and H. J. Bulten and A. Buonanno and K. Burtnyk and R. Buscicchio and D. Buskulic and J. Calderón Bustillo and C. Buy and R. L. Byer and V. Cáceres-Barbosa and G. S. Cabourn Davies and R. Cabrita and L. Cadonati and G. Cagnoli and C. Cahillane and A. Calafat and T. A. Callister and E. Calloni and S. R. Callos and M. Canepa and G. Caneva Santoro and K. C. Cannon and H. Cao and L. A. Capistran and E. Capocasa and E. Capote and G. Capurri and G. Carapella and F. Carbognani and M. Carlassara and J. B. Carlin and T. K. Carlson and M. F. Carney and M. Carpinelli and G. Carrillo and J. J. Carter and G. Carullo and A. Casallas-Lagos and J. Casanueva Diaz and C. Casentini and S. Y. Castro-Lucas and S. Caudill and M. Cavaglià and R. Cavalieri and A. Ceja and G. Cella and P. Cerdá-Durán and E. Cesarini and N. Chabbra and W. Chaibi and A. Chakraborty and P. Chakraborty and S. Chakraborty and S. Chalathadka Subrahmanya and J. C. L. Chan and M. Chan and K. Chang and S. Chao and P. Charlton and E. Chassande-Mottin and C. Chatterjee and Debarati Chatterjee and Deep Chatterjee and M. Chaturvedi and S. Chaty and K. Chatziioannou and A. Chen and A. H.-Y. Chen and D. Chen and H. Chen and H. Y. Chen and S. Chen and Yanbei Chen and Yitian Chen and H. P. Cheng and P. Chessa and H. T. Cheung and S. Y. Cheung and F. Chiadini and D. Chiaramello and G. Chiarini and A. Chiba and A. Chincarini and M. L. Chiofalo and A. Chiummo and C. Chou and S. Choudhary and N. Christensen and S. S. Y. Chua and G. Ciani and M. Cieślar and P. Ciecielag and M. Cifaldi and B. Cirok and F. Clara and J. A. Clark and T. A. Clarke and P. Clearwater and S. Clesse and F. Cleva and E. Coccia and E. Codazzo and P.-F. Cohadon and S. Colace and E. Colangeli and M. Colleoni and C. G. Collette and J. Collins and S. Colloms and A. Colombo and C. M. Compton and G. Connolly and L. Conti and T. R. Corbitt and I. Cordero-Carrión and S. Corezzi and N. J. Cornish and I. Coronado and A. Corsi and R. Cottingham and M. W. Coughlin and A. Couineaux and P. Couvares and D. M. Coward and R. Coyne and A. Cozzumbo and J. D. E. Creighton and T. D. Creighton and P. Cremonese and S. Crook and R. Crouch and J. Csizmazia and J. R. Cudell and T. J. Cullen and A. Cumming and E. Cuoco and M. Cusinato and B. D’Angelo and S. D’Antonio and L. D’Onofrio and D. D’Urso and G. Dálya and M. C. Díaz and T. Dal Canton and S. Dal Pra and T. Damour and S. Danilishin and K. Danzmann and K. E. Darroch and L. P. Dartez and R. Das and A. Dasgupta and V. Dattilo and A. Daumas and N. Davari and I. Dave and A. Davenport and M. Davier and T. F. Davies and D. Davis and L. Davis and M. C. Davis and P. Davis and E. J. Daw and M. Dax and L. V. Da Conceição and M. Deenadayalan and J. Degallaix and S. Della Torre and W. Del Pozzo and A. Demagny and G. Demasi and N. Demos and T. Dent and A. Depasse and N. DePergola and M. Desai and R. DeSalvo and A. DeSimone and J. De Bolle and M. De Laurentis and F. De Lillo and F. De Marco and F. De Matteis and R. De Pietri and R. De Rosa and C. De Rossi and R. De Simone and A. Dhani and R. Diab and G. Dideron and T. Dietrich and D. Diksha and J. Ding and M. Di Cesare and L. Di Fiore and C. Di Fronzo and M. Di Giovanni and T. Di Girolamo and S. Di Pace and I. Di Palma and D. Di Piero and Divyajyoti and F. Di Renzo and A. Dmitriev and J. P. Docherty and Z. Doctor and N. Doerksen and E. Dohmen and A. Doke and A. Domiciano De Souza and F. Donovan and K. L. Dooley and T. Dooney and S. Doravari and O. Dorosh and W. J. D. Doyle and M. Drago and J. C. Driggers and L. Dunn and U. Dupletsa and P. Dutta Roy and H. Duval and P.-A. Duverne and S. E. Dwyer and C. Eassa and M. Ebersold and T. Eckhardt and G. Eddolls and A. Effler and J. Eichholz and H. Einsle and M. Eisenmann and M. Emma and K. Endo and R. Enficiaud and L. Errico and R. Espinosa and M. Esposito and R. C. Essick and H. Estellés and T. Etzel and M. Evans and T. Evstafyeva and B. E. Ewing and J. M. Ezquiaga and F. Fabrizi and V. Fafone and S. Fairhurst and A. M. Farah and B. Farr and W. M. Farr and G. Favaro and M. Favata and M. Fays and M. Fazio and J. Feicht and M. M. Fejer and R. Felicetti and E. Fenyvesi and J. Fernandes and T. Fernandes and D. Fernando and S. Ferraiuolo and T. A. Ferreira and F. Fidecaro and P. Figura and E. Finch and A. Fiori and I. Fiori and M. Fishbach and R. P. Fisher and R. Fittipaldi and V. Fiumara and R. Flaminio and S. M. Fleischer and L. S. Fleming and E. Floden and H. Fong and J. A. Font and F. Fontinele-Nunes and C. Foo and B. Fornal and K. Franceschetti and F. Frappez and S. Frasca and F. Frasconi and J. P. Freed and Z. Frei and A. Freise and O. Freitas and R. Frey and W. Frischhertz and P. Fritschel and V. V. Frolov and G. G. Fronzé and M. Fuentes-Garcia and S. Fujii and T. Fujimori and P. Fulda and M. Fyffe and B. Gadre and J. R. Gair and S. Galaudage and V. Galdi and R. Gamba and A. Gamboa and S. Gamoji and D. Ganapathy and A. Ganguly and B. Garaventa and J. García-Bellido and C. García-Quirós and J. W. Gardner and K. A. Gardner and S. Garg and J. Gargiulo and X. Garrido and A. Garron and F. Garufi and P. A. Garver and C. Gasbarra and B. Gateley and F. Gautier and V. Gayathri and T. Gayer and G. Gemme and A. Gennai and V. Gennari and J. George and R. George and O. Gerberding and Archisman Ghosh and L. Gergely and Sayantan Ghosh and Shaon Ghosh and Shrobana Ghosh and Suprovo Ghosh and Tathagata Ghosh and J. A. Giaime and K. D. Giardina and D. R. Gibson and C. Gier and S. Gkaitatzis and J. Glanzer and F. Glotin and J. Godfrey and R. V. Godley and P. Godwin and A. S. Goettel and E. Goetz and J. Golomb and S. Gomez Lopez and B. Goncharov and G. González and P. Goodarzi and S. Goode and A. W. Goodwin-Jones and M. Gosselin and R. Gouaty and D. W. Gould and K. Govorkova and A. Grado and V. Graham and A. E. Granados and M. Granata and V. Granata and S. Gras and P. Grassia and J. Graves and C. Gray and R. Gray and G. Greco and A. C. Green and L. Green and S. M. Green and S. R. Green and C. Greenberg and A. M. Gretarsson and H. K. Griffin and D. Griffith and H. L. Griggs and G. Grignani and C. Grimaud and H. Grote and S. Grunewald and D. Guerra and D. Guetta and G. M. Guidi and A. R. Guimaraes and H. K. Gulati and F. Gulminelli and Anuradha Gupta and H. Guo and W. Guo and Y. Guo and I. Gupta and N. C. Gupta and S. K. Gupta and V. Gupta and N. Gupte and J. Gurs and N. Gutierrez and N. Guttman and F. Guzman and D. Haba and M. Haberland and S. Haino and E. D. Hall and E. Z. Hamilton and G. Hammond and M. Haney and J. Hanks and C. Hanna and M. D. Hannam and O. A. Hannuksela and A. G. Hanselman and H. Hansen and J. Hanson and S. Hanumasagar and R. Harada and A. R. Hardison and S. Harikumar and K. Haris and I. Harley-Trochimczyk and T. Harmark and J. Harms and G. M. Harry and I. W. Harry and J. Hart and B. Haskell and C. J. Haster and K. Haughian and H. Hayakawa and K. Hayama and M. C. Heintze and J. Heinze and J. Heinzel and H. Heitmann and F. Hellman and A. F. Helmling-Cornell and G. Hemming and O. Henderson-Sapir and M. Hendry and I. S. Heng and M. H. Hennig and C. Henshaw and M. Heurs and A. L. Hewitt and J. Heynen and J. Heyns and S. Higginbotham and S. Hild and S. Hill and Y. Himemoto and N. Hirata and C. Hirose and D. Hofman and B. E. Hogan and N. A. Holland and I. J. Hollows and D. E. Holz and L. Honet and D. J. Horton-Bailey and J. Hough and S. Hourihane and N. T. Howard and E. J. Howell and C. G. Hoy and C. A. Hrishikesh and P. Hsi and H.-F. Hsieh and H.-Y. Hsieh and C. Hsiung and S.-H. Hsu and W.-F. Hsu and Q. Hu and H. Y. Huang and Y. Huang and Y. T. Huang and A. D. Huddart and B. Hughey and V. Hui and S. Husa and R. Huxford and L. Iampieri and G. A. Iandolo and M. Ianni and G. Iannone and J. Iascau and K. Ide and R. Iden and A. Ierardi and S. Ikeda and H. Imafuku and Y. Inoue and G. Iorio and P. Iosif and M. H. Iqbal and J. Irwin and R. Ishikawa and M. Isi and K. S. Isleif and Y. Itoh and M. Iwaya and B. R. Iyer and C. Jacquet and P.-E. Jacquet and T. Jacquot and S. J. Jadhav and S. P. Jadhav and M. Jain and T. Jain and A. L. James and K. Jani and J. Janquart and N. N. Janthalur and S. Jaraba and P. Jaranowski and R. Jaume and W. Javed and A. Jennings and M. Jensen and W. Jia and J. Jiang and H.-B. Jin and G. R. Johns and N. A. Johnson and M. C. Johnston and R. Johnston and N. Johny and D. H. Jones and D. I. Jones and R. Jones and H. E. Jose and P. Joshi and S. K. Joshi and G. Joubert and J. Ju and L. Ju and K. Jung and J. Junker and V. Juste and H. B. Kabagoz and T. Kajita and I. Kaku and V. Kalogera and M. Kalomenopoulos and M. Kamiizumi and N. Kanda and S. Kandhasamy and G. Kang and N. C. Kannachel and J. B. Kanner and S. A. KantiMahanty and S. J. Kapadia and D. P. Kapasi and M. Karthikeyan and M. Kasprzack and H. Kato and T. Kato and E. Katsavounidis and W. Katzman and R. Kaushik and K. Kawabe and R. Kawamoto and D. Keitel and L. J. Kemperman and J. Kennington and F. A. Kerkow and R. Kesharwani and J. S. Key and R. Khadela and S. Khadka and S. S. Khadkikar and F. Y. Khalili and F. Khan and T. Khanam and M. Khursheed and N. M. Khusid and W. Kiendrebeogo and N. Kijbunchoo and C. Kim and J. C. Kim and K. Kim and M. H. Kim and S. Kim and Y.-M. Kim and C. Kimball and K. Kimes and M. Kinnear and J. S. Kissel and S. Klimenko and A. M. Knee and E. J. Knox and N. Knust and K. Kobayashi and S. M. Koehlenbeck and G. Koekoek and K. Kohri and K. Kokeyama and S. Koley and P. Kolitsidou and A. E. Koloniari and K. Komori and A. K. H. Kong and A. Kontos and L. M. Koponen and M. Korobko and X. Kou and A. Koushik and N. Kouvatsos and M. Kovalam and T. Koyama and D. B. Kozak and A. Królak and S. L. Kranzhoff and V. Kringel and N. V. Krishnendu and S. Kroker and K. Kruska and J. Kubisz and G. Kuehn and S. Kulkarni and A. Kulur Ramamohan and Achal Kumar and Anil Kumar and Praveen Kumar and Prayush Kumar and Rahul Kumar and Rakesh Kumar and J. Kume and K. Kuns and N. Kuntimaddi and S. Kuroyanagi and S. Kuwahara and K. Kwak and K. Kwan and S. Kwon and H. Lück and G. Lacaille and D. Laghi and A. H. Laity and E. Lalande and M. Lalleman and P. C. Lalremruati and M. Landry and B. B. Lane and R. N. Lang and J. Lange and R. Langgin and B. Lantz and J. Larsen and A. Lartaux-Vollard and P. D. Lasky and J. Lawrence and M. Laxen and C. Lazarte and A. Lazzarini and C. Lazzaro and I. La Rosa and P. Leaci and L. Leali and Y. K. Lecoeuche and H. M. Lee and H. W. Lee and J. Lee and K. Lee and R.-K. Lee and R. Lee and Sungho Lee and Sunjae Lee and Y. Lee and I. N. Legred and J. Lehmann and L. Lehner and A. Lemaître and M. Lenti and M. Leonardi and M. Lequime and N. Leroy and M. Lesovsky and N. Letendre and M. Lethuillier and Y. Levin and K. Leyde and M. Le Jean and A. K. Y. Li and K. L. Li and T. G. F. Li and X. Li and Y. Li and Z. Li and A. Lihos and E. T. Lin and F. Lin and L. C.-C. Lin and Y.-C. Lin and C. Lindsay and S. D. Linker and A. Liu and G. C. Liu and Jian Liu and F. Llamas Villarreal and J. Llobera-Querol and R. K. L. Lo and J.-P. Locquet and S. C. G. Loggins and M. R. Loizou and L. T. London and A. Longo and D. Lopez and M. Lopez Portilla and M. Lorenzini and A. Lorenzo-Medina and V. Loriette and M. Lormand and G. Losurdo and E. Lotti and T. P. Lott, IV and J. D. Lough and H. A. Loughlin and C. O. Lousto and N. Low and N. Lu and L. Lucchesi and D. Lumaca and A. P. Lundgren and A. W. Lussier and J. R. Mérou and R. Macas and M. MacInnis and D. M. Macleod and I. A. O. MacMillan and A. Macquet and K. Maeda and S. Maenaut and S. S. Magare and R. M. Magee and E. Maggio and R. Maggiore and M. Magnozzi and M. Mahesh and M. Maini and S. Majhi and E. Majorana and C. N. Makarem and N. Malagon and D. Malakar and J. A. Malaquias-Reis and U. Mali and S. Maliakal and A. Malik and L. Mallick and A.-K. Malz and N. Man and M. Mancarella and V. Mandic and V. Mangano and N. Manning and B. Mannix and G. L. Mansell and M. Manske and M. Mantovani and M. Mapelli and C. Marinelli and F. Marion and A. S. Markosyan and A. Markowitz and E. Maros and S. Marsat and F. Martelli and I. W. Martin and R. M. Martin and B. B. Martinez and D. A. Martinez and M. Martinez and V. Martinez and A. Martini and J. C. Martins and D. V. Martynov and E. J. Marx and L. Massaro and A. Masserot and M. Masso-Reid and S. Mastrogiovanni and T. Matcovich and M. Matiushechkina and L. Maurin and N. Mavalvala and N. Maxwell and G. McCarrol and R. McCarthy and D. E. McClelland and S. McCormick and L. McCuller and S. McEachin and C. McElhenny and G. I. McGhee and J. McGinn and K. B. M. McGowan and J. McIver and A. McLeod and I. McMahon and T. McRae and R. McTeague and D. Meacher and B. N. Meagher and R. Mechum and Q. Meijer and A. Melatos and C. S. Menoni and F. Mera and R. A. Mercer and L. Mereni and K. Merfeld and E. L. Merilh and J. D. Merritt and M. Merzougui and C. Messick and B. Mestichelli and M. Meyer-Conde and F. Meylahn and A. Mhaske and A. Miani and H. Miao and C. Michel and Y. Michimura and H. Middleton and D. P. Mihaylov and S. J. Miller and M. Millhouse and E. Milotti and V. Milotti and Y. Minenkov and E. M. Minihan and Ll. M. Mir and L. Mirasola and M. Miravet-Tenés and C.-A. Miritescu and A. Mishra and C. Mishra and T. Mishra and A. L. Mitchell and J. G. Mitchell and K. Mitman and S. Mitra and V. P. Mitrofanov and K. Mitsuhashi and R. Mittleman and O. Miyakawa and S. Miyoki and A. Miyoko and G. Mo and L. Mobilia and S. R. P. Mohapatra and S. R. Mohite and M. Molina-Ruiz and M. Mondin and M. Montani and C. J. Moore and D. Moraru and A. More and S. More and C. Moreno and E. A. Moreno and G. Moreno and A. Moreso Serra and S. Morisaki and Y. Moriwaki and G. Morras and A. Moscatello and M. Mould and B. Mours and C. M. Mow-Lowry and L. Muccillo and F. Muciaccia and D. Mukherjee and Samanwaya Mukherjee and Soma Mukherjee and Subroto Mukherjee and Suvodip Mukherjee and N. Mukund and A. Mullavey and H. Mullock and J. Mundi and C. L. Mungioli and M. Murakoshi and P. G. Murray and D. Nabari and S. L. Nadji and A. Nagar and N. Nagarajan and K. Nakagaki and K. Nakamura and H. Nakano and M. Nakano and D. Nanadoumgar-Lacroze and D. Nandi and V. Napolano and P. Narayan and I. Nardecchia and T. Narikawa and H. Narola and L. Naticchioni and R. K. Nayak and L. Negri and A. Nela and C. Nelle and A. Nelson and T. J. N. Nelson and M. Nery and A. Neunzert and S. Ng and L. Nguyen Quynh and S. A. Nichols and A. B. Nielsen and Y. Nishino and A. Nishizawa and S. Nissanke and W. Niu and F. Nocera and J. Noller and M. Norman and C. North and J. Novak and R. Nowicki and J. F. Nuño Siles and L. K. Nuttall and J. O’Dell and T. O’Hanlon and B. O’Neal and B. O’Reilly and R. O’Shaughnessy and S. O’Shea and K. Obayashi and J. Oberling and E. Oelker and M. Oertel and G. Oganesyan and M. Ohashi and F. Ohme and R. Oliveri and R. Omer and M. Onishi and K. Oohara and M. Orselli and S. Oshino and C. Osthelder and I. Ota and D. J. Ottaway and A. Ouzriat and H. Overmier and B. J. Owen and R. Ozaki and M. Pürrer and M. Pálfi and C. Périgois and A. E. Pace and R. Pagano and M. A. Page and A. Pai and L. Paiella and A. Pal and S. Pal and M. A. Palaia and P. P. Palma and C. Palomba and P. Palud and H. Pan and J. Pan and K. C. Pan and P. K. Panda and Shiksha Pandey and Swadha Pandey and P. T. H. Pang and F. Pannarale and K. A. Pannone and B. C. Pant and F. H. Panther and M. Panzeri and F. Paoletti and A. Paolone and A. Papadopoulos and E. E. Papalexakis and L. Papalini and G. Papigkiotis and A. Paquis and A. Parisi and B.-J. Park and J. Park and W. Parker and G. Pascale and D. Pascucci and A. Pasqualetti and R. Passaquieti and L. Passenger and D. Passuello and O. Patane and A. V. Patel and D. Pathak and A. Patra and B. Patricelli and B. G. Patterson and K. Paul and S. Paul and E. Payne and F. E. Peña Arellano and T. Pearce and M. Pedraza and A. Pele and X. Peng and Y. Peng and S. Penn and M. D. Penuliar and A. Perego and Z. Pereira and G. Perna and A. Perreca and J. Perret and S. Perriès and J. W. Perry and D. Pesios and S. Peters and S. Petracca and C. Petrillo and H. P. Pfeiffer and H. Pham and K. A. Pham and K. S. Phukon and H. Phurailatpam and M. Piarulli and L. Piccari and O. J. Piccinni and M. Pichot and M. Piendibene and F. Piergiovanni and L. Pierini and G. Pierra and V. Pierro and M. Pietrzak and M. Pillas and F. Pilo and L. Pinard and I. M. Pinto and M. Pinto and B. J. Piotrzkowski and M. Pirello and M. D. Pitkin and A. Placidi and E. Placidi and M. L. Planas and W. Plastino and C. Plunkett and R. Poggiani and E. Polini and J. Pomper and L. Pompili and J. Poon and E. Porcelli and E. K. Porter and C. Posnansky and R. Poulton and J. Powell and G. S. Prabhu and M. Pracchia and B. K. Pradhan and T. Pradier and A. K. Prajapati and V. Prasad and K. Prasai and R. Prasanna and P. Prasia and G. Pratten and G. Principe and G. A. Prodi and P. Prosperi and P. Prosposito and A. C. Providence and A. Puecher and J. Pullin and P. Puppo and H. Qi and J. Qin and G. Quéméner and V. Quetschke and P. J. Quinonez and N. Qutob and R. Rading and I. Rainho and S. Raja and C. Rajan and B. Rajbhandari and K. E. Ramirez and F. A. Ramis Vidal and A. Ramos-Buades and M. Ramos Arevalo and S. Ranjan and K. Ransom and P. Rapagnani and B. Ratto and A. Ravichandran and A. Ray and V. Raymond and M. Razzano and J. Read and T. Regimbau and S. Reid and C. Reissel and D. H. Reitze and A. Renzini and B. Revenu and A. Revilla Peña and R. Reyes and L. Ricca and F. Ricci and M. Ricci and A. Ricciardone and J. Rice and J. W. Richardson and M. L. Richardson and A. Rijal and K. Riles and H. K. Riley and S. Rinaldi and J. Rittmeyer and C. Robertson and F. Robinet and M. Robinson and A. Rocchi and L. Rolland and J. G. Rollins and A. E. Romano and R. Romano and A. Romero and I. M. Romero-Shaw and J. H. Romie and S. Ronchini and T. J. Roocke and L. Rosa and T. J. Rosauer and C. A. Rose and D. Rosińska and M. P. Ross and M. Rossello-Sastre and S. Rowan and S. K. Roy and S. Roy and D. Rozza and P. Ruggi and N. Ruhama and K. Ruiz-Rocha and E. Ruiz Morales and E. M. Sänger and S. Sachdev and T. Sadecki and P. Saffarieh and S. Safi-Harb and M. R. Sah and S. Saha and T. Sainrat and S. Sajith Menon and K. Sakai and Y. Sakai and M. Sakellariadou and S. Sakon and O. S. Salafia and F. Salces-Carcoba and L. Salconi and M. Saleem and F. Salemi and M. Sallé and S. U. Salunkhe and S. Salvador and A. Salvarese and A. Samajdar and A. Sanchez and E. J. Sanchez and L. E. Sanchez and N. Sanchis-Gual and J. R. Sanders and F. Santoliquido and F. Sarandrea and T. R. Saravanan and N. Sarin and P. Sarkar and A. Sasli and P. Sassi and B. Sassolas and B. S. Sathyaprakash and R. Sato and S. Sato and Yukino Sato and Yu Sato and O. Sauter and R. L. Savage and T. Sawada and H. L. Sawant and S. Sayah and V. Scacco and D. Schaetzl and M. Scheel and A. Schiebelbein and M. G. Schiworski and P. Schmidt and S. Schmidt and R. Schnabel and M. Schneewind and R. M. S. Schofield and K. Schouteden and B. W. Schulte and B. F. Schutz and E. Schwartz and M. Scialpi and J. Scott and S. M. Scott and R. M. Sedas and T. C. Seetharamu and M. Seglar-Arroyo and Y. Sekiguchi and D. Sellers and N. Sembo and A. S. Sengupta and E. G. Seo and J. W. Seo and V. Sequino and M. Serra and A. Sevrin and T. Shaffer and U. S. Shah and M. A. Shaikh and L. Shao and A. K. Sharma and Preeti Sharma and Prianka Sharma and Ritwik Sharma and S. Sharma Chaudhary and P. Shawhan and N. S. Shcheblanov and E. Sheridan and Z.-H. Shi and M. Shikauchi and R. Shimomura and H. Shinkai and S. Shirke and D. H. Shoemaker and D. M. Shoemaker and R. W. Short and S. ShyamSundar and A. Sider and H. Siegel and D. Sigg and L. Silenzi and L. Silvestri and M. Simmonds and Amitesh Singh and Anika Singh and L. P. Singer and D. Singh and N. Singh and S. Singh and A. M. Sintes and V. Sipala and V. Skliris and B. J. J. Slagmolen and D. A. Slater and T. J. Slaven-Blair and J. Smetana and J. R. Smith and L. Smith and R. J. E. Smith and W. J. Smith and M. Soares-Santos and S. Soares de Albuquerque Filho and K. Somiya and I. Song and S. Soni and V. Sordini and F. Sorrentino and H. Sotani and F. Spada and V. Spagnuolo and A. P. Spencer and P. Spinicelli and A. K. Srivastava and F. Stachurski and C. J. Stark and D. A. Steer and N. Steinle and J. Steinlechner and S. Steinlechner and N. Stergioulas and P. Stevens and S. Stevenson and M. StPierre and M. D. Strong and A. Strunk and A. L. Stuver and M. Suchenek and S. Sudhagar and Y. Sudo and N. Sueltmann and L. Suleiman and K. D. Sullivan and J. Sun and L. Sun and S. Sunil and J. Suresh and B. J. Sutton and P. J. Sutton and K. Suzuki and M. Suzuki and B. L. Swinkels and A. Syx and M. J. Szczepańczyk and P. Szewczyk and M. Tacca and H. Tagoshi and K. Takada and H. Takahashi and R. Takahashi and A. Takamori and S. Takano and H. Takeda and K. Takeshita and I. Takimoto Schmiegelow and M. Takou-Ayaoh and C. Talbot and M. Tamaki and N. Tamanini and D. Tanabe and K. Tanaka and S. J. Tanaka and S. Tanioka and D. B. Tanner and W. Tanner and L. Tao and R. D. Tapia and E. N. Tapia San Martín and C. Taranto and A. Taruya and J. D. Tasson and J. G. Tau and D. Tellez and R. Tenorio and S. A. Teukolsky and H. Themann and A. Theodoropoulos and M. P. Thirugnanasambandam and L. M. Thomas and M. Thomas and P. Thomas and J. E. Thompson and S. R. Thondapu and K. A. Thorne and K. S. Thorne and E. Thrane and J. Tissino and A. Tiwari and Pawan Tiwari and Praveer Tiwari and S. Tiwari and V. Tiwari and M. R. Todd and M. Toffano and A. M. Toivonen and K. Toland and A. E. Tolley and T. Tomaru and V. Tommasini and T. Tomura and H. Tong and C. Tong-Yu and A. Torres-Forné and C. I. Torrie and I. Tosta e Melo and E. Tournefier and M. Trad Nery and K. Tran and A. Trapananti and R. Travaglini and F. Travasso and G. Traylor and M. Trevor and M. C. Tringali and A. Tripathee and G. Troian and A. Trovato and L. Trozzo and R. J. Trudeau and T. Tsang and S. Tsuchida and L. Tsukada and K. Turbang and M. Turconi and C. Turski and H. Ubach and N. Uchikata and T. Uchiyama and R. P. Udall and T. Uehara and K. Ueno and V. Undheim and L. E. Uronen and T. Ushiba and M. Vacatello and H. Vahlbruch and N. Vaidya and G. Vajente and A. Vajpeyi and J. Valencia and M. Valentini and S. A. Vallejo-Peña and S. Vallero and V. Valsan and K. Vandra and M. VanDyke and J. Vanier and M. VanKeuren and J. Vanosky and M. van Dael and E. Van den Bossche and J. F. J. van den Brand and C. Van Den Broeck and M. van der Sluys and A. Van de Walle and J. van Dongen and H. van Haevermaet and J. V. van Heijningen and P. Van Hove and N. van Remortel and M. Vardaro and A. F. Vargas and V. Varma and A. N. Vazquez and A. Vecchio and G. Vedovato and J. Veitch and P. J. Veitch and S. Venikoudis and R. C. Venterea and P. Verdier and M. Vereecken and D. Verkindt and B. Verma and Y. Verma and S. M. Vermeulen and F. Vetrano and A. Veutro and A. Viceré and S. Vidyant and A. D. Viets and A. Vijaykumar and A. Vilkha and V. Villa-Ortega and N. Villanueva Espinosa and E. T. Vincent and J.-Y. Vinet and S. Viret and S. Vitale and H. Vocca and D. Voigt and E. R. G. von Reis and J. S. A. von Wrangel and W. E. Vossius and L. Vujeva and S. P. Vyatchanin and J. Wack and L. E. Wade and M. Wade and K. J. Wagner and R. M. Wald and L. Wallace and E. J. Wang and H. Wang and J. Z. Wang and W. H. Wang and Y. F. Wang and G. Waratkar and J. Warner and M. Was and T. Washimi and N. Y. Washington and D. Watarai and B. Weaver and S. A. Webster and N. L. Weickhardt and M. Weinert and A. J. Weinstein and R. Weiss and L. Wen and K. Wette and J. T. Whelan and B. F. Whiting and C. Whittle and E. G. Wickens and D. Wilken and A. T. Wilkin and B. M. Williams and D. Williams and M. J. Williams and N. S. Williams and J. L. Willis and B. Willke and M. Wils and L. Wilson and C. W. Winborn and J. Winterflood and C. C. Wipf and G. Woan and J. Woehler and N. E. Wolfe and H. T. Wong and I. C. F. Wong and K. Wong and T. Wouters and J. L. Wright and M. Wright and B. Wu and C. Wu and D. S. Wu and H. Wu and K. Wu and Q. Wu and Y. Wu and Z. Wu and E. Wuchner and D. M. Wysocki and V. A. Xu and Y. Xu and N. Yadav and H. Yamamoto and K. Yamamoto and T. S. Yamamoto and T. Yamamoto and R. Yamazaki and T. Yan and K. Z. Yang and Y. Yang and Z. Yarbrough and J. Yebana and S.-W. Yeh and A. B. Yelikar and X. Yin and J. Yokoyama and T. Yokozawa and S. Yuan and H. Yuzurihara and M. Zanolin and M. Zeeshan and T. Zelenova and J.-P. Zendri and M. Zeoli and M. Zerrad and M. Zevin and L. Zhang and N. Zhang and R. Zhang and T. Zhang and C. Zhao and Yue Zhao and Yuhang Zhao and Z.-C. Zhao and Y. Zheng and H. Zhong and H. Zhou and H. O. Zhu and Z.-H. Zhu and A. B. Zimmerman and L. Zimmermann and M. E. Zucker and J. Zweizig}, doi = {10.1103/kw5g-d732}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111403}, shortjournal = {Phys. Rev. Lett.}, title = {GW250114: Testing hawking’s area law and the kerr nature of black holes}, volume = {135}, year = {2025}, }
• (2025). Probing the nature of dark matter using strongly lensed gravitational waves from binary black holes. PRL, 135(11), 111402. (www)

  @article{ , abstract = {Next-generation ground-based gravitational-wave (GW) detectors are expected to detect millions of binary black hole mergers during their operation period. A small fraction ( ∼ 0.1 – 1 % ) of them will be strongly lensed by intervening galaxies and clusters, producing multiple copies of the GW signals. The expected number of lensed events and the distribution of the time delay between lensed images will depend on the mass distribution of the lenses at different redshifts. Warm dark matter and fuzzy dark matter models predict lower abundances of low-mass dark matter halos as compared to the standard cold dark matter. This will result in a reduction in the number of strongly lensed GW events, especially with small time delays. Using the number of lensed events and the lensing time delay distribution, we will be able to put a lower bound on the mass of the warm and fuzzy dark matter particles from a catalog of lensed GW events. Our first forecasts suggest that the expected bounds from GW strong lensing from next-generation detectors are better than the current constraints.}, archive = {J_PRL}, author = {Souvik Jana and Shasvath J. Kapadia and Tejaswi Venumadhav and Surhud More and Parameswaran Ajith}, doi = {10.1103/7q31-3qwz}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111402}, shortjournal = {Phys. Rev. Lett.}, title = {Probing the nature of dark matter using strongly lensed gravitational waves from binary black holes}, volume = {135}, year = {2025}, }
• (2025). Two-step procedure to detect cosmological gravitational wave backgrounds with next-generation terrestrial gravitational-wave detectors. PRL, 135(11), 111401. (www)

  @article{ , abstract = {Cosmological gravitational-wave backgrounds are an exciting science target for next-generation ground-based detectors, as they encode invaluable information about the primordial Universe. However, any such background is expected to be obscured by the astrophysical foreground from compact-binary coalescences. We propose a novel framework to detect a cosmological gravitational-wave background in the presence of binary black holes and binary neutron star signals with next-generation ground-based detectors, including Cosmic Explorer and the Einstein Telescope. Our procedure involves first removing all the individually resolved binary black hole signals by notching them out in the time-frequency domain. Then, we perform joint Bayesian inference on the individually resolved binary neutron star signals, the unresolved binary neutron star foreground, and the cosmological background. For a flat cosmological background, we find that we can claim detection at level when , where is the observation time (in years), which is within a factor of from the sensitivity reached in the absence of these astrophysical foregrounds.}, archive = {J_PRL}, author = {Haowen Zhong and Luca Reali and Bei Zhou and Emanuele Berti and Vuk Mandic}, doi = {10.1103/j9jg-4drj}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111401}, shortjournal = {Phys. Rev. Lett.}, title = {Two-step procedure to detect cosmological gravitational wave backgrounds with next-generation terrestrial gravitational-wave detectors}, volume = {135}, year = {2025}, }
• (2025). Systematic analysis of parity-violating modes. PRL, 135(11), 111003. (www)

  @article{ , abstract = {Recent reports of cosmological parity violation in the four-point correlation function (4PCF) raise the question of how such violations could be systematically generated. Here we present a constructive procedure to generate arbitrary violations of vectorial and tensorial types on any scale, which is computationally efficient in the squeezed limit. We directly compute their numerical transfer function and find strong conservation in the linear regime. This procedure spans all squeezed parity-violating observables at the 4PCF following the quadratic estimator classification.}, archive = {J_PRL}, author = {Hong-Ming Zhu (朱弘明 and Ue-Li Pen (彭威禮}, doi = {10.1103/8s52-x3r2}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111003}, shortjournal = {Phys. Rev. Lett.}, title = {Systematic analysis of parity-violating modes}, volume = {135}, year = {2025}, }
• (2025). Could we observe an exploding black hole in the near future?. PRL, 135(11), 111002. (www)

  @article{ , abstract = {Observation of gamma rays from an exploding black hole would provide strong evidence for primordial black holes, the first direct evidence of Hawking radiation, and definitive information on the particles present in nature. However, indirect constraints suggest that direct observation of an exploding Schwarzschild black hole at current or upcoming gamma ray observatories is implausible. We introduce a dark-QED toy model consisting of a dark photon and a heavy dark electron. In this scenario a population of light primordial black holes charged under the dark symmetry can become quasiextremal, so they survive much longer than if they were uncharged, before discharging and exhibiting a Schwarzschild-like final explosion. We show that the answer is “yes,” in this scenario the probability of observing an exploding black hole over the next 10 years could potentially be over 90%.}, archive = {J_PRL}, author = {Michael J. Baker and Joaquim Iguaz Juan and Aidan Symons and Andrea Thamm}, doi = {10.1103/nwgd-g3zl}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111002}, shortjournal = {Phys. Rev. Lett.}, title = {Could we observe an exploding black hole in the near future?}, volume = {135}, year = {2025}, }
• (2025). Resonant axion-plasmon conversion in neutron star magnetospheres. PRL, 135(11), 111001. (www)

  @article{ , abstract = {Resonant axion-plasmon conversion in the magnetospheres of magnetars may substantially impact the landscape of dark-matter axion detection. This Letter explores how resonant axion-plasmon conversion modify the expected radio signals from axion-photon conversions observed on Earth. Critically, the resonant conversion radius lies within the region expected for axion-photon conversion, introducing a nonradiative power loss that diminishes the anticipated photon flux. Our analysis demonstrates that this effect can reduce radio telescope sensitivities, shifting them into regions excluded by previous experiments. These findings compel a reassessment of experimental constraints derived from radio signatures of axion-photon conversions and highlight the necessity of accounting for plasmon effects in astrophysical axion searches. The presented corrections provide critical insights for refining the detection strategies of future telescope-based dark matter axion experiments.}, archive = {J_PRL}, author = {H. Terças and J. T. Mendonça and R. Bingham}, doi = {10.1103/5hbb-yy48}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {111001}, shortjournal = {Phys. Rev. Lett.}, title = {Resonant axion-plasmon conversion in neutron star magnetospheres}, volume = {135}, year = {2025}, }
• (2025). Optimal moment-based characterization of a gaussian state. PRL, 135(11), 110805. (www)

  @article{ , abstract = {Fast and precise characterization of Gaussian states is crucial for their effective use in quantum technologies. In this work, we apply a multiparameter moment-based estimation method that enables rapid and accurate determination of squeezing, antisqueezing, and the squeezing angle of the squeezed vacuum state. Compared to conventional approaches, our method achieves faster parameter estimation with reduced uncertainty, reaching the Cramér-Rao bound. We validate its effectiveness using the two most common measurement schemes in continuous-variable quantum optics: homodyne detection and double homodyne detection. This rapid estimation framework is well suited for dynamically characterizing sources with time-dependent parameters, potentially enabling real-time feedback stabilization.}, archive = {J_PRL}, author = {Niels Tripier-Mondancin and Ilya Karuseichyk and Mattia Walschaers and Valentina Parigi and Nicolas Treps}, doi = {10.1103/1kln-n48s}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110805}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal moment-based characterization of a gaussian state}, volume = {135}, year = {2025}, }
• (2025). Approaching the multiparameter quantum cramér-rao bound via classical correlation and entangling measurements. PRL, 135(11), 110804. (www)

  @article{ , abstract = {Multiparameter quantum metrology is essential for a wide range of practical applications. However, simultaneously achieving the ultimate precision for all parameters, as prescribed by the quantum Cramér-Rao bound (QCRB), remains a significant challenge. In this work, we propose a scheme termed local operation with entangling measurements (LOEM) strategy, which leverages classically correlated orthogonal pure states combined with entangling measurements to attain the multiparameter QCRB. We experimentally validate this scheme using a quantum photonic system. Additionally, we employ iterative interactions to demonstrate that the LOEM strategy can achieve the precision of Heisenberg scaling. By theoretically and experimentally demonstrating the saturation of the multiparameter QCRB with the LOEM strategy, our work advances the practical applications of quantum metrology in multiparameter estimation.}, archive = {J_PRL}, author = {Minghao Mi and Ben Wang and Lijian Zhang}, doi = {10.1103/37kb-qq6k}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110804}, shortjournal = {Phys. Rev. Lett.}, title = {Approaching the multiparameter quantum cramér-rao bound via classical correlation and entangling measurements}, volume = {135}, year = {2025}, }
• (2025). Topological phase transitions in a constrained two-qubit quantum control landscape. PRL, 135(11), 110803. (www)

  @article{ , abstract = {In optimal quantum control, control landscape phase transitions (CLPTs) indicate sharp changes occurring in the set of optimal protocols, as a physical model parameter is varied. Here, we demonstrate the existence of a new class of CLPTs, associated with changes in the topological properties of the optimal level set in a two-qubit state-preparation problem. In particular, the distance distribution of control protocols sampled through stochastic homotopic dynamics reveals discontinuous changes in the number of connected components in the optimal level set, as a function of the protocol duration. We demonstrate how topological CLPTs can be detected in modern-day experiments.}, archive = {J_PRL}, author = {Nicolò Beato and Pranay Patil and Marin Bukov}, doi = {10.1103/dqvj-p6fq}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110803}, shortjournal = {Phys. Rev. Lett.}, title = {Topological phase transitions in a constrained two-qubit quantum control landscape}, volume = {135}, year = {2025}, }
• (2025). Entangling two rydberg superatoms via single-photon interference. PRL, 135(11), 110802. (www)

  @article{ , abstract = {Remote entanglement of matter qubits plays an important role in quantum networks and quantum repeater. Collective excitations generated via Rydberg blockade in an atomic ensemble—known as Rydberg superatoms—are promising candidates due to collectively enhanced atom-photon coupling and Rydberg-enabled nonlinearity. Here, we experimentally realize remote entanglement between two Rydberg superatoms via single-photon interference. The two setups are separated by 3 m and linked with two 20-m fibers, operated with independent control lasers. We verify that the entanglement generated is free from high-order excitation noise that is a key drawback in the traditional Duan-Lukin-Cirac-Zoller scheme. This Letter paves the way for entangling long-distance separated Rydberg superatoms at a high rate, as the success probability of a single-photon-based entangling scheme scales with the square root of the channel transmittance.}, archive = {J_PRL}, author = {Chao-Wei Yang and Jun Li and Peng-Fei Sun and Zi-Ye An and Xiao-Hui Bao and Jian-Wei Pan}, doi = {10.1103/zqkr-8991}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110802}, shortjournal = {Phys. Rev. Lett.}, title = {Entangling two rydberg superatoms via single-photon interference}, volume = {135}, year = {2025}, }
• (2025). Covariant quantum error-correcting codes with metrological entanglement advantage. PRL, 135(11), 110801. (www)

  @article{ , abstract = {We show that a subset of the basis for the irreducible representations of a tensor-product SU(2) rotation forms a covariant approximate quantum error-correcting code with transversal U(1) logical gates. Generalizing previous work on “thermodynamic codes” to general local spin and different irreducible representations using only properties of the angular momentum algebra, we obtain bounds on the code inaccuracy under generic noise on any known sites, under independent and identically distributed noise, and under heralded -local erasures. We demonstrate that this family of codes protects a probe state with quantum Fisher information surpassing the standard quantum limit when the sensing parameter couples to the generator of the U(1) logical gate.}, archive = {J_PRL}, author = {Cheng-Ju Lin and Zi-Wen Liu and Victor V. Albert and Alexey V. Gorshkov}, doi = {10.1103/dttc-ksdn}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110801}, shortjournal = {Phys. Rev. Lett.}, title = {Covariant quantum error-correcting codes with metrological entanglement advantage}, volume = {135}, year = {2025}, }
• (2025). Strain-enhanced spin readout contrast in silicon carbide membranes. PRL, 135(11), 110601. (www)

  @article{ , abstract = {Quantum defects in solids have emerged as a transformative platform for advancing quantum technologies. A key requirement for these applications is achieving high-fidelity single-spin readout, particularly at room temperature for quantum biosensing. Here, we demonstrate through ab initio simulations of a primary quantum defect in 4H silicon carbide that strain is an effective control parameter for significantly enhancing readout contrast. We validate this principle experimentally by inducing local strain in silicon carbide-on-insulator membranes, achieving a readout contrast exceeding 60% while preserving the favorable coherence properties of single spins. Our findings establish strain engineering as a powerful strategy for optimizing coherent spin-photon interfaces in PL6 divacancy centers within silicon carbide membranes and potentially other similar defect systems.}, archive = {J_PRL}, author = {Haibo Hu and Guodong Bian and Ailun Yi and Chunhui Jiang and Junhua Tan and Qi Luo and Bo Liang and Zhengtong Liu and Xinfang Nie and Dawei Lu and Shumin Xiao and Xin Ou and Ádám Gali and Yu Zhou and Qinghai Song}, doi = {10.1103/tdb3-tqfv}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110601}, shortjournal = {Phys. Rev. Lett.}, title = {Strain-enhanced spin readout contrast in silicon carbide membranes}, volume = {135}, year = {2025}, }
• (2025). Quantum dissipative continuous time crystals. PRL, 135(11), 110404. (www)

  @article{ , abstract = {Continuous time crystals, i.e., nonequilibrium phases with a spontaneously broken continuous time-translational symmetry, have been studied and recently observed in the long time dynamics of open quantum systems. Here, we investigate a lattice of interacting three-level particles and find two distinct time-crystal phases that cannot be described within mean-field theory. Remarkably, one of them emerges only in the presence of correlations, upon accounting for beyond-mean-field effects. Our findings extend explorations of continuous time-translational symmetry breaking in dissipative systems beyond the classical phenomenology of periodic orbits in a low-dimensional nonlinear system. The proposed model applies directly to the laser-driven dynamics of interacting Rydberg states in neutral-atom arrays and suggests that the predicted time-crystal phases are observable in such experiments.}, archive = {J_PRL}, author = {Felix Russo and Thomas Pohl}, doi = {10.1103/dc2s-94gv}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110404}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum dissipative continuous time crystals}, volume = {135}, year = {2025}, }
• (2025). Quantum information perspective on many-body dispersive forces. PRL, 135(11), 110403. (www)

  @article{ , abstract = {Despite its ubiquity, the quantum many-body properties of dispersion remain poorly understood. Here, we investigate the entanglement distribution in assemblies of quantum Drude oscillators, minimal models for dispersion-bound systems. We establish an analytic relationship between entanglement and correlation energy and show how entanglement monogamy determines whether many-body corrections to the pair potential are attractive, repulsive, or zero. These findings, demonstrated in trimers and extended lattices, apply in more general chemical environments where dispersion coexists with other cohesive forces.}, archive = {J_PRL}, author = {Christopher Willby and Martin Kiffner and Joseph Tindall and Jason Crain and Dieter Jaksch}, doi = {10.1103/f7yf-mxd5}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110403}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum information perspective on many-body dispersive forces}, volume = {135}, year = {2025}, }
• (2025). Quantum thermodynamic advantage in work extraction from steerable quantum correlations. PRL, 135(11), 110402. (www)

  @article{ , abstract = {Inspired by the primary goal of quantum thermodynamics—to characterize quantum signatures and leverage their benefits in thermodynamic scenarios—we design a work extraction task within a bipartite framework that exhibits a quantum thermodynamic advantage. The steerability of quantum correlations between the two parties is the key resource enabling such an advantage. In designing the task, we exploit the correspondence between steerability and the incompatibility of observables. Our work extraction protocol involves mutually unbiased bases, which exhibit maximum incompatibility and therefore maximum steerability, showcased in maximally entangled quantum states. The work extraction protocols consist of quenches and thermalization processes, which serve as fundamental building blocks for various thermodynamic protocols, such as heat engines. We derive upper bounds on the extractable work for unsteerable and steerable correlations and devise a protocol that saturates the latter. The ratio between the extractable work in steerable and unsteerable scenarios, which encapsulates the quantum advantage, increases with the dimension of the underlying system (sometimes referred to as an unbounded advantage). This proves a quantum thermodynamic advantage arising from steerable quantum correlations.}, archive = {J_PRL}, author = {Tanmoy Biswas and Chandan Datta and Luis Pedro García-Pintos}, doi = {10.1103/9qcc-7lq5}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110402}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum thermodynamic advantage in work extraction from steerable quantum correlations}, volume = {135}, year = {2025}, }
• (2025). Prethermal time-crystalline corner modes. PRL, 135(11), 110401. (www)

  @article{ , abstract = {We demonstrate the existence of prethermal discrete time crystals whose subharmonic response is entirely localized to zero-dimensional corner modes. Within the exponentially long prethermal regime, we show that the robustness of these corner modes arises from two related, yet distinct, mechanisms: the presence of a higher-order symmetry-protected topological phase in the effective Hamiltonian, or the emergence of a dynamical constraint that prevents the decay of the corner mode. While the first mechanism ensures the stability of the subharmonic response throughout the entirety of the prethermal regime, it is restricted to initial states in the ground state manifold of the effective Hamiltonian. By contrast, the second mechanism enables the observation of the prethermal time-crystalline order for arbitrary initial states , albeit with a timescale that is not only determined by the frequency of the drive, but also the relative energy scale across the system’s sublattices. We characterize these two mechanisms by simulating the dynamics of a periodically driven two-dimensional spin model, and discuss natural extensions of our model to all other dimensions.}, archive = {J_PRL}, author = {Si Jiang and Dong Yuan and Wenjie Jiang and Dong-Ling Deng and Francisco Machado}, doi = {10.1103/np9w-jsf9}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110401}, shortjournal = {Phys. Rev. Lett.}, title = {Prethermal time-crystalline corner modes}, volume = {135}, year = {2025}, }
• (2025). Experimental observation of genuine triplewise monogamy of contextuality correlations. PRL, 135(11), 110202. (www)

  @article{ , abstract = {Contextuality is a pivotal nonclassical phenomenon that challenges traditional interpretations of nature based on noncontextual realistic theories and serves as a valuable resource for quantum information. In this Letter, we explore the relationship of jointly tested contextuality correlations within the Cabello-Severini-Winter framework, with a particular emphasis on the concept of genuine triplewise monogamy. We propose and experimentally test a novel scenario involving three jointly tested contextuality correlations constrained by a genuine triplewise monogamy relation. Remarkably, our experimental design reveals the existence of triplewise monogamy without explicitly implementing it. Furthermore, our experimental results demonstrate that any two of the three correlations can exhibit contextuality simultaneously, thereby confirming, for the first time, the genuine feature of the triplewise monogamy. This phenomenon constitutes a nontrivial extension of monogamy relations to multiple correlations. These findings deepen our theoretical understanding and enhance our experimental capabilities in probing the intricate interplay of contextuality correlations, paving the way for future advancements in quantum information science.}, archive = {J_PRL}, author = {Xiang Zhan and Bingzi Huo and Dengke Qu and Peng Xue}, doi = {10.1103/b3xm-hcsl}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110202}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental observation of genuine triplewise monogamy of contextuality correlations}, volume = {135}, year = {2025}, }
• (2025). Information and majorization theory for fermionic phase-space distributions. PRL, 135(11), 110201. (www)

  @article{ , abstract = {We put forward several information-theoretic measures for analyzing the uncertainty of fermionic phase-space distributions using the theory of supernumbers. In contrast to the bosonic case, the anticommuting nature of Grassmann variables allows us to provide simple expressions for the Glauber , Wigner , and Husimi distributions of the arbitrary state of a single fermionic mode. It appears that all physical states are Gaussian and, thus, can be described by positive or negative thermal distributions (over Grassmann variables). We then prove several fermionic uncertainty relations, including notably the fermionic analogs of the (yet unproven) phase-space majorization and Wigner entropy conjectures for a bosonic mode, as well as the Lieb-Solovej theorem and the Wehrl-Lieb inequality. Our central point is that, although fermionic phase-space distributions are Grassmann-valued and do not have a straightforward interpretation, the corresponding uncertainty measures are expressed as Berezin integrals, which take on real values and are physically relevant.}, archive = {J_PRL}, author = {Nicolas J. Cerf and Tobias Haas}, doi = {10.1103/3qg7-r4mq}, journal = {Physical Review Letters}, month = {9}, number = {11}, pages = {110201}, shortjournal = {Phys. Rev. Lett.}, title = {Information and majorization theory for fermionic phase-space distributions}, volume = {135}, year = {2025}, }
• (2025). Erratum: Giant splitting of the hydrogen rotational eigenenergies in the c2 filled ice [Phys. rev. lett. 133, 236101 (2024)]. PRL, 135(10), 109902. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 109902 (2025)}, archive = {J_PRL}, author = {Simone Di Cataldo and Maria Rescigno and Lorenzo Monacelli and Umbertoluca Ranieri and Richard Gaal and Stefan Klotz and Jacques Ollivier and Michael Marek Koza and Cristiano De Michele and Livia Eleonora Bove}, doi = {10.1103/srpf-rp6z}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {109902}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Giant splitting of the hydrogen rotational eigenenergies in the c2 filled ice [Phys. rev. lett. 133, 236101 (2024)]}, volume = {135}, year = {2025}, }
• (2025). Erratum: Quantum state smoothing for linear gaussian systems [Phys. rev. lett. 122, 190402 (2019)]. PRL, 135(10), 109901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 109901 (2025)}, archive = {J_PRL}, author = {Kiarn T. Laverick and Areeya Chantasri and Howard M. Wiseman}, doi = {10.1103/gwxb-4pnq}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {109901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Quantum state smoothing for linear gaussian systems [Phys. rev. lett. 122, 190402 (2019)]}, volume = {135}, year = {2025}, }
• (2025). Deciphering complexity in human brain organoids via a novel hurst exponent estimation. PRL, 135(10), 108402. (www)

  @article{ , abstract = {Complexity is a hallmark of the human brain, emerging from the interaction of billions of neurons over time. Among various measures, the Hurst exponent ( H ) has been used to characterize temporal correlations in neuronal activity. Here, we introduce a method to estimate H directly from binary spike train series and propose that the coefficient of variation (CV) of H , rather than H itself, more accurately reflects neural complexity during organoid maturation. After validating the method on simulated data with embedded short- and long-range correlations, we applied it to cortical organoids derived from human-induced pluripotent stem cells, recorded via multielectrode arrays over 250 day. The analysis revealed a peak in complexity, as indicated by the CV of H , around the 100th day. At this stage, the organoids exhibited a wide repertoire of dynamic patterns, including both isolated spiking and highly synchronized network events. These results suggest that organoid activity undergoes a structured evolution in complexity and that CV of H provides a robust metric to capture this transition. Our approach offers a scalable tool for quantifying neural complexity in the developing brain.}, archive = {J_PRL}, author = {Mariana Sacrini Ayres Ferraz and Alysson R. Muotri and Alexandre Hiroaki Kihara}, doi = {10.1103/kl6z-ctdd}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {108402}, shortjournal = {Phys. Rev. Lett.}, title = {Deciphering complexity in human brain organoids via a novel hurst exponent estimation}, volume = {135}, year = {2025}, }
• (2025). Cell stiffness-mediated mechanochemical waves in three-dimensional tissues. PRL, 135(10), 108401. (www)

  @article{ , abstract = {Tissue development, physiological or pathological, commonly involves stiffness alterations in the constituent cells. Here, we develop a three-dimensional (3D) active vertex model incorporating mechanical feedback from extracellular signal-regulated kinase (ERK) to explore mechanochemical waves in tissues with varying cell stiffness. Combining theory and simulations, we show that rich cell oscillations, mediated by cell stiffness and its spatial heterogeneity, can arise from mechanochemical instability. Increasing cell stiffness promotes the long-range force transmission and synchronization of collective waves, which exhibit robustness against cell heterogeneity of both size and stiffness. These mechanochemical waves can propagate around the locally stiffened inclusions or traverse stiff walls but retain their intrinsic modes. We further generate and interpret the ERK edge wave in 3D multicellular spheroids with stiffness variation, consistent with previous experiments. Our work uncovers the multifaceted roles of mechanics in self-organized mechanochemical dynamics within 3D multicellular tissues.}, archive = {J_PRL}, author = {Pengyu Yu and Rui Zhang and Bo Li}, doi = {10.1103/r4fs-4qqk}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {108401}, shortjournal = {Phys. Rev. Lett.}, title = {Cell stiffness-mediated mechanochemical waves in three-dimensional tissues}, volume = {135}, year = {2025}, }
• (2025). Nonreciprocal mixtures in suspension: The role of hydrodynamic interactions. PRL, 135(10), 108301. (www)

  @article{ , abstract = {The collective chasing dynamics of nonreciprocally coupled densities leads to stable traveling waves which can be mapped to a model for emergent flocking. In this Letter, we couple the nonreciprocal Cahn-Hilliard model to a fluid to minimally describe scalar active mixtures in a suspension, with the aim to explore the stability of the waves, i.e., the emergent flock in the presence of self-generated fluid flows. We show that the emergent polarity is linearly unstable to perturbations for a specific sign of the active stress recalling instabilities of orientational order in a fluid. Using numerical simulations, we find, however, that nonreciprocity stabilizes the waves against the linear instability in a large region of the phase space.}, archive = {J_PRL}, author = {Giulia Pisegna and Navdeep Rana and Ramin Golestanian and Suropriya Saha}, doi = {10.1103/gbg1-lwwt}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {108301}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal mixtures in suspension: The role of hydrodynamic interactions}, volume = {135}, year = {2025}, }
• (2025). Anomalous shear stress growth during relaxation of a soft glass. PRL, 135(10), 108202. (www)

  @article{ , abstract = {We show experimentally that multiple soft glassy fluids are capable of storing directional rheological signatures from past shear history, evidenced during stress growth and overall nonmonotonic stress relaxation after small steps in strain. We illustrate theoretically that these responses can be reproduced without requiring thixotropy or shear banding, which are typically implicated in time-dependent rheological complexities. Instead, we use a simple elastoplastic rheological model with power-law yielding that incorporates a distribution of local strain states. Using insight from the model, we suggest a mechanism for the experimentally observed stress increase to be driven by residual anisotropy in strain states that are relaxed at different rates. We demonstrate that these effects persist even after material is stressed beyond the yield stress, indicating that past deformation may have more influence than previously thought.}, archive = {J_PRL}, author = {Crystal E. Owens}, doi = {10.1103/421k-58rm}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {108202}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous shear stress growth during relaxation of a soft glass}, volume = {135}, year = {2025}, }
• (2025). Particle scale anisotropy controls bulk properties in sheared granular materials. PRL, 135(10), 108201. (www)

  @article{ , abstract = {The bulk dynamics of dense granular materials arise through a combination of particle-scale and mesoscale effects. Theoretical and numerical studies have shown that collective effects are created by particle-scale anisotropic structures such as grain connectivity, force transmission, and frictional mobilization, all of which influence bulk properties like bulk friction and the stress tensor through the stress-force-fabric (SFF) relationship. To date, establishing the relevance of these effects to laboratory systems has remained elusive due to the challenge of measuring both normal and frictional contact forces at the particle scale. In this study, we perform experiments on a sheared photoelastic granular system in a quasi-2D annular cell. During these experiments, we measure particle locations, contacts, and normal and frictional forces vectors during loading. We reconstruct the angular distributions of the contact and force vectors, and extract the corresponding emergent anisotropies for each of these metrics. Finally, we show for the first time in an experimental system that the SFF relation quantitatively predicts the relationship between particle scale anisotropies, the stress tensor components, and the bulk friction coefficient, capturing even transient behaviors—closing the gap between experimental measurements and prior theoretical and numerical models.}, archive = {J_PRL}, author = {Carmen L. Lee and Ephraim Bililign and Emilien Azéma and Karen E. Daniels}, doi = {10.1103/gp8t-v82n}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {108201}, shortjournal = {Phys. Rev. Lett.}, title = {Particle scale anisotropy controls bulk properties in sheared granular materials}, volume = {135}, year = {2025}, }
• (2025). Theory of microphase separation in elastomers. PRL, 135(10), 108101. (www)

  @article{ , abstract = {Inspired by recent experiments, we present a phase-field model of microphase separation in an elastomer swollen with a solvent. The imbalance between the molecular scale of demixing and the mesoscopic scale beyond which elasticity operates produces effective long-range interactions, forming stable finite-sized domains. Our predictions concerning the dependence of the domain size and transition temperature on the stiffness of the elastomer are in good agreement with the experiments. Analytical phase diagrams, aided by numerical findings, capture the richness of the microphase morphologies, paving the way to create stable, patterned elastomers for various applications.}, archive = {J_PRL}, author = {Manu Mannattil and Haim Diamant and David Andelman}, doi = {10.1103/5q7m-3fpn}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {108101}, shortjournal = {Phys. Rev. Lett.}, title = {Theory of microphase separation in elastomers}, volume = {135}, year = {2025}, }
• (2025). Exact computation of transfer entropy with path weight sampling. PRL, 135(10), 107404. (www)

  @article{ , abstract = {The ability to quantify the directional flow of information is vital to understanding natural systems and designing engineered information-processing systems. A widely used measure to quantify this information flow is the transfer entropy. However, until now, this quantity could only be obtained in dynamical models using approximations that are typically uncontrolled. Here we introduce a computational algorithm called “transfer entropy-path weight sampling” (TE-PWS), which makes it possible, for the first time, to quantify the transfer entropy and its variants exactly for any stochastic model, including those with multiple hidden variables, nonlinearity, transient conditions, and feedback. By leveraging techniques from polymer and path sampling, TE-PWS efficiently computes the transfer entropy as a Monte Carlo average over signal trajectory space. We use our exact technique to demonstrate that commonly used approximate methods to compute transfer entropies incur large systematic errors and high computational costs. As an application, we use TE-PWS in linear and nonlinear systems to reveal how transfer entropy can overcome naive applications of the data processing inequality in the presence of feedback.}, archive = {J_PRL}, author = {Avishek Das and Pieter Rein ten Wolde}, doi = {10.1103/t8z9-ylvg}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {107404}, shortjournal = {Phys. Rev. Lett.}, title = {Exact computation of transfer entropy with path weight sampling}, volume = {135}, year = {2025}, }
• (2025). Weak-correlation universality and macroscopic fluctuations in power-law recurrent networks. PRL, 135(10), 107403. (www)

  @article{ , abstract = {Balanced network theory describes the dynamic state of randomly connected systems with intrinsic negative feedback, predicting the suppression of correlations as connectivity increases. We show that this weak-correlation universality holds broadly but breaks down in power-law networks where the largest out-degrees scale with system size. In such networks, residual correlations cross over to a regime that retains macroscopic fluctuations in the thermodynamic limit. Unlike Erdös-Rényi networks, the degree heterogeneity of power-law topologies amplifies coherent population-level fluctuations. Our results provide a theoretical foundation for the strong correlations observed in real-world networks with sparse and heterogeneous connectivity.}, archive = {J_PRL}, author = {Farzada Farkhooi}, doi = {10.1103/l6pc-y1x6}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {107403}, shortjournal = {Phys. Rev. Lett.}, title = {Weak-correlation universality and macroscopic fluctuations in power-law recurrent networks}, volume = {135}, year = {2025}, }
• (2025). Hydrodynamics of cooperation and self-interest in a two-population occupation model. PRL, 135(10), 107402. (www)

  @article{ , abstract = {We study the hydrodynamics of a system of agents that optimize either their individual utility (self-interest) or the collective welfare (cooperation). When agents act selfishly, their interactions are nonreciprocal, driving the system out of equilibrium; by contrast, purely altruistic dynamics restore reciprocity and yield an equilibrium description. We investigate how mixtures of these two behaviors shape the macroscopic properties of the liquid of agents. For highly rational agents, we find that introducing a small fraction of altruists can suppress the suboptimal clustering induced by selfish dynamics. This phenomenon can be attributed to altruists localizing at interfaces and acting as effective surfactants, shedding a new light on earlier findings in fixed neighborhood-based models [ Phys. Rev. Lett. 120 , 208301 (2018) ]. When agents are “boundedly rational,” we introduce a well-mixed approximation that reduces the two-population model to a single effective scalar field theory. This allows us to leverage state-of-the-art tools from active matter to analytically characterize how altruism modifies surface tension and nucleation dynamics.}, archive = {J_PRL}, author = {Jérôme Garnier-Brun and Ruben Zakine and Michael Benzaquen}, doi = {10.1103/3bj7-jc92}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {107402}, shortjournal = {Phys. Rev. Lett.}, title = {Hydrodynamics of cooperation and self-interest in a two-population occupation model}, volume = {135}, year = {2025}, }
• (2025). Diffusive nature of housing prices. PRL, 135(10), 107401. (www)

  @article{ , abstract = {We analyze the French housing market prices in the period 1970–2022, with high-resolution data from 2018 to 2022. The spatial correlation of the observed price field exhibits logarithmic decay characteristic of the two-dimensional random diffusion equation— local interactions may create long-range correlations. We introduce a stylized model, used in the past to model spatial regularities in voting patterns, that accounts for both spatial and temporal correlations with reasonable values of parameters, some fitted on impulse response data. Our analysis reveals that price shocks are persistent in time and their amplitude is strongly heterogeneous in space. Our study quantifies the diffusive nature of housing prices that was anticipated in the 1990s, albeit on much restricted local datasets.}, archive = {J_PRL}, author = {Antoine-Cyrus Becharat and Michael Benzaquen and Jean-Philippe Bouchaud}, doi = {10.1103/f4vr-xdny}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {107401}, shortjournal = {Phys. Rev. Lett.}, title = {Diffusive nature of housing prices}, volume = {135}, year = {2025}, }
• (2025). Optical signatures of dynamical excitonic condensates. PRL, 135(10), 106902. (www)

  @article{ , abstract = {We theoretically study dynamical excitonic condensates occurring in bilayers with an imposed chemical potential difference and in photodoped semiconductors. We show that optical spectroscopy can experimentally identify phase-trapped and phase-delocalized dynamical regimes of condensation. In the weak-bias regime, the trapped dynamics of the order parameter’s phase lead to an in-gap absorption line at a frequency almost independent of the bias voltage, while, for larger biases, the frequency of the spectral feature increases approximately linearly with bias. In both cases, there is a pronounced second-harmonic response. Close to the transition between the trapped and freely oscillating states, we find a strong response upon application of a weak electric probe field, compare the results to those found in a minimal model description for the dynamics of the order parameter’s phase, and analyze the limitations of the latter.}, archive = {J_PRL}, author = {Alexander Osterkorn and Yuta Murakami and Tatsuya Kaneko and Zhiyuan Sun and Andrew J. Millis and Denis Golež}, doi = {10.1103/58r8-cpzn}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106902}, shortjournal = {Phys. Rev. Lett.}, title = {Optical signatures of dynamical excitonic condensates}, volume = {135}, year = {2025}, }
• (2025). Mixing of surface and bulk optical nonlinearities via surface plasmon polaritons. PRL, 135(10), 106901. (www)

  @article{ , abstract = {We present controlled interplay between the surface second-order and bulk third-order nonlinearities of gold, utilizing wave mixing between surface plasmons on the metal-air interface and free-space photons. By tuning the nonlinear interactions, we demonstrate experimentally that photons emerging from these inherently different mechanisms can interfere, while both their relative amplitude and phase are controlled solely by the pump beam. These results provide a foundation for engineering plasmonic nonlinearities and open new possibilities for quantum photonic applications.}, archive = {J_PRL}, author = {Guy Sayer and Matan Iluz and Amit Kam and Guy Bartal}, doi = {10.1103/qs45-4rqd}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106901}, shortjournal = {Phys. Rev. Lett.}, title = {Mixing of surface and bulk optical nonlinearities via surface plasmon polaritons}, volume = {135}, year = {2025}, }
• (2025). High-temperature phase separation and charge-magnon liquid in kinetic antiferromagnets. PRL, 135(10), 106702. (www)

  @article{ , abstract = {Understanding mechanisms of quantum ordering in strongly correlated systems remains a central challenge in condensed matter physics, with implications for designing novel quantum materials. Here, we investigate kinetic antiferromagnetism on a triangular lattice under an applied magnetic field, where spin polarons emerge as charge-magnon bound states with mutual attraction. Using large-scale diagrammatic Monte Carlo simulations, we show that this interaction drives high-temperature phase separation into charge- and magnon-rich regions, bordered by polarized Mott insulating voids. Spectral function analysis reveals a substantial energy correction from magnon interactions, indicating that these carrier-rich regions form a strongly bound charge-magnon liquid. These findings shed new light on recent experiments on moiré bilayers, underscoring kinetic magnetism as a unique pathway for strong intercarrier attraction and high-temperature quantum ordering, with potential applications in quantum materials.}, archive = {J_PRL}, author = {Johan Carlström}, doi = {10.1103/d9c2-yr7j}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106702}, shortjournal = {Phys. Rev. Lett.}, title = {High-temperature phase separation and charge-magnon liquid in kinetic antiferromagnets}, volume = {135}, year = {2025}, }
• (2025). Tomography of parametric transition in magnets. PRL, 135(10), 106701. (www)

  @article{ , abstract = {Temporal evolution of Wigner functions representing fluctuation distribution of magnetization in (YIG) at the moment of parametric oscillation onset has been investigated. Our newly developed time-resolved spectroscopy unmasks that highly distorted and stretched correlation of magnetization fluctuation leads the parametric oscillation, being consistent with numerical simulation incorporating nonlinear four-magnon scattering. The method offers a powerful tool for probing nonlinear dynamics in a variety of magnets.}, archive = {J_PRL}, author = {Hiroki Shimizu and Tomosato Hioki and Shuntaro Takeda and Eiji Saitoh}, doi = {10.1103/v1rk-rtrq}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106701}, shortjournal = {Phys. Rev. Lett.}, title = {Tomography of parametric transition in magnets}, volume = {135}, year = {2025}, }
• (2025). Extrinsic mechanisms of phonon magnetic moment. PRL, 135(10), 106605. (www)

  @article{ , abstract = {We develop a general formalism of the phonon magnetic moment by including the relaxation processes. We then identify the skew-scattering and side-jump contributions to the phonon magnetic moment originating from the nonadiabaticity, both of which are related to the nonlocal phonon Berry curvature and are in close analogy to those in the electronic Hall effect. All contributions of the phonon magnetic moment are exemplified in a honeycomb lattice, showing that the extrinsic contribution can be as important as the intrinsic one and that the resulting phonon angular momentum varies significantly across the Brillouin zone. Our Letter offers a systematic framework of the phonon chirality and paves the way for tuning the phonon magnetic moment through the nonadiabaticity.}, archive = {J_PRL}, author = {Rui Xue and Zhenhua Qiao and Yang Gao and Qian Niu}, doi = {10.1103/6m7v-p99w}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106605}, shortjournal = {Phys. Rev. Lett.}, title = {Extrinsic mechanisms of phonon magnetic moment}, volume = {135}, year = {2025}, }
• (2025). Non-abelian fractional chern insulators and competing states in flat moiré bands. PRL, 135(10), 106604. (www)

  @article{ , abstract = {Breakthrough experiments have recently realized fractional Chern insulators (FCIs) in moiré materials. However, all states observed are Abelian; the possible existence of more exotic non-Abelian FCIs remains controversial both experimentally and theoretically. Here, we investigate the competition between charge density wave (CDW) order, gapless composite fermion liquid (CFL), and non-Abelian Moore-Read states at half filling of a moiré band. Although ground-state (quasi)degeneracies and spectral flow are not sufficient for distinguishing between charge order and Moore-Read states, we find evidence using entanglement spectroscopy that both these states of matter can be realized with Coulomb interactions. By further analyzing the graviton excitations of Moore-Read states, we unveil that the ground states exhibit a mixed behavior of Pfaffian and anti-Pfaffian, despite the weak breaking of particle-hole symmetry. In a double twisted bilayer graphene model, transitions between these phases can be driven by the coupling strength between the layers: at weak coupling there is a CFL phase and at strong coupling a CDW order emerges. Remarkably, however, there is compelling evidence for a non-Abelian Moore-Read FCI phase at intermediate coupling.}, archive = {J_PRL}, author = {Hui Liu and Zhao Liu and Emil J. Bergholtz}, doi = {10.1103/43nq-ntqm}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106604}, shortjournal = {Phys. Rev. Lett.}, title = {Non-abelian fractional chern insulators and competing states in flat moiré bands}, volume = {135}, year = {2025}, }
• (2025). Anomalous hall effect in the dirac semimetal Cd3As2 probed by in-plane magnetic field. PRL, 135(10), 106603. (www)

  @article{ , abstract = {Intrinsic anomalous Hall effect (AHE) formulated by geometric properties of Bloch wave functions is a ubiquitous transport phenomenon not limited to magnetic systems but also allowed in nonmagnetic ones under an external field breaking time-reversal symmetry. On the other hand, detection of field-induced AHE is practically challenging because the band modulation through the Zeeman and spin-orbit couplings is typically small compared to other contributions as induced by the Lorentz force. Here, we demonstrate on Dirac semimetal films that the field-induced AHE in nonmagnetic systems can be quantitatively probed by applying and rotating the magnetic field within the Hall deflection plane. Measurements on the (112) plane reveal that AHE emerges as a clear threefold symmetric component for the in-plane field rotation. This intrinsic response becomes more pronounced in ultralow-electron-density films where significant variations in the geometric properties are expected under the magnetic field. Our findings open new opportunities in the research of Hall responses manifested as orbital magnetization in nonmagnetic systems.}, archive = {J_PRL}, author = {Shinichi Nishihaya and Hiroaki Ishizuka and Yuki Deguchi and Ayano Nakamura and Tadashi Yoneda and Hsiang Lee and Markus Kriener and Masaki Uchida}, doi = {10.1103/5d7l-mr7k}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106603}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous hall effect in the dirac semimetal Cd3As2 probed by in-plane magnetic field}, volume = {135}, year = {2025}, }
• (2025). Quantum geometry and the electric magnetochiral anisotropy in noncentrosymmetric polar media. PRL, 135(10), 106602. (www)

  @article{ , abstract = {The electric magnetochiral anisotropy is a nonreciprocal phenomenon accessible via second harmonic transport in noncentrosymmetric, time-reversal invariant materials, in which the rectification of current, can be controlled by an external magnetic field, . Quantum geometry, which characterizes the topology of Bloch electrons in a Hilbert space, provides a powerful description of the nonlinear dynamics in topological materials. Here, we demonstrate that the electric magnetochiral anisotropy in noncentrosymmetric polar media owes its existence to the quantum metric, arising from the spin-orbit coupling, and to large Born effective charges. In this context, the reciprocal magnetoresistance is modified to , where the chirality dependent is determined by the quantum metric dipole and is the polarization. In 2D, we predict a universal scaling , which we compare to available phase sensitive, second harmonic transport measurements on hydrothermally grown tellurium films under applied gate voltage, . The control of rectification by varying , and , demonstrated in this work, opens up new avenues for the building of ultrascaled complementary metal-oxide-semiconductor circuits.}, archive = {J_PRL}, author = {Pierpaolo Fontana and Victor Velasco and Chang Niu and Peide D. Ye and Pedro V. Lopes and Kaio E. M. de Souza and Marcus V. O. Moutinho and Caio Lewenkopf and Marcello B. Silva Neto}, doi = {10.1103/7nxc-j62y}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106602}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum geometry and the electric magnetochiral anisotropy in noncentrosymmetric polar media}, volume = {135}, year = {2025}, }
• (2025). Non-hermitian floquet topological sensors for ultrasensitive detection of dynamic signals. PRL, 135(10), 106601. (www)

  @article{ , abstract = {Non-Hermitian systems, distinguished by the presence of exceptional points and non-Hermitian topological states, have transformed sensing technologies through the implementation of novel physical mechanisms. However, despite their demonstrated potential, existing non-Hermitian sensors are predominantly limited to static operational configurations, which substantially restricts their effects in detecting time-varying signals. Here, we transcend this limitation by introducing a new sensing framework: non-Hermitian Floquet topological sensors (NHFTSs). This approach harnesses the synergistic interplay among time-periodic driving, nonlinear dynamics, and non-Hermitian topology to enable ultrasensitive detection of dynamic signals. NHFTSs establish nonlinear non-Hermitian Floquet topological zero modes as robust global attractors. These modes manifest extraordinary sensitivity to dynamic boundary perturbations, exhibiting frequency shifts that scale exponentially with system size. Moreover, NHFTSs possess exceptional resilience against both background noise and structural perturbations, a feature enabled by the dual protective mechanisms of nonlinear stability and topological band gaps. Notably, the signal-to-noise ratio of NHFTSs can be exponentially amplified through sensor size scaling. We experimentally validate the NHFTS using time-varying topolectrical circuits, demonstrating their unparalleled capability in detecting dynamic electrical signals with high sensitivity and signal-to-noise ratios. This Letter not only establishes a new paradigm for non-Hermitian dynamical sensing but also paves the way for exploring non-Hermitian topological phenomena in Floquet nonlinear systems, with profound implications for the development of next-generation non-Hermitian sensors and beyond.}, archive = {J_PRL}, author = {Xiaoqi Zhou and Weixuan Zhang and Wenhui Cao and Xiangdong Zhang}, doi = {10.1103/f6wd-gljq}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106601}, shortjournal = {Phys. Rev. Lett.}, title = {Non-hermitian floquet topological sensors for ultrasensitive detection of dynamic signals}, volume = {135}, year = {2025}, }
• (2025). Current-induced nonequilibrium hidden spin polarization in topological dirac semimetals. PRL, 135(10), 106505. (www)

  @article{ , abstract = {The effect of hidden spin polarization (HSP) has expanded the material pool for spintronics and provided new physical insights into relevant hidden phenomena such as optical polarization, valley polarization, orbital polarization, and Berry curvature. Here, we uncover an intrinsic HSP in topological Dirac semimetals originating from the three-dimensional quantum Hall effect. This local spin polarization arises through nonequilibrium processes, where the Landau levels tilt due to the -symmetry breaking induced by crossed electric and magnetic fields. We find that the nonequilibrium HSP exhibits directional selectivity owing to the spin-momentum-surface locking of the Fermi arcs. As a result of the Weyl-orbit quantization, the local spin polarization exhibits quantum oscillations with sample thickness and displays plateaus as the Fermi energy varies. This nonequilibrium HSP, which can be detected through current-induced nonlocal spin-orbit torques, is unique to the Weyl orbits. Our findings present a novel mechanism for detecting Weyl orbits and for nonlocally controlling magnetization using external electric fields.}, archive = {J_PRL}, author = {Yun-Jing Lai and Meng-Rou Huang and Hou-Jian Duan and Mou Yang and Rui-Qiang Wang and Ming-Xun Deng}, doi = {10.1103/snby-9xsr}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106505}, shortjournal = {Phys. Rev. Lett.}, title = {Current-induced nonequilibrium hidden spin polarization in topological dirac semimetals}, volume = {135}, year = {2025}, }
• (2025). Terahertz field control of electronic-ferroelectric anisotropy at room temperature in LuFe2O4. PRL, 135(10), 106504. (www)

  @article{ , abstract = {Electronic ferroelectrics, with polarization P induced by strongly correlated charges, are expected to show ultrafast, huge, and flexible responses required in future optoelectronics. Although the challenges for ultrafast manipulation of such a polarization are ongoing, the expected advantages have been unclear. In this Letter, we demonstrate an unprecedentedly large increase by a factor of 2.7 in optical second harmonic generation at room temperature in the prototypical electronic ferroelectrics, the rare-earth ferrite LuFe 2 O 4 , by applying a terahertz field of 260 kV / cm . The transient anisotropy indicates that the direction of macroscopic polarization can be controlled three dimensionally on subpicosecond timescales, offering additional degrees of freedom in controlling polarization. Although the polarization response is in phase concerning the terahertz field, its sensitivity increased with delay, indicating that cooperative interactions among microscopic domains play an important role in the unprecedented response.}, archive = {J_PRL}, author = {Hirotake Itoh and Ryusei Minakami and Hongwu Yu and Ryohei Tsuruoka and Tatsuya Amano and Yohei Kawakami and Shin-ya Koshihara and Kosuke Fujiwara and Naoshi Ikeda and Yoichi Okimoto and Shinichiro Iwai}, doi = {10.1103/fryl-jjnj}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106504}, shortjournal = {Phys. Rev. Lett.}, title = {Terahertz field control of electronic-ferroelectric anisotropy at room temperature in LuFe2O4}, volume = {135}, year = {2025}, }
• (2025). Robust charge density wave correlations in optimally doped YBa2Cu3Oy. PRL, 135(10), 106503. (www)

  @article{ , abstract = {Charge density wave (CDW) order is a key property of high- cuprates, but its boundaries in the phase diagram and potential connections to other phases remain controversial. We report nuclear magnetic resonance (NMR) measurements in the prototypical cuprate demonstrating that short-range static CDW order remains robust at optimal doping ( ), exhibiting a strength and temperature dependence in the normal state similar to those observed at in the underdoped regime. For an overdoped sample with , we detect no static CDW down to , though weak CDW order plausibly emerges below . More broadly, we argue that both quenched disorder and competition with superconductivity influence the apparent boundary of the CDW phase, likely causing an underestimation of its intrinsic extent in doping. These findings challenge the view that the CDW phase boundary lies below , widely regarded as the critical doping where the pseudogap phase ends in .}, archive = {J_PRL}, author = {Rui Zhou and Igor Vinograd and Hadrien Mayaffre and Juan Porras and Hun-Ho Kim and Toshinao Loew and Yiran Liu and Matthieu Le Tacon and Bernhard Keimer and Marc-Henri Julien}, doi = {10.1103/8klr-4wc5}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106503}, shortjournal = {Phys. Rev. Lett.}, title = {Robust charge density wave correlations in optimally doped YBa2Cu3Oy}, volume = {135}, year = {2025}, }
• (2025). Density matrix renormalization group algorithm for non-hermitian systems. PRL, 135(10), 106502. (www)

  @article{ , abstract = {A biorthonormal-block density-matrix renormalization group algorithm is proposed to accurately compute properties of large-scale non-Hermitian many-body systems, in which a renormalized-space partition of the non-Hermitian reduced density matrix is implemented to fulfill the prerequisite for the biorthonormality of the renormalization group (RG) transformation and to optimize the construction of saved Hilbert spaces. A redundancy in saved spaces of the reduced density matrix is exploited to reduce a condition number resulting from the nonunitarity of the left and right transformation matrices, in order to ensure the numerical stability of the RG procedure. The algorithm is successfully applied to an interacting fermionic Su-Schrieffer-Heeger model with nonreciprocal hoppings and staggered complex chemical potential, exhibiting novel many-body phenomena.}, archive = {J_PRL}, author = {Peigeng Zhong and Wei Pan and Haiqing Lin and Xiaoqun Wang and Shijie Hu}, doi = {10.1103/5vnl-w9p4}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106502}, shortjournal = {Phys. Rev. Lett.}, title = {Density matrix renormalization group algorithm for non-hermitian systems}, volume = {135}, year = {2025}, }
• (2025). High-throughput search for metallic altermagnets by embedded dynamical mean field theory. PRL, 135(10), 106501. (www)

  @article{ , abstract = {We introduce a high-fidelity high-throughput screening (HTS) strategy to accelerate the discovery of altermagnets by combining density functional theory (DFT) with embedded dynamical mean-field theory. Our approach improves over the HTS with the conventional DFT method in the accuracy of predicting metallicity and spin splitting, especially in transition-metal-rich compounds. Our method is based on an automated workflow that incorporates prescreening and symmetry analysis and can be applied to a variety of correlated materials. This approach identified two previously unreported metallic altermagnets, CrSe and (in addition to one known altermagnet CrSb), as well as a dozen semiconducting altermagnets among over 2000 magnetic materials. Our findings reveal that while altermagnets are abundant among magnetic materials, only a tiny fraction are metallic.}, archive = {J_PRL}, author = {Xuhao Wan and Subhasish Mandal and Yuzheng Guo and Kristjan Haule}, doi = {10.1103/k47t-23gp}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106501}, shortjournal = {Phys. Rev. Lett.}, title = {High-throughput search for metallic altermagnets by embedded dynamical mean field theory}, volume = {135}, year = {2025}, }
• (2025). Probing green’s function zeros by cotunneling through mott insulators. PRL, 135(10), 106303. (www)

  @article{ , abstract = {Quantum tunneling experiments have provided deep insights into basic excitations occurring as Green’s function poles in the realm of complex quantum matter. However, strongly correlated quantum materials also allow for Green’s functions zeros (GFZs) that may be seen as an antidote to the familiar poles and have so far largely eluded direct experimental study. Here, we propose and investigate theoretically how cotunneling through Mott insulators enables direct access to the shadow band structure of GFZs. In particular, we derive an effective Hamiltonian for the GFZ that is shown to govern the cotunneling amplitude and reveal fingerprints of many-body correlations clearly distinguishing the GFZ structure from the underlying free Bloch band structure of the system. Our perturbative analytical results are corroborated by numerical data in the framework of both exact diagonalization and matrix product state simulations for a one-dimensional model system consisting of a Su-Schrieffer-Heeger-Hubbard model coupled to two single-level quantum dots.}, archive = {J_PRL}, author = {Carl Lehmann and Lorenzo Crippa and Giorgio Sangiovanni and Jan Carl Budich}, doi = {10.1103/jnq4-sykq}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106303}, shortjournal = {Phys. Rev. Lett.}, title = {Probing green’s function zeros by cotunneling through mott insulators}, volume = {135}, year = {2025}, }
• (2025). Nonreciprocity of hydrodynamic electron transport in noncentrosymmetric conductors. PRL, 135(10), 106302. (www)

  @article{ , abstract = {We show that the nonreciprocity of hydrodynamic electron transport in noncentrosymmetric conductors with broken time-reversal symmetry is significantly enhanced compared to the disorder-dominated regime. This enhancement is caused by the linear dependence of the viscosity of the electron liquid on the flow velocity, which is allowed in the absence of time-reversal symmetry and Galilean invariance. The resulting nonlinear flows break dynamical similarity, and, thus, in addition to the Reynolds number, they are characterized by a second dimensionless parameter, the nonreciprocity number. The latter is linear in velocity but independent of system size. We determine the nonlinear conductance of a Hall bar and show that the nonreciprocal correction to the current can be of comparable magnitude to its reciprocal counterpart.}, archive = {J_PRL}, author = {E. Kirkinis and L. Bonds and A. Levchenko and A. V. Andreev}, doi = {10.1103/nx9z-vkk2}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106302}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocity of hydrodynamic electron transport in noncentrosymmetric conductors}, volume = {135}, year = {2025}, }
• (2025). Intrinsic dynamic generation of spin polarization by time-varying electric field. PRL, 135(10), 106301. (www)

  @article{ , abstract = {Electric control of spin in insulators is desired for low-consumption and ultrafast spintronics, but the underlying mechanism remains largely unexplored. Here, we propose an intrinsic effect of dynamic spin generation driven by time-varying electric field. In the intraband response regime, it can be nicely formulated as a Berry curvature effect and leads to two phenomena that are forbidden in the dc limit: linear spin generation in nonmagnetic insulators and intrinsic Néel spin-orbit torque in -symmetric antiferromagnetic insulators. These phenomena are driven by the time derivative of field rather than the field itself, and have a quantum origin in the first-order dynamic anomalous spin polarizability. Combined with first-principles calculations, we predict sizable effects driven by the terahertz field in nonmagnetic monolayer Bi and in antiferromagnetic even-layer , which can be detected in experiment.}, archive = {J_PRL}, author = {Xukun Feng and Jin Cao and Zhi-Fan Zhang and Lay Kee Ang and Shen Lai and Hua Jiang and Cong Xiao and Shengyuan A. Yang}, doi = {10.1103/7blz-pswv}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106301}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic dynamic generation of spin polarization by time-varying electric field}, volume = {135}, year = {2025}, }
• (2025). Multiorbital interactions and spin polarization in single rare-earth adatoms. PRL, 135(10), 106203. (www)

  @article{ , abstract = {Surface-adsorbed rare-earth nanostructures are ideal platforms to investigate the interplay between intra-atomic interactions and multiorbital spin configurations. However, addressing these properties has posed severe experimental and theoretical challenges. Here, we use the orbital selectivity offered by x-ray absorption spectroscopy to quantify the Coulomb integrals of Nd atoms on conductive surfaces directly from experimental quantities, as well as the variation of individual orbital occupation upon cluster nucleation. Using x-ray magnetic circular dichroism we identify magnetic moments of the order of 0. at the orbitals and their magnetic coupling with the spins. Our results validate orbital-resolved x-ray spectroscopy as a reliable method for quantifying complex multiorbital interactions in surface-adsorbed lanthanides.}, archive = {J_PRL}, author = {Massine Kelai and Stefano Reale and Roberto Robles and Jaehyun Lee and Divya Jyoti and Philippe Ohresser and Edwige Otero and Fadi Choueikani and Fabrice Scheurer and Nicolás Lorente and Deung-Jang Choi and Aparajita Singha and Fabio Donati}, doi = {10.1103/mkqz-p424}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106203}, shortjournal = {Phys. Rev. Lett.}, title = {Multiorbital interactions and spin polarization in single rare-earth adatoms}, volume = {135}, year = {2025}, }
• (2025). Singlet-only always-on gapless exchange qubits with baseband control. PRL, 135(10), 106202. (www)

  @article{ , abstract = {We propose a singlet-only always-on gapless exchange (SAGE) spin qubit that encodes a single qubit in the spins of four electrons while allowing universal baseband control. While conventional exchange-only qubits suffer from magnetic-field-gradient-induced leakage and coherent errors due to local nuclear environments and variations in the -factor, the SAGE qubit subspace is protected from coherent errors due to local magnetic field gradients, and leakage out of the computational subspace is energetically suppressed due to the exchange interactions between electrons being always on. Consequently, we find that when magnetic gradient noise dominates over charge noise, coherence times and single-qubit gate infidelities of the SAGE qubit improve by an order of magnitude compared to conventional exchange-only qubits. Moreover, using realistic parameters, two-qubit gates can be performed with a single interqubit exchange pulse with times comparable in duration to conventional exchange-only qubits but with a significantly simplified pulse sequence.}, archive = {J_PRL}, author = {Nathan L. Foulk and Silas Hoffman and Katharina Laubscher and Sankar Das Sarma}, doi = {10.1103/j1hn-k5m8}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106202}, shortjournal = {Phys. Rev. Lett.}, title = {Singlet-only always-on gapless exchange qubits with baseband control}, volume = {135}, year = {2025}, }
• (2025). Dual role for heterogeneity in dynamic fracture. PRL, 135(10), 106201. (www)

  @article{ , abstract = {We approach the problem of heterogeneous dynamic fracture by considering spatiotemporal perturbations to planar crack fronts. Front propagation is governed by local energy balance between the elastic energy per unit area available to fracture and the dissipation in creating new surfaces. is known analytically as a perturbation series in the crack front fluctuation. For dissipation that monotonically increases with the crack speed, we derive an equation of motion for crack fronts that is second-order accurate. In the linear order, heterogeneity does not change the net speed of fracture. In the second order, nonlinear interactions of the front and the heterogeneous landscape populate an intermediate-scale fluctuation spectrum. We find that, when dissipation weakly grows with velocity, nonlinearities globally amplify dissipation and reduce the crack speed. Strong velocity dependence, however, mitigates toughening effects and may facilitate fracture.}, archive = {J_PRL}, author = {Itamar Kolvin and Mokhtar Adda-Bedia}, doi = {10.1103/j4vb-y1ng}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106201}, shortjournal = {Phys. Rev. Lett.}, title = {Dual role for heterogeneity in dynamic fracture}, volume = {135}, year = {2025}, }
• (2025). Pressure-induced polyhedral reorganization causes indirect-to-direct band-gap transition in spinel structure. PRL, 135(10), 106102. (www)

  @article{ , abstract = {Spinel oxides ( ) are promising optoelectronic materials due to their structural stability and tunable electronic properties. However, conventional strategies like doping, element substitution, and thermal treatment have achieved limited success in optimizing their performance. Here, we demonstrate that pressure-induced polyhedral reorganization triggers an indirect-to-direct band-gap transition driven by the enhanced hybridization of orbitals in systems. The pressure-induced polyhedral reorganization also causes a connectivity shift from corner-sharing tetrahedra ( ) to edge-sharing octahedra ( ) in single-phase crystals, which tailors the electronic redistribution from isolated to quasi-1D ladderlike configurations. The optimized electronic structure leads to a concurrent enhancement in the photoresponsivity by and the emergence of an exotic white-light emission, which can be quenched to ambient conditions. These findings reveal how polyhedral reorganization directly governs electronic evolution in , providing a new pathway to tailor electronic structures and optoelectronic properties through pressure-driven design that bypasses the limitations of traditional approaches.}, archive = {J_PRL}, author = {Pengfei Shen and Donghao Xu and Zhiguo Xia and Mingguang Yao}, doi = {10.1103/v4x6-hksk}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106102}, shortjournal = {Phys. Rev. Lett.}, title = {Pressure-induced polyhedral reorganization causes indirect-to-direct band-gap transition in spinel structure}, volume = {135}, year = {2025}, }
• (2025). Emergent negative thermal expansion in amorphous fe-Y-zr-B alloys. PRL, 135(10), 106101. (www)

  @article{ , abstract = {Negative thermal expansion (NTE) is an unusual yet highly useful phenomenon that has been extensively studied in numerous crystals, including ceramics, alloys, and metal-organic frameworks. This Letter reports an unprecedented NTE in an amorphous alloy that lacks a periodic atomic arrangement. Such an NTE is significant for metallic materials and extends over a wide temperature range ( , 200–375 K). We demonstrate that this NTE is intrinsic to the amorphous nature of the alloy and is correlated with Fe moment. Extended x-ray absorption fine structure reveals a strong NTE for nearest neighboring Fe-Fe pairs. Further analysis using a x-ray pair distribution function indicates that the amorphous alloy, serving as a transition state, exhibits a tendency toward local ordered atomic arrangement. A complex interplay among local structure, magnetic interaction, and thermal relaxation results in volume contraction upon heating below . This Letter introduces amorphous alloys as a new family of materials with NTE functionality, offering interesting prospects for both scientific research and practical applications.}, archive = {J_PRL}, author = {Ming Gao and Hankun Xu and Kun Lin and Andrea Sanson and Alessandro Venier and Alessandro Puri and Jochi Tseng and Guodong Li and Qian Zhang and Xuyu Dong and Yili Cao and Qiang Li and Xianran Xing}, doi = {10.1103/2g25-bdjx}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {106101}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent negative thermal expansion in amorphous fe-Y-zr-B alloys}, volume = {135}, year = {2025}, }
• (2025). Experimental evidence of stimulated raman rescattering in laser-plasma interaction. PRL, 135(10), 105101. (www)

  @article{ , abstract = {We present the first experimental evidence of stimulated Raman rescattering of a laser in plasma: The scattered light produced by the Raman instability is intense enough to scatter again through the same instability. Although never observed, rescattering processes have been studied theoretically and numerically for many years in the context of inertial confinement fusion, since the plasma waves they generate could bootstrap thermal electrons to high energies [B. J. Winjum et al. , Phys. Rev. Lett. 110 , 165001 (2013) ], preheating the fuel and degrading ignition conditions. Our experimental results are obtained with a spatially smoothed laser beam consisting of many speckles, with an average intensity around and close to in the speckles, such as those usually used in direct-drive inertial confinement fusion. Kinetic and hydrodynamic simulations show good agreement with the observations.}, archive = {J_PRL}, author = {J.-R. Marquès and F. Pérez and P. Loiseau and L. Lancia and C. Briand and S. Depierreux and M. Grech and C. Riconda}, doi = {10.1103/r7th-rq38}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {105101}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental evidence of stimulated raman rescattering in laser-plasma interaction}, volume = {135}, year = {2025}, }
• (2025). Sea ice aging by diffusion-driven desalination. PRL, 135(10), 104201. (www)

  @article{ , abstract = {Sea ice is a key component of Earth’s climate system, making its aging process an essential focus of current research. The age of sea ice is closely linked to its thermal and mechanical properties, which govern its interactions with the surrounding environment. In this study, we combine experimental techniques and modeling to explore the full dynamical process of mushy ice growth and spontaneous aging in saline water, within a natural convective flow system. We show that the aging of newly formed mushy ice in the present system, characterized by a gradual long-term reduction in porosity, is controlled by diffusion-driven desalination. Moreover, we observe that the system eventually transits into a dense freshwater ice layer adjacent to a well-mixed saline water region. The shape of the ice layer in this asymptotic state is well captured by numerical simulations of nonporous ice. Our findings improve the understanding of the complex physics governing phase changes in aqueous systems and provide a framework for studying sea ice aging in laboratory settings, with implications spanning diverse natural and industrial applications.}, archive = {J_PRL}, author = {Yihong Du and Feng Wang and Enrico Calzavarini and Chao Sun}, doi = {10.1103/mct1-6hbw}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {104201}, shortjournal = {Phys. Rev. Lett.}, title = {Sea ice aging by diffusion-driven desalination}, volume = {135}, year = {2025}, }
• (2025). Tricritical directed percolation controls the laminar-turbulent transition in pipes with body forces. PRL, 135(10), 104001. (www)

  @article{ , abstract = {The laminar-turbulent transition in straight pipes is believed to occur through a continuous nonequilibrium phase transition in the directed percolation universality class. However, in curved pipes or in the presence of body forces it is possible to observe a discontinuous transition and other phenomenology which seem inconsistent with the emerging consensus. Here, we consider the perturbing effects of body forces and incorporate them into a minimal Landau theory of the transition. We calculate the phase diagram as a function of Reynolds number and body force strength, and show that above a threshold strength of the latter, there is a tricritical point which accounts for the observed discontinuity behavior, including spatially heterogeneous states. Our results are consistent with recent experiments in centrifugal pipes and direct numerical simulations of heated flows.}, archive = {J_PRL}, author = {Guru K. Jayasingh and Nigel Goldenfeld}, doi = {10.1103/46g3-n7cx}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {104001}, shortjournal = {Phys. Rev. Lett.}, title = {Tricritical directed percolation controls the laminar-turbulent transition in pipes with body forces}, volume = {135}, year = {2025}, }
• (2025). Cavity QED based on strongly localized modes: Exponentially enhancing single-atom cooperativity. PRL, 135(10), 103602. (www)

  @article{ , abstract = {Large single-atom cooperativity in quantum systems is important for quantum information processing. Here, we propose to exponentially enhance the single-atom cooperativity parameter by exploiting the strongly localized effect of modes in cavity quantum electrodynamics (QED) systems. By increasing the wing width of a cavity with special geometry symmetry, the interference property allows us to exponentially improve the quality factor without altering the mode volume for cavities supporting subwavelength light modes. This effectively overcomes the trade-off between and in conventional subwavelength Fabry-Pérot cavities. Consequently, we demonstrate the occurrence of ultralong vacuum Rabi oscillations and the generation of strong photon blockade by enhancing the single-atom cooperativity parameter. This Letter offers a promising approach for advancing coherent manipulation and holds significant potential for applications in establishing longer-distance quantum communication networks, enhancing the precision and stability of quantum sensors, and improving the efficiency of quantum algorithms.}, archive = {J_PRL}, author = {Qian Bin and Ying Wu and Jin-Hua Gao and Aixi Chen and Franco Nori and Xin-You Lü}, doi = {10.1103/7frd-pf1m}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {103602}, shortjournal = {Phys. Rev. Lett.}, title = {Cavity QED based on strongly localized modes: Exponentially enhancing single-atom cooperativity}, volume = {135}, year = {2025}, }
• (2025). Atomic coherence of 2 minutes and instability of 1.5×10−18 at 1 s in a wannier-stark lattice clock. PRL, 135(10), 103601. (www)

  @article{ , abstract = {We explore the limits of atomic coherence and measurement precision in a optical lattice clock. We perform a detailed characterization of key effects, including lattice Raman scattering and atomic collisions in a shallow lattice configuration, determining a 174(28) s clock state lifetime. Investigation of atomic coherence across a range of lattice depths and atomic densities reveals decoherence mechanisms related to photon scattering and atomic interaction. At a reduced density, we observe a coherence time of 118(9) s, approaching the fundamental limit set by spontaneous emission. Guided by this coherence understanding, we demonstrate a clock instability for an atomic ensemble of at 1 s in fractional frequency units. Our results are important for further advancing the state of the art of an optical lattice clock for fundamental physics applications.}, archive = {J_PRL}, author = {Kyungtae Kim and Alexander Aeppli and William Warfield and Anjun Chu and Ana Maria Rey and Jun Ye}, doi = {10.1103/3wtv-sty2}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {103601}, shortjournal = {Phys. Rev. Lett.}, title = {Atomic coherence of 2 minutes and instability of 1.5×10−18 at 1 s in a wannier-stark lattice clock}, volume = {135}, year = {2025}, }
• (2025). Magnifying the wave function of interacting fermionic atoms. PRL, 135(10), 103401. (www)

  @article{ , abstract = {Understanding many body systems is a key challenge in physics. Single atom resolved imaging techniques have unlocked access to microscopic correlations in ultracold quantum gases. However they cannot be used when the relevant length scales are obscured by the resolution of the detection technique. We present a matter wave magnification scheme, based on evolutions in optical potentials, tailored to magnify the wave function of atoms, such that all length scales can be resolved. To showcase this method, we image atoms in the strongly interacting regime, establishing a new way to characterize correlated systems.}, archive = {J_PRL}, author = {Sandra Brandstetter and Carl Heintze and Paul Hill and Philipp M. Preiss and Maciej Gałka and Selim Jochim}, doi = {10.1103/wdjr-m2hg}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {103401}, shortjournal = {Phys. Rev. Lett.}, title = {Magnifying the wave function of interacting fermionic atoms}, volume = {135}, year = {2025}, }
• (2025). Leveraging resonant frequencies of an optical cavity for spectroscopic measurement of gas temperature and concentration. PRL, 135(10), 103201. (www)

  @article{ , abstract = {We introduce a spectroscopic approach to primary gas thermometry, harnessing precise optical cavity resonance frequencies and ab initio molecular line intensity calculations. By utilizing CO (3-0) vibrational band lines and cavity mode dispersion spectroscopy, we achieve an uncertainty of 82 ppm (24 mK at 296 K) in line intensity ratio thermometry—over an order of magnitude lower than any previously reported spectroscopic thermometry at gas pressures above 1.2 kPa. This method extends high-precision spectroscopic thermometry across a pressure range an order of magnitude larger than prior techniques, enabling a fully optical, noncontact, and molecule-selective primary amount-of-substance measurement. We further demonstrate sub-permille uncertainty in gas concentration measurements across pressures from 50 Pa to 20 kPa, significantly enhancing the precision and versatility of spectroscopic gas metrology.}, archive = {J_PRL}, author = {Daniel Lisak and Vittorio D’Agostino and Szymon Wójtewicz and Agata Cygan and Marcin Gibas and Piotr Wcisło and Roman Ciuryło and Katarzyna Bielska}, doi = {10.1103/2jz1-dr5l}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {103201}, shortjournal = {Phys. Rev. Lett.}, title = {Leveraging resonant frequencies of an optical cavity for spectroscopic measurement of gas temperature and concentration}, volume = {135}, year = {2025}, }
• (2025). Effect of incremental hydration on reverse internal conversion vibrational autodetachment of an anion. PRL, 135(10), 103001. (www)

  @article{ , abstract = {The recently discovered mechanism of reverse internal conversion vibrational autodetachment (RICVAD), by which an excess electron is emitted at specific energies from an isolated hot ground state anion, is mediated by the statistical population of a dipole-bound state. Here, we consider how this process is influenced by the presence of up to two water molecules. Using anion photoelectron imaging of the nitrobenzene radical anion, clustered to water molecules, we find that RICVAD remains active for . However, we also find that an additional decay channel opens at higher photoexcitation energies, which arises from dissociation of the cluster upon accessing an electronic resonance of , forming hot isolated , which then undergoes RICVAD. also shows evidence of RICVAD, but its signatures are obscured by other low energy electron signal. Our work shows that the RICVAD mechanism remains possible in a complex environment and shows how resonance dynamics are influenced by hydration.}, archive = {J_PRL}, author = {E. Michi Burrow and Connor J. Clarke and Jan R. R. Verlet}, doi = {10.1103/zfxx-8r4x}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {103001}, shortjournal = {Phys. Rev. Lett.}, title = {Effect of incremental hydration on reverse internal conversion vibrational autodetachment of an anion}, volume = {135}, year = {2025}, }
• (2025). Dilepton production from moaton quasiparticles. PRL, 135(10), 101904. (www)

  @article{ , abstract = {The phase diagram of QCD probably exhibits a moat regime over a large region of temperature and chemical potential . A moat regime is characterized by quasiparticle moatons (pions) whose energy is minimal at nonzero spatial momentum. At , higher mass dimension operators play a critical role in a moat regime. At dimension six, there are nine possible gauge-invariant couplings between scalars and photons. For back-to-back dilepton production, only one operator contributes, which significantly enhances production near a moat threshold. This enhancement is an experimental signature of moatons.}, archive = {J_PRL}, author = {Zohar Nussinov and Michael C. Ogilvie and Laurin Pannullo and Robert D. Pisarski and Fabian Rennecke and Stella T. Schindler and Marc Winstel}, doi = {10.1103/1f8w-p4m4}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101904}, shortjournal = {Phys. Rev. Lett.}, title = {Dilepton production from moaton quasiparticles}, volume = {135}, year = {2025}, }
• (2025). Elliptic leading singularities and canonical integrands. PRL, 135(10), 101903. (www)

  @article{ , abstract = {In the well-studied genus zero case, bases of d log integrands with integer leading singularities define Feynman integrals that automatically satisfy differential equations in canonical form. Such integrand bases can be constructed without input from the differential equations and without explicit involvement of dimensional regularization parameter . We propose a generalization of this construction to genus one geometry arising from the appearance of elliptic curves. We argue that a particular choice of algebraic 1-forms of the second kind that avoids derivatives is crucial. We observe that the corresponding Feynman integrals satisfy a special form of differential equations that has not been previously reported, and that their solutions order by order in yield pure functions. We conjecture that our integrand-level construction universally leads to such differential equations.}, archive = {J_PRL}, author = {E. Chaubey and V. Sotnikov}, doi = {10.1103/4fjc-lfnx}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101903}, shortjournal = {Phys. Rev. Lett.}, title = {Elliptic leading singularities and canonical integrands}, volume = {135}, year = {2025}, }
• (2025). String-breaking mechanism in a lattice schwinger model simulator. PRL, 135(10), 101902. (www)

  @article{ , abstract = {String breaking is a fundamental concept in gauge theories, describing the decay of a flux string connecting two charges through the production of particle–antiparticle pairs. This phenomenon is particularly important in particle physics, notably in quantum chromodynamics, and plays a crucial role in condensed matter physics. However, achieving a theoretical understanding of this nonperturbative effect is challenging, as conventional numerical approaches often fall short and require substantial computational resources. On the experimental side, studying these effects necessitates advanced setups, such as high-energy colliders, which makes direct observation difficult. Here, we report an experimental investigation of the string breaking mechanism in a one-dimensional U(1) lattice gauge theory using an optical lattice quantum simulator. By deterministically preparing initial states of varying lengths with fixed charges at each end, and adiabatically tuning the mass and string tension, we observed in situ microscopic confined phases that exhibit either string or broken-string states. Further analysis reveals that string breaking occurs under a resonance condition, leading to the creation of new particle–antiparticle pairs. These findings offer compelling evidence of string breaking and provide valuable insights into the intricate dynamics of lattice gauge theories. Our work underscores the potential of optical lattices as controllable quantum simulators, enabling the exploration of complex gauge theories and their associated phenomena.}, archive = {J_PRL}, author = {Ying Liu and Wei-Yong Zhang and Zi-Hang Zhu and Ming-Gen He and Zhen-Sheng Yuan and Jian-Wei Pan}, doi = {10.1103/mwy1-v9hk}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101902}, shortjournal = {Phys. Rev. Lett.}, title = {String-breaking mechanism in a lattice schwinger model simulator}, volume = {135}, year = {2025}, }
• (2025). Single-inclusive hadron production in electron-positron annihilation at next-to-next-to-next-to-leading order in QCD. PRL, 135(10), 101901. (www)

  @article{ , abstract = {Single-inclusive hadron production in electron-positron annihilation (SIA) represents the cleanest process for investigating the dynamics of parton hadronization, as encapsulated in parton fragmentation functions. In this Letter, we present, for the first time, the analytical computation of quantum chromodynamics corrections to the coefficient functions for SIA at next-to-next-to-next-to-leading order ( ) accuracy, achieving the highest precision to date for hadron production processes. Utilizing the BABAR measurement as a benchmark, we assess the phenomenological implications of this high-precision calculation. Our findings demonstrate a substantial reduction in scale uncertainties at and offer an improved description of the experimental data compared to lower-order calculations. This advancement underscores the importance of higher-order corrections in achieving a more accurate understanding of hadronization processes.}, archive = {J_PRL}, author = {Chuan-Qi He and Hongxi Xing and Tong-Zhi Yang and Hua Xing Zhu}, doi = {10.1103/vtz2-6bnm}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101901}, shortjournal = {Phys. Rev. Lett.}, title = {Single-inclusive hadron production in electron-positron annihilation at next-to-next-to-next-to-leading order in QCD}, volume = {135}, year = {2025}, }
• (2025). Measurement of the positive muon anomalous magnetic moment to 127 ppb. PRL, 135(10), 101802. (www)

  @article{ , abstract = {A new measurement of the magnetic anomaly of the positive muon is presented based on data taken from 2020 to 2023 by the Muon Experiment at Fermi National Accelerator Laboratory (FNAL). This dataset contains over 2.5 times the total statistics of our previous results. From the ratio of the precession frequencies for muons and protons in our storage ring magnetic field, together with precisely known ratios of fundamental constants, we determine (139 ppb) for the new datasets, and (127 ppb) when combined with our previous results. The new experimental world average, dominated by the measurements at FNAL, is (124 ppb). The measurements at FNAL have improved the precision on the world average by over a factor of 4.}, archive = {J_PRL}, author = {Muon g−2 Collaboration and D. P. Aguillard and T. Albahri and D. Allspach and J. Annala and K. Badgley and S. Baeßler and I. Bailey and L. Bailey and E. Barlas-Yucel and T. Barrett and E. Barzi and F. Bedeschi and M. Berz and M. Bhattacharya and H. P. Binney and P. Bloom and J. Bono and E. Bottalico and T. Bowcock and S. Braun and M. Bressler and G. Cantatore and R. M. Carey and B. C. K. Casey and D. Cauz and R. Chakraborty and A. Chapelain and S. Chappa and S. Charity and C. Chen and M. Cheng and R. Chislett and Z. Chu and T. E. Chupp and C. Claessens and F. Confortini and M. E. Convery and S. Corrodi and L. Cotrozzi and J. D. Crnkovic and S. Dabagov and P. T. Debevec and S. Di Falco and G. Di Sciascio and S. Donati and B. Drendel and A. Driutti and M. Eads and A. Edmonds and J. Esquivel and M. Farooq and R. Fatemi and K. Ferraby and C. Ferrari and M. Fertl and A. T. Fienberg and A. Fioretti and D. Flay and S. B. Foster and H. Friedsam and N. S. Froemming and C. Gabbanini and I. Gaines and S. Ganguly and J. George and L. K. Gibbons and A. Gioiosa and K. L. Giovanetti and P. Girotti and W. Gohn and L. Goodenough and T. Gorringe and J. Grange and S. Grant and F. Gray and S. Haciomeroglu and T. Halewood-Leagas and D. Hampai and F. Han and J. Hempstead and D. W. Hertzog and G. Hesketh and E. Hess and A. Hibbert and Z. Hodge and S. Y. Hoh and K. W. Hong and R. Hong and T. Hu and Y. Hu and M. Iacovacci and M. Incagli and S. Israel and P. Kammel and M. Kargiantoulakis and M. Karuza and J. Kaspar and D. Kawall and L. Kelton and A. Keshavarzi and D. S. Kessler and K. S. Khaw and Z. Khechadoorian and B. Kiburg and M. Kiburg and O. Kim and N. Kinnaird and E. Kraegeloh and K. R. Labe and J. LaBounty and M. Lancaster and S. Lee and B. Li and D. Li and L. Li and I. Logashenko and A. Lorente Campos and Z. Lu and A. Lucà and G. Lukicov and A. Lusiani and A. L. Lyon and B. MacCoy and R. Madrak and K. Makino and S. Mastroianni and R. McCarthy and J. P. Miller and S. Miozzi and B. Mitra and J. P. Morgan and W. M. Morse and J. Mott and A. Nath and J. K. Ng and H. Nguyen and Y. Oksuzian and Z. Omarov and W. Osar and R. Osofsky and S. Park and G. Pauletta and J. Peck and G. M. Piacentino and R. N. Pilato and K. T. Pitts and B. Plaster and D. Počanić and N. Pohlman and C. C. Polly and J. Price and B. Quinn and M. U. H. Qureshi and G. Rakness and S. Ramachandran and E. Ramberg and R. Reimann and B. L. Roberts and D. L. Rubin and M. Sakurai and L. Santi and C. Schlesier and A. Schreckenberger and Y. K. Semertzidis and A. K. Soha and M. Sorbara and J. Stapleton and D. Still and D. Stöckinger and C. Stoughton and D. Stratakis and H. E. Swanson and G. Sweetmore and D. A. Sweigart and M. J. Syphers and Y. Takeuchi and D. A. Tarazona and T. Teubner and A. E. Tewsley-Booth and V. Tishchenko and N. H. Tran and W. Turner and E. Valetov and D. Vasilkova and G. Venanzoni and T. Walton and A. Weisskopf and L. Welty-Rieger and P. Winter and Y. Wu and B. Yu and M. Yucel and E. Zaid and Y. Zeng and C. Zhang}, doi = {10.1103/7clf-sm2v}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101802}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of the positive muon anomalous magnetic moment to 127 ppb}, volume = {135}, year = {2025}, }
• (2025). Electroweak symmetry restoration and radiation amplitude zeros. PRL, 135(10), 101801. (www)

  @article{ , abstract = {In high-energy collisions far above the electroweak scale, the effects of electroweak symmetry breaking are expected to become parametrically small . This defines the extent to which the electroweak gauge symmetry is restored: (i) the physics of the transverse gauge bosons and fermions is described by a massless theory in the unbroken phase; (ii) the longitudinal gauge bosons behave like the Goldstone bosons and join the Higgs boson to restore the unbroken O(4) symmetry in the original Higgs sector. Using the unique feature of the radiation amplitude zeros in gauge theory, we propose to study the electroweak symmetry restoration quantitatively by examining the processes for the gauge boson pair production , and at the LHC and muon colliders.}, archive = {J_PRL}, author = {Rodolfo Capdevilla and Tao Han}, doi = {10.1103/sv5n-t5xm}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101801}, shortjournal = {Phys. Rev. Lett.}, title = {Electroweak symmetry restoration and radiation amplitude zeros}, volume = {135}, year = {2025}, }
• (2025). Localization of the m2-brane. PRL, 135(10), 101601. (www)

  @article{ , abstract = {We study quantum M2-branes in holographic backgrounds and show that their moduli spaces of zero modes are localized according to an R-symmetry Killing vector. We discuss the relation with recent results in the context of equivariant localization in gauged supergravity and argue its origin within M-theory path integrals expanded in saddle points over M2-branes. We argue that the M2-brane partition function, including its nonperturbative corrections, should be compared to the field theory grand canonical partition function. Our results extend recent observations in the context of the giant graviton expansion of superconformal indices to generic supersymmetric anti–de Sitter boundary conditions. As a byproduct we predict nonperturbative corrections to a variety of supersymmetric observables of the Aharony-Bergman-Jafferis-Maldacena theory.}, archive = {J_PRL}, author = {Friðrik Freyr Gautason and Jesse van Muiden}, doi = {10.1103/67bh-xd42}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101601}, shortjournal = {Phys. Rev. Lett.}, title = {Localization of the m2-brane}, volume = {135}, year = {2025}, }
• (2025). Broadband limits on stochastic length fluctuations from a pair of table-top interferometers. PRL, 135(10), 101402. (www)

  @article{ , abstract = {The Quantum-Enhanced Space-Time (QUEST) experiment consists of a pair of colocated power recycled Michelson interferometers, each designed to have a broadband, shot-noise-limited displacement sensitivity of from 1 to 200 MHz. Here, we present the first results of QUEST, with a search up to 80 MHz, that set new upper limits on correlated length fluctuations from 13 to 80 MHz, constituting the first broadband constraints for a stochastic gravitational wave background at these frequencies. In a coincident observing run of , the averaging of the cross-correlation spectra between the two interferometer signals resulted in a strain sensitivity of , making QUEST the most sensitive table-top interferometric system to date.}, archive = {J_PRL}, author = {Abhinav Patra and Lorenzo Aiello and Aldo Ejlli and William L. Griffiths and Alasdair L. James and Nikitha Kuntimaddi and Ohkyung Kwon and Eyal Schwartz and Henning Vahlbruch and Sander M. Vermeulen and Keiko Kokeyama and Katherine L. Dooley and Hartmut Grote}, doi = {10.1103/61j9-cjkk}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101402}, shortjournal = {Phys. Rev. Lett.}, title = {Broadband limits on stochastic length fluctuations from a pair of table-top interferometers}, volume = {135}, year = {2025}, }
• (2025). Unveiling the electrodynamic nature of spacetime collisions. PRL, 135(10), 101401. (www)

  @article{ , abstract = {Gravitational waves from merging binary black holes present exciting opportunities for understanding fundamental aspects of gravity, including nonlinearities in the strong-field regime. One challenge in studying and interpreting the dynamics of binary black hole collisions is the intrinsically geometrical nature of spacetime, which in many ways is unlike that of other classical field theories. By exactly recasting Einstein’s equations into a set of coupled nonlinear Maxwell equations closely resembling classical electrodynamics, we visualize the intricate dynamics of gravitational electric and magnetic fields during the inspiral, merger, and ringdown of a binary black hole collision.}, archive = {J_PRL}, author = {Siddharth Boyeneni and Jiaxi Wu and Elias R. Most}, doi = {10.1103/995s-wxl7}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101401}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling the electrodynamic nature of spacetime collisions}, volume = {135}, year = {2025}, }
• (2025). Scalar relics from the hot big bang. PRL, 135(10), 101003. (www)

  @article{ , abstract = {In this Letter, we motivate the fact that couplings between a scalar field and the standard model with strengths 10 − 6 ( m ϕ / eV ) − 1 / 4 relative to gravity yield the total measured cosmological dark matter abundance over a broad mass range of 10 − 12 to 10 14 eV . Remarkably, this result holds with minimal sensitivity to whether the scalar couples to electrons, photons, hadrons, or other particles at laboratory energy scales, thereby linking fifth force experiments to the search for dark matter.}, archive = {J_PRL}, author = {David Cyncynates and Olivier Simon}, doi = {10.1103/wjt8-9dh9}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101003}, shortjournal = {Phys. Rev. Lett.}, title = {Scalar relics from the hot big bang}, volume = {135}, year = {2025}, }
• (2025). Universal bound on the duration of a kination era. PRL, 135(10), 101002. (www)

  @article{ , abstract = {We show that primordial adiabatic curvature fluctuations generate an instability of the scalar field sourcing a kination era. We demonstrate that the generated higher Fourier modes constitute a radiationlike component dominating over the kination background after about 11 e-folds of cosmic expansion. Current constraints on the extra number of neutrino flavors thus imply the observational bound of approximately 10 e-folds, representing the most stringent bound to date on the stiffness of the equation of state of the pre–Big Bang–nucleosynthesis universe.}, archive = {J_PRL}, author = {Cem Eröncel and Yann Gouttenoire and Ryosuke Sato and Géraldine Servant and Peera Simakachorn}, doi = {10.1103/k7ty-gwjg}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101002}, shortjournal = {Phys. Rev. Lett.}, title = {Universal bound on the duration of a kination era}, volume = {135}, year = {2025}, }
• (2025). Ultralight dark matter statistics for pulsar timing detection. PRL, 135(10), 101001. (www)

  @article{ , abstract = {Fluctuations in ultralight dark matter produce significant metric perturbations, which may be detected by monitoring the arrival times of light from millisecond pulsars. While searches using this technique are already underway, they do not consistently account for the statistical properties of the dark matter field. The statistics of this field depend on the velocity dispersion of dark matter and, consequently, its coherence length. In the mass range relevant for pulsar timing arrays, the coherence length is comparable to separations between pulsars, making it crucial to incorporate its effects into the analysis. This Letter presents a consistent statistical method for gravitational direct detection of ultralight dark matter. Our key result is the derivation of the two-point function of the metric fluctuations, which we apply to pulsar timing and discuss its implementation in future searches.}, archive = {J_PRL}, author = {Kimberly K. Boddy and Jeff A. Dror and Austin Lam}, doi = {10.1103/hgnx-w1dn}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {101001}, shortjournal = {Phys. Rev. Lett.}, title = {Ultralight dark matter statistics for pulsar timing detection}, volume = {135}, year = {2025}, }
• (2025). Quantum metrology in the ultrastrong coupling regime of light-matter interactions: Leveraging virtual excitations without extracting them. PRL, 135(10), 100802. (www)

  @article{ , abstract = {Virtual excitations, inherent to ultrastrongly coupled light-matter systems, induce measurable modifications in system properties, offering a novel resource for quantum technologies. In this Letter, we demonstrate how these virtual excitations and their correlations can be harnessed to enhance precision measurements, without the need to extract them. Building on the paradigmatic Dicke model, which describes the interaction between an ensemble of two-level atoms and a single radiation mode, we propose a method to harness hybridized light-matter modes whose renormalized frequencies encode the effects of virtual excitations for quantum metrology. Remarkably, we find that, for a fixed squeezing parameter , exploiting virtual squeezing through oscillator frequency shifts yields a quadratic enhancement in estimation precision—scaling as —compared to the conventional scaling of real squeezed states. These results show that virtual excitations, though unobservable, can drive metrological performance beyond the standard quantum limit. Our approach establishes a broadly applicable framework for high-precision measurements across a wide class of ultrastrongly coupled quantum systems.}, archive = {J_PRL}, author = {Christoph Hotter and Adam Miranowicz and Karol Gietka}, doi = {10.1103/cxvs-5pb1}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {100802}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum metrology in the ultrastrong coupling regime of light-matter interactions: Leveraging virtual excitations without extracting them}, volume = {135}, year = {2025}, }
• (2025). Heisenberg-limited continuous-variable distributed quantum metrology with arbitrary weights. PRL, 135(10), 100801. (www)

  @article{ , abstract = {Distributed quantum metrology (DQM) enables the estimation of global functions of d distributed parameters beyond the capability of separable sensors. Continuous-variable DQM involves using a linear network with at least one nonclassical input. Here, we fully elucidate the structure of linear networks with two nonvacuum inputs, which allows us to prove a number of fundamental properties of continuous-variable DQM. While measuring the sum of d parameters at the Heisenberg limit can be achieved with a single nonvacuum input, we show that two inputs, one of which can be classical, are required to measure an arbitrary linear combination of d parameters and an arbitrary global function of the parameters. We obtain a universal and tight upper bound on the sensitivity of DQM networks with two inputs, and completely characterize the properties of the nonclassical input required to obtain a quantum advantage. This reveals that a wide range of nonclassical states makes this possible, including a squeezed vacuum. We also show that, for a class of nonclassical inputs, local photon number detection will achieve the maximum sensitivity. Finally we show that a general DQM network has two distinct regimes. The first achieves Heisenberg scaling. In the second the nonclassical input is much weaker than the coherent input, nevertheless providing a multiplicative enhancement to the otherwise classical sensitivity.}, archive = {J_PRL}, author = {Wenchao Ge and Kurt Jacobs}, doi = {10.1103/jkjj-3gvb}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {100801}, shortjournal = {Phys. Rev. Lett.}, title = {Heisenberg-limited continuous-variable distributed quantum metrology with arbitrary weights}, volume = {135}, year = {2025}, }
• (2025). Efficient computation of cumulant evolution and full counting statistics: Application to infinite temperature quantum spin chains. PRL, 135(10), 100401. (www)

  @article{ , abstract = {We propose a numerical method to efficiently compute quantum generating functions for a wide class of observables in one-dimensional quantum systems at high temperature. We obtain high-accuracy estimates for the cumulants and reconstruct full counting statistics from the quantum generating functions. We demonstrate its potential on spin anisotropic Heisenberg chain, where we can reach timescales hitherto inaccessible to state-of-the-art classical and quantum simulations. Our results challenge the conjecture of the Kardar-Parisi-Zhang universality for isotropic integrable quantum spin chains.}, archive = {J_PRL}, author = {Angelo Valli and Cătălin Paşcu Moca and Miklós Antal Werner and Márton Kormos and Žiga Krajnik and Tomaž Prosen and Gergely Zaránd}, doi = {10.1103/f3c4-n21z}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {100401}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient computation of cumulant evolution and full counting statistics: Application to infinite temperature quantum spin chains}, volume = {135}, year = {2025}, }
• (2025). Measurement incompatibility under loss. PRL, 135(10), 100202. (www)

  @article{ , abstract = {We investigate the measurement incompatibility of continuous-variable systems with infinite-dimensional Hilbert spaces under the influence of pure losses, a fundamental noise source in quantum optics, and a significant challenge for long-distance quantum communication. We show that loss channels with transmissivities less than make any set of measurements compatible. Additionally, we design a set of measurements that remains incompatible even under extreme losses, where the number of measurements in the set increases with the amount of loss. These measurements rely on on-off photodetectors and linear optics, making them feasible for implementation under realistic laboratory conditions. Furthermore, we demonstrate that no loss channel can break the incompatibility of all measurements. As a result, quantum steering remains achievable in the presence of pure loss.}, archive = {J_PRL}, author = {Mohammad Mehboudi and Fatemeh Rezaeinia and Saleh Rahimi-Keshari}, doi = {10.1103/s9sp-2fd7}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {100202}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement incompatibility under loss}, volume = {135}, year = {2025}, }
• (2025). Quantifying two-mode entanglement of bosonic gaussian states from their full counting statistics. PRL, 135(10), 100201. (www)

  @article{ , abstract = {We study the entanglement properties of two-mode bosonic Gaussian states based on their multi-mode counting statistics. We exploit the idea that measuring high-order correlations of particle numbers can reveal entanglement without making any assumptions about the coherence of the fields. We show that the two- and four-body number correlations are sufficient to fully characterize the entanglement of two-mode bosonic Gaussian states for which each mode exhibits a thermal distribution. In addition, we derive an entanglement witness based on two-body correlations alone. Our findings are of great importance because it becomes possible to reveal entanglement in a series of recent experiments.}, archive = {J_PRL}, author = {Victor Gondret and Clothilde Lamirault and Rui Dias and Charlie Leprince and Christoph I. Westbrook and David Clément and Denis Boiron}, doi = {10.1103/1y1p-zqhh}, journal = {Physical Review Letters}, month = {9}, number = {10}, pages = {100201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantifying two-mode entanglement of bosonic gaussian states from their full counting statistics}, volume = {135}, year = {2025}, }
• (2025). Reply to “Comment on aharonov-bohm phase is locally generated like all other quantum phases”. PRL, 135(9), 098902. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 098902 (2025)}, archive = {J_PRL}, author = {Chiara Marletto and Vlatko Vedral}, doi = {10.1103/rtwt-g7y7}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {098902}, shortjournal = {Phys. Rev. Lett.}, title = {Reply to “Comment on aharonov-bohm phase is locally generated like all other quantum phases”}, volume = {135}, year = {2025}, }
• (2025). Comment on “Aharonov-bohm phase is locally generated like all other quantum phases”. PRL, 135(9), 098901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 098901 (2025)}, archive = {J_PRL}, author = {Shan Gao}, doi = {10.1103/v117-v5wn}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {098901}, shortjournal = {Phys. Rev. Lett.}, title = {Comment on “Aharonov-bohm phase is locally generated like all other quantum phases”}, volume = {135}, year = {2025}, }
• (2025). Pseudogiant number fluctuations and nematic order in microswimmer suspensions. PRL, 135(9), 098302. (www)

  @article{ , abstract = {Giant number fluctuations (GNFs), whereby the standard deviation in the local number of particles grows faster than , are a hallmark property of dry active matter systems with orientational order, such as a collection of granular particles on a vibrated plate. This contrasts with momentum-conserving (“wet”) active matter systems, such as suspensions of swimming bacteria, where no theoretical prediction of GNFs exist, although numerous experimental observations of such enhanced fluctuations have been reported. In this Letter, we numerically confirm the emergence of super-Gaussian number fluctuations in a three-dimensional suspension of pusher microswimmers undergoing a transition to collective motion. These fluctuations emerge sharply above the transition, but only for sufficiently large values of the bacterial persistence length , where is the bacterial swimming speed and the tumbling rate. Crucially, these “pseudo-GNFs” differ from true GNFs, as they only occur on length scales shorter than the typical size of nematic patches in the collective motion state, which is in turn proportional to the single-swimmer persistence length . Our results thus suggest that observations of enhanced density fluctuations in biological active matter systems actually represent transient effects that decay away beyond mesoscopic length scales and raises the question to what extent “true” GNFs with universal properties can exist in the presence of fluid flows.}, archive = {J_PRL}, author = {Ismail El Korde and Dóra Bárdfalvy and Jason M. Lewis and Alexander Morozov and Cesare Nardini and Joakim Stenhammar}, doi = {10.1103/31q1-hj3n}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {098302}, shortjournal = {Phys. Rev. Lett.}, title = {Pseudogiant number fluctuations and nematic order in microswimmer suspensions}, volume = {135}, year = {2025}, }
• (2025). Cluster dynamics in macroscopic photoactive particles. PRL, 135(9), 098301. (www)

  @article{ , abstract = {We present an experimental study on the collective behavior of macroscopic self-propelled particles that are externally excited by light. This property allows for testing the system response to the excitation intensity in a very versatile manner. We discover that, for low excitation intensities, clustering at the boundaries is always present, even when this is prevented by implementing flower-shaped confining walls. For high excitation intensities, however, clusters are dissolved more or less easily depending on their size. Then, a thorough analysis of the cluster dynamics allows us to depict a phase diagram depending on the number of agents in the arena and the excitation intensity. To explain this, we introduce a simple kinetic model where cluster evolution is governed by a balance between adsorption and desorption processes. Interestingly, this simple model is able to reproduce the phase space observed experimentally.}, archive = {J_PRL}, author = {Sára Lévay and Axel Katona and Hartmut Löwen and Raúl Cruz Hidalgo and Iker Zuriguel}, doi = {10.1103/t7st-flj2}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {098301}, shortjournal = {Phys. Rev. Lett.}, title = {Cluster dynamics in macroscopic photoactive particles}, volume = {135}, year = {2025}, }
• (2025). Flow-driven stretch fluctuations govern the nonlinear viscoelasticity of elongating associative polymer networks. PRL, 135(9), 098101. (www)

  @article{ , abstract = {We use nonequilibrium molecular dynamics simulations to verify recent tube-model predictions that associative polymer networks exhibit broad stretch fluctuations during elongational flow. Simulations further show that these fluctuating dynamics give rise to the rate-dependent extensional viscosity η E measured in filament stretching experiments on H-bonding networks. Simulations model bivalent associative networks with a reactive bead-spring model for varying association strength and extensional strain rate. We observe that stretch fluctuations are driven by a new form of chain tumbling, where chains continually collapse and elongate as their associations break and reform within the advecting network. This produces a broad, nearly uniform distribution of chain stretch over a wide range of strain rates, manifesting as a rate-independent plateau in the extensional stress. Our results show that the nonlinear viscoelasticity of associative networks is dominated by large fluctuations in molecular response, which cannot be captured by current mean-field models.}, archive = {J_PRL}, author = {Songyue Liu and Thomas C. O’Connor}, doi = {10.1103/kgrd-8gkb}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {098101}, shortjournal = {Phys. Rev. Lett.}, title = {Flow-driven stretch fluctuations govern the nonlinear viscoelasticity of elongating associative polymer networks}, volume = {135}, year = {2025}, }
• (2025). Quantifying disorder in data. PRL, 135(9), 097401. (www)

  @article{ , abstract = {The quantification of disorder in data remains a fundamental challenge in science, as many phenomena yield short length datasets with order-disorder behavior, significant (un)correlated fluctuations, and indistinguishable characteristics even when arising from distinct natures, such as chaotic or stochastic processes. In this Letter, we propose a novel method to directly quantify disorder in data through recurrence microstate analysis, showing that maximizing this measure is essential for its optimal estimation. Our approach reveals that the disorder condition corresponds to the action of the symmetric group on recurrence space, producing classes of equiprobable recurrence microstates. By leveraging information entropy, we define a robust quantifier that reliably differentiates between chaotic, correlated, and uncorrelated stochastic signals even using just small time series. Additionally, it uncovers the characteristics of corrupting noise in dynamical systems. As an application, we show that disorder minima over time often align with well-known stage transitions of the Cenozoic era, indicating periods of dominant drivers in paleoclimatic data.}, archive = {J_PRL}, author = {João Vitor Vieira Flauzino and Thiago Lima Prado and Norbert Marwan and Jürgen Kurths and Sergio Roberto Lopes}, doi = {10.1103/1y98-x33s}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {097401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantifying disorder in data}, volume = {135}, year = {2025}, }
• (2025). Nonlinearity-induced fractional thouless pumping of solitons. PRL, 135(9), 097202. (www)

  @article{ , abstract = {Recent studies have shown that a soliton can be fractionally transported by slowly varying a system parameter over one period in a nonlinear system. This phenomenon is attributed to the nontrivial topology of the corresponding energy bands of a linear Hamiltonian. Here we find the occurrence of fractional Thouless pumping of solitons in a nonlinear off-diagonal Aubry-André-Harper model. Surprisingly, this happens despite the fact that all the energy bands of the linear Hamiltonian are topologically trivial, indicating that nonlinearity can induce fractional Thouless pumping of solitons. Specifically, our results show that a soliton can be pumped across one unit cell over one, two, three, or four pump periods, implying an average displacement of 1, or unit cells per cycle, respectively. We attribute these behaviors to changes in on-site potentials induced by a soliton solution, leading to the nontrivial topology for the modified linear Hamiltonian. Given that our model relies solely on varying nearest-neighbor hoppings, it is readily implementable on existing state-of-the-art photonic platforms.}, archive = {J_PRL}, author = {Yu-Liang Tao and Yongping Zhang and Yong Xu}, doi = {10.1103/96f5-qszj}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {097202}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinearity-induced fractional thouless pumping of solitons}, volume = {135}, year = {2025}, }
• (2025). Three strongly coupled kerr parametric oscillators forming a boltzmann machine. PRL, 135(9), 097201. (www)

  @article{ , abstract = {Coupled Kerr parametric oscillators (KPOs) are a promising resource for classical and quantum analog computation, for example to find the ground state of Ising Hamiltonians. Yet, the state space of strongly coupled KPO networks is very involved. As such, their phase diagram sometimes features either too few or too many states, including some that cannot be mapped to Ising spin configurations. This complexity makes it challenging to find and meet the conditions under which an analog optimization algorithm can be successful. Here, we demonstrate how to use three strongly coupled KPOs as a simulator for an Ising Hamiltonian, and estimate its ground state using a Boltzmann sampling measurement. While fully classical, our Letter is directly relevant for quantum systems operating on coherent states.}, archive = {J_PRL}, author = {Gabriel Margiani and Orjan Ameye and Oded Zilberberg and Alexander Eichler}, doi = {10.1103/npp4-b1xb}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {097201}, shortjournal = {Phys. Rev. Lett.}, title = {Three strongly coupled kerr parametric oscillators forming a boltzmann machine}, volume = {135}, year = {2025}, }
• (2025). Optimal control of levitated nanoparticles through finite-stiffness confinement. PRL, 135(9), 097102. (www)

  @article{ , abstract = {Optimal control of levitated nanoparticles subjected to thermal fluctuations is a challenging problem, both theoretically and experimentally. In this Letter, we compute the time-dependent harmonic confining potential that steers, in a prescribed time and with the minimum energetic cost, a Brownian particle between two assigned equilibrium states. We take full account of inertial effects, thus addressing the general underdamped dynamics, and, to address actual experimental conditions, the stiffness of the confining potential is required to be bounded. We carry out an experiment realizing the described protocol for an optically confined nanoparticle, which is shown to reach the target state within accuracy—while spending less energy than other protocols with the same duration, significantly shorter than the characteristic relaxation time. The results presented here are expected to have relevant applications in the design of optimal devices, such as engines at the nanoscale.}, archive = {J_PRL}, author = {Marco Baldovin and Ines Ben Yedder and Carlos A. Plata and Damien Raynal and Loïc Rondin and Emmanuel Trizac and Antonio Prados}, doi = {10.1103/pss4-b69w}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {097102}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal control of levitated nanoparticles through finite-stiffness confinement}, volume = {135}, year = {2025}, }
• (2025). Fluctuation-response inequalities for kinetic and entropic perturbations. PRL, 135(9), 097101. (www)

  @article{ , abstract = {We derive fluctuation-response inequalities for Markov jump processes that link the fluctuations of general observables to the response to perturbations in the transition rates within a unified framework. These inequalities are derived using the Cramér-Rao bound, enabling broader applicability compared to existing fluctuation-response relations formulated for static responses of currentlike observables. The fluctuation-response inequalities are valid for a wider class of observables and are applicable to finite observation times through dynamic responses. Furthermore, we extend these inequalities to open quantum systems governed by the Lindblad quantum master equation and find the quantum fluctuation-response inequality, where dynamical activity plays a central role.}, archive = {J_PRL}, author = {Euijoon Kwon and Hyun-Myung Chun and Hyunggyu Park and Jae Sung Lee}, doi = {10.1103/h45s-4118}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {097101}, shortjournal = {Phys. Rev. Lett.}, title = {Fluctuation-response inequalities for kinetic and entropic perturbations}, volume = {135}, year = {2025}, }
• (2025). Electrical control of ultrafast magnetic speeds in graphene spin field-effect junctions. PRL, 135(9), 097001. (www)

  @article{ , abstract = {We demonstrate ultrafast graphene spin-field-effect junctions, where gate-tunable superdiffusive spin currents across graphene-ferromagnet interfaces enable electric field control of magnetization dynamics in the ferromagnet. By electrostatically tuning the Fermi level in graphene underlying a cobalt thin film, we modulate the ultrafast spin transport across graphene-cobalt interfaces, reducing femtosecond laser-induced demagnetization time from 203 fs in bare cobalt thin films to 93 fs, a more than 100% increase in the rate of magnetization quenching. Supported by superdiffusive spin transport calculations, our findings unlock field-tunable magnetic speeds in devices, paving the way for innovations in subpicosecond spintronic memory-logic operations. Furthermore, this work creates new possibilities for electrical modulation of spin dynamics and ultrafast spin injection into two-dimensional quantum materials, with potential for next-generation quantum sensors and faster magnetic technologies.}, archive = {J_PRL}, author = {David Muradas-Belinchón and Suchetana Mukhopadhyay and Francesco Foggetti and Surya N. Panda and Olof Karis and Peter M. Oppeneer and Anjan Barman and M. Venkata Kamalakar}, doi = {10.1103/7ldk-csp9}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {097001}, shortjournal = {Phys. Rev. Lett.}, title = {Electrical control of ultrafast magnetic speeds in graphene spin field-effect junctions}, volume = {135}, year = {2025}, }
• (2025). Moiré-orbital-resolved excitonic mott insulating states and their optical and electric control in van der waals heterostructures. PRL, 135(9), 096902. (www)

  @article{ , abstract = {Moiré potential formed in van der Waals heterostructures is predicted to feature multiple local minima functioning as orbital degree of freedom, which is an important ingredient for understanding intriguing strong correlation phenomena. However, an experimental demonstration of this moiré-orbital enabled quantum state engineering is still unexplored. Here, we report clear evidence of moiré-orbital resolved excitonic Mott insulating states in multiannealing H-type heterobilayers and demonstrate their application in generating spatially ordered excitonic quantum phases. This moiré orbital is evidenced by interlayer exciton emissions with an energy separation of and further supported by our multiple field-dependent characterizations. Remarkably, the moiré orbital allows a sequential formation of correlated Mott insulating states, with the extracted onsite Hubbard interaction reaching . A combined optical and electric doping allows control of strongly correlated quantum phases with various spatially ordered fermionic-bosonic orbital components.}, archive = {J_PRL}, author = {Lanyu Huang and Cuihuan Ge and Boyi Xu and Yufan Wang and Siyao Li and Xinyi Luo and Haipeng Zhao and Danliang Zhang and Zhouxiaosong Zeng and Qingjun Tong and Dong Li and Xiaoli Zhu and Kai Braun and Tingge Gao and Xiao Wang and Anlian Pan}, doi = {10.1103/gg98-1vhp}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096902}, shortjournal = {Phys. Rev. Lett.}, title = {Moiré-orbital-resolved excitonic mott insulating states and their optical and electric control in van der waals heterostructures}, volume = {135}, year = {2025}, }
• (2025). Structural contribution to light-induced gap suppression in Ta2NiSe5. PRL, 135(9), 096901. (www)

  @article{ , abstract = {An excitonic insulator is a material that hosts an exotic ground state, where an energy gap opens due to spontaneous condensation of bound electron-hole pairs. is a promising candidate for this type of material, but the coexistence of a structural phase transition with the gap opening has led to a long-standing debate regarding the origin of the insulating gap. Here we employ MeV ultrafast electron diffraction to obtain quantitative insights into the atomic displacements in following photoexcitation, which has been overlooked in previous time-resolved spectroscopy studies. In conjunction with first-principles calculations using the measured atomic displacements, we find that the structural change can largely account for the photoinduced reduction in the energy gap without considering excitonic effects. Our Letter illustrates the importance of a quantitative reconstruction of individual atomic pathways during nonequilibrium phase transitions, paving the way for a mechanistic understanding of a diverse array of phase transitions in correlated materials where lattice dynamics can play a pivotal role.}, archive = {J_PRL}, author = {Zijing Chen and Chenhang Xu and Chendi Xie and Weichen Tang and Qiaomei Liu and Dong Wu and Qing Xu and Tao Jiang and Pengfei Zhu and Xiao Zou and Jun Li and Zhiwei Wang and Nanlin Wang and Dong Qian and Alfred Zong and Dao Xiang}, doi = {10.1103/1kzk-sz7g}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096901}, shortjournal = {Phys. Rev. Lett.}, title = {Structural contribution to light-induced gap suppression in Ta2NiSe5}, volume = {135}, year = {2025}, }
• (2025). Determining energy dispersion of spin excitations with scanning tunneling spectroscopy. PRL, 135(9), 096703. (www)

  @article{ , abstract = {Conventional methods to measure the dispersion relations of collective spin excitations involve probing bulk samples with particles such as neutrons, photons, or electrons, which carry a well-defined momentum. Open-ended finite-size spin chains, on the contrary, do not have a well-defined momentum due to the lack of translation symmetry, and their spin excitations are measured with an eminently local probe, using inelastic electron tunneling spectroscopy (IETS) with a scanning tunneling microscope (STM). Here, we discuss under what conditions STM-IETS spectra can be Fourier-transformed to yield dispersion relations in these systems. We relate the success of this approach to the degree to which spin excitations form standing waves. We show that STM-IETS can reveal the energy dispersion of magnons in ferromagnets and triplons in valence bond crystals, but not that of spinons, the spin excitations in Heisenberg spin- chains. We compare our theoretical predictions with state-of-the-art measurements on nanographene chains that realize the relevant spin Hamiltonians.}, archive = {J_PRL}, author = {J. C. G. Henriques and Chenxiao Zhao and G. Catarina and Pascal Ruffieux and Roman Fasel and J. Fernández-Rossier}, doi = {10.1103/n8jn-p468}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096703}, shortjournal = {Phys. Rev. Lett.}, title = {Determining energy dispersion of spin excitations with scanning tunneling spectroscopy}, volume = {135}, year = {2025}, }
• (2025). Signatures of fluctuation-driven magnetic topological charge in pt-ferromagnetic insulator bilayers. PRL, 135(9), 096702. (www)

  @article{ , abstract = {Chiral magnetic textures are of fundamental interest for studying exotic spin behavior, but also promising for the development of energy-efficient memory and logic devices. Recent computational work has suggested that in contrast to well-studied static chiral textures like skyrmions, there exists dynamic fluctuation-driven magnetic chirality even in the absence of long-range magnetic order. Here, we present definitive magnetotransport signatures of fluctuation-driven chirality in a model material system of (LAFO) bilayers, where LAFO is a ferromagnetic insulator. We establish a fluctuation-driven origin for the magnetic chirality by observing a strong correlation between the onset of the topological Hall effect and the destruction of magnetic order. Corroborated by Monte Carlo simulations, we develop a rigorous analytical framework to gain a first-principles understanding of scaling behaviors in the transport data. Our results bring novel insights to fluctuation-driven chirality and analysis of magnetotransport data.}, archive = {J_PRL}, author = {Sanyum Channa and Houssam Sabri and Xin Yu Zheng and Tian-Yue Chen and Haowen Ren and Qiuchen Wu and Kun Wang and Yuntian Li and Zbigniew Galazka and Ian R. Fisher and Xia Hong and Andrew D. Kent and Jiadong Zang and Yuri Suzuki}, doi = {10.1103/r5pw-sqk2}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096702}, shortjournal = {Phys. Rev. Lett.}, title = {Signatures of fluctuation-driven magnetic topological charge in pt-ferromagnetic insulator bilayers}, volume = {135}, year = {2025}, }
• (2025). Field-driven band asymmetry and nonreciprocal transport in a helimagnet. PRL, 135(9), 096701. (www)

  @article{ , abstract = {Helimagnets exhibit noncollinear spin arrangements characterized by a periodic helical modulation, giving rise to emergent chiral properties. These materials have attracted significant interest due to their potential applications in spintronics, particularly for robust information storage and the realization of topological spin textures such as skyrmions. In this work, we focus on Yoshimori-type helimagnets, where competing exchange interactions mediated by conduction electrons stabilize helical spin structures without requiring Dzyaloshinskii-Moriya interaction. We introduce a minimal model describing the electronic structure of a one-dimensional helimagnet in the presence of an external magnetic field and investigate its impact on nonreciprocal transport. We demonstrate how band asymmetry emerges in the conical phase induced by the external field, leading to a nonzero second-order electronic conductivity and injection photoconductivity. Our results provide insight into the interplay between the real space magnetic texture and electronic properties, paving the way for future studies on chirality-driven transport phenomena in centrosymmetric helimagnets.}, archive = {J_PRL}, author = {Darius-Alexandru Deaconu and Aneesh Agarwal and Rodion Vladimirovich Belosludov and Robert-Jan Slager and Mohammad Saeed Bahramy}, doi = {10.1103/lhj4-9h29}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096701}, shortjournal = {Phys. Rev. Lett.}, title = {Field-driven band asymmetry and nonreciprocal transport in a helimagnet}, volume = {135}, year = {2025}, }
• (2025). Observation of high-decay-rate topological corner states in diffusive thermal metamaterials. PRL, 135(9), 096604. (www)

  @article{ , abstract = {Effective thermal regulation is increasingly vital in numerous technological applications. The recent progress on topological diffusion in thermal materials offers promising potential. A distinct feature of diffusive systems is that their anti-Hermitian characteristics ensure purely imaginary eigenvalues representing decay rates, where higher decay rates imply better heat dissipation efficiency. Although research on higher-order topology has been extensive across various systems, investigations specifically of diffusive systems are just beginning. In particular, the few studies on the corner states are limited in their controllability. In this Letter, inspired by the concepts of the atomic p orbital and higher-orbital topology, we introduce multipolar thermal modes in the domain wall between two thermal kagome lattices to achieve multiple corner states. Diverging from traditional research on kagome lattices, we discovered higher-decay-rate corner states above the third band and linked their properties to multipolar modes localized at the domain wall. This approach not only enables higher-decay-rate corner states but also explores new dimensions of control over them. We theoretically identify and experimentally observe various corner states in a two-dimensional diffusive system. It is also demonstrated that simple thermal pulses can trigger transitions between different corner states, thereby dynamically enhancing the decay rate. This study further reveals the potential of topological approaches in heat dissipation, paving the way for the development of thermal management and related fields.}, archive = {J_PRL}, author = {Minghong Qi and Yanxiang Wang and Hongzhu Li and Pei-Chao Cao and Rui Xi and Xue-Feng Zhu and Fei Gao and Hongsheng Chen and Cheng-Wei Qiu and Ying Li}, doi = {10.1103/s97b-qcjc}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096604}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of high-decay-rate topological corner states in diffusive thermal metamaterials}, volume = {135}, year = {2025}, }
• (2025). Robustness of vacancy-bound non-abelian anyons in the kitaev model in a magnetic field. PRL, 135(9), 096603. (www)

  @article{ , abstract = {Non-Abelian anyons in quantum spin liquids (QSLs) provide a promising route to fault-tolerant topological quantum computation. In the exactly solvable Kitaev honeycomb model, such anyons of the QSL state can be bound to nonmagnetic spin vacancies and endowed with non-Abelian statistics by an infinitesimal magnetic field. Here, we investigate how this approach for stabilizing non-Abelian anyons extends to a finite magnetic field represented by a proper Zeeman term. Through large-scale density-matrix renormalization group simulations, we compute the vacancy-anyon binding energy as a function of magnetic field for both the ferromagnetic and antiferromagnetic Kitaev models. We find that anyon binding remains robust within the entire QSL phase for the ferromagnetic Kitaev model but breaks down already inside this phase for the antiferromagnetic Kitaev model. To compute a binding energy several orders of magnitude below the magnetic energy scale, we introduce both a refined definition and an extrapolation scheme based on carefully tailored perturbations.}, archive = {J_PRL}, author = {Bo Xiao and Gonzalo Alvarez and Gábor B. Halász}, doi = {10.1103/fl9b-4h4v}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096603}, shortjournal = {Phys. Rev. Lett.}, title = {Robustness of vacancy-bound non-abelian anyons in the kitaev model in a magnetic field}, volume = {135}, year = {2025}, }
• (2025). Probing k-space alternating spin polarization via the anomalous hall effect. PRL, 135(9), 096602. (www)

  @article{ , abstract = {Altermagnets represent a recently discovered class of collinear magnets, characterized by antiparallel neighboring magnetic moments and an alternating-sign spin polarization in momentum space ( k space). However, experimental methods for probing the k -space spin polarization in altermagnets remain limited. In this Letter, we propose an approach to address this challenge by interfacing an altermagnet with the surface of a topological insulator. We show that the altermagnet’s unique k -space spin polarization imprints a momentum-dependent, sign-alternating Dirac mass onto the otherwise massless surface states of the topological insulator, a direct consequence of breaking time-reversal symmetry. This engineered Dirac mass results in a unique, alternating half-quantized anomalous Hall effect. By measuring the Hall conductance, we can extract the local k -space magnetic moment. Moreover, we can map the global magnetic moment distribution by tuning the Dirac point position using an in-plane magnetic field, thereby revealing the k -space spin density of the altermagnet. This Letter establishes the Dirac fermion on the topological insulator surface as a sensitive probe for unveiling spin characters of altermagnets and those of other unconventional antiferromagnets.}, archive = {J_PRL}, author = {Rui Chen and Zi-Ming Wang and Ke Wu and Hai-Peng Sun and Bin Zhou and Rui Wang and Dong-Hui Xu}, doi = {10.1103/yrs7-m6zy}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096602}, shortjournal = {Phys. Rev. Lett.}, title = {Probing k-space alternating spin polarization via the anomalous hall effect}, volume = {135}, year = {2025}, }
• (2025). Non-hermitian origin of detachable boundary states in topological insulators. PRL, 135(9), 096601. (www)

  @article{ , abstract = {While topology can impose obstructions to exponentially localized Wannier functions, certain topological insulators are exempt from such Wannier obstructions. The absence of the Wannier obstructions can further accompany topological boundary states that are detachable from the bulk bands. Here, we elucidate a close connection between these detachable topological boundary states and non-Hermitian topology. Identifying Hermitian topological boundary states as non-Hermitian topology, we demonstrate that intrinsic non-Hermitian topology leads to the inevitable spectral flow. By contrast, we show that extrinsic non-Hermitian topology underlies the detachment of topological boundary states and clarify anti-Hermitian topology of the detached boundary states. Based on this connection and -theory, we complete the tenfold classification of Wannier localizability and detachable topological boundary states.}, archive = {J_PRL}, author = {Daichi Nakamura and Ken Shiozaki and Kenji Shimomura and Masatoshi Sato and Kohei Kawabata}, doi = {10.1103/q4nh-m1jh}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096601}, shortjournal = {Phys. Rev. Lett.}, title = {Non-hermitian origin of detachable boundary states in topological insulators}, volume = {135}, year = {2025}, }
• (2025). Nature of metallic and insulating domains in the charge-density-wave system 1T−TaSe2. PRL, 135(9), 096501. (www)

  @article{ , abstract = {We study the electronic structure of bulk in the charge-density wave phase at low temperature. Our spatially and angle-resolved photoemission data show insulating areas coexisting with metallic regions characterized by a chiral Fermi surface and moderately correlated quasiparticle bands. Additionally, high-resolution laser angle-resolved photoemission reveals variations in the metallic regions, with series of low-energy states, whose energy, number, and dispersion can be explained by the formation of quantum well states of different thicknesses. Dynamical mean field theory calculations show that the observed rich behavior can be rationalized by assuming occasional stacking faults of the charge density wave. Our results indicate that the diverse electronic phenomena reported previously in are dictated by the stacking arrangement and the resulting quantum size effects while correlation effects play a secondary role.}, archive = {J_PRL}, author = {M. Straub and F. Petocchi and C. Witteveen and F. B. Kugler and A. Hunter and Y. Alexanian and G. Gatti and S. Mandloi and C. Polley and G. Carbone and J. Osiecki and F. O. von Rohr and A. Georges and F. Baumberger and A. Tamai}, doi = {10.1103/pbyw-mzfy}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096501}, shortjournal = {Phys. Rev. Lett.}, title = {Nature of metallic and insulating domains in the charge-density-wave system 1T−TaSe2}, volume = {135}, year = {2025}, }
• (2025). Thermomodulated intrinsic josephson effect in kagome CsV3Sb5. PRL, 135(9), 096002. (www)

  @article{ , abstract = {Superconducting chiral domains associated with a time-reversal symmetry-breaking order parameter have garnered significant attention in kagome systems. In this Letter, we demonstrate both the intrinsic direct-current and alternating-current Josephson effects in the nanoplates of the vanadium-based kagome material CsV 3 Sb 5 , as evidenced by Fraunhofer-like patterns and Shapiro steps. Moreover, both the Fraunhofer-like patterns and Shapiro steps are modulated by thermal cycling, suggesting that the Josephson effects arise from dynamic superconducting domains. These findings may provide new insights into chiral superconductivity in CsV 3 Sb 5 and highlight the potential of these intrinsic Josephson junctions for applications in chiral superconductor-based quantum devices.}, archive = {J_PRL}, author = {Tian Le and Zhuokai Xu and Jinjin Liu and Ruiya Zhan and Zhiwei Wang and Xiao Lin}, doi = {10.1103/yqth-sfm8}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096002}, shortjournal = {Phys. Rev. Lett.}, title = {Thermomodulated intrinsic josephson effect in kagome CsV3Sb5}, volume = {135}, year = {2025}, }
• (2025). Evidence for the meissner effect in the nickelate superconductor La3Ni2O7−δ single crystal using diamond quantum sensors. PRL, 135(9), 096001. (www)

  @article{ , abstract = {Quantum sensing with nitrogen-vacancy (NV) centers in diamond enables the characterization of magnetic properties in the extreme situation of a tiny sample with defects. Recent studies have reported superconductivity in La 3 Ni 2 O 7 − δ under pressure, with zero resistance near 80 K, though the Meissner effect remains debated due to low superconducting volume fractions and limited high-pressure magnetic measurement techniques. In this work, we use diamond quantum sensors and four-probe detection to observe both zero resistance and the Meissner effect in the same La 3 Ni 2 O 7 − δ single crystal. By mapping the Meissner effect, we visualized superconducting regions and revealed sample inhomogeneities. Our combined magnetic and electrical measurements on the same crystal provide dual evidence of superconductivity, supporting the high-temperature superconductivity of La 3 Ni 2 O 7 − δ . This study also offers insights into its structural and magnetic properties under high pressure.}, archive = {J_PRL}, author = {Lin Liu and Jianning Guo and Deyuan Hu and Guizhen Yan and Yuzhi Chen and Lunxuan Yu and Meng Wang and Xiao-Di Liu and Xiaoli Huang}, doi = {10.1103/yvj7-htb4}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {096001}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for the meissner effect in the nickelate superconductor La3Ni2O7−δ single crystal using diamond quantum sensors}, volume = {135}, year = {2025}, }
• (2025). Unified phenomenology and test-particle simulations of ion heating in low-β plasmas. PRL, 135(9), 095201. (www)

  @article{ , abstract = {We argue that stochastic and resonant ion heating, often viewed as distinct processes in low- collisionless plasmas, are the far limits of a continuum controlled by nonlinear broadening of turbulent fluctuations, and thus by the normalized cross helicity. We propose a simple empirical formula that captures both regimes, generalizing the model commonly used to describe stochastic heating. Simulations of test ions interacting with turbulence confirm our scalings across a wide range of different ion and turbulence properties, including with a steep ion-kinetic transition range as seen in the solar wind. Our results provide a unified framework for understanding ion heating processes across diverse astrophysical environments from black-hole accretion disks to the solar corona, also providing a compact and versatile subgrid model for larger-scale simulations.}, archive = {J_PRL}, author = {Zade Johnston and Jonathan Squire and Romain Meyrand}, doi = {10.1103/rp85-hhg4}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {095201}, shortjournal = {Phys. Rev. Lett.}, title = {Unified phenomenology and test-particle simulations of ion heating in low-β plasmas}, volume = {135}, year = {2025}, }
• (2025). Analysis of the blowout plasma wakefields produced by drive beams with elliptical symmetry. PRL, 135(9), 095001. (www)

  @article{ , abstract = {In the underdense, or blowout regime, of plasma wakefield acceleration, the particle beam is denser than the plasma. In this scenario, the plasma electrons are nearly completely rarefied from the beam channel, leaving only a nominally uniform ion-filled “bubble.” Extensive investigations of this interaction assuming axisymmetry have been undertaken. However, the blowout produced by a transversely asymmetric (flat) driver, which would be present in linear collider “afterburner” schemes, possesses quite different characteristics. Such beams create an asymmetric plasma bubble which leads to unequal focusing in the two transverse dimensions, accompanied by a nonuniform accelerating gradient. The asymmetric blowout cross section is found through simulation to be elliptical, and treating it as such permits a simple extension of the symmetric theory. In particular, focusing fields linear in both transverse directions inside the bubble are found. The form of the wake potential and the associated beam-matching conditions in this elliptical cavity are discussed. We also examine blowout boundary estimation in the long driver limit and applications of the salient asymmetric features of the wakefield.}, archive = {J_PRL}, author = {P. Manwani and Y. Kang and J. Mann and B. Naranjo and G. Andonian and J. B. Rosenzweig}, doi = {10.1103/28c4-blhg}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {095001}, shortjournal = {Phys. Rev. Lett.}, title = {Analysis of the blowout plasma wakefields produced by drive beams with elliptical symmetry}, volume = {135}, year = {2025}, }
• (2025). Flowing menisci: Coupled dynamics and liquid exchange with soap films. PRL, 135(9), 094001. (www)

  @article{ , abstract = {Liquid foams exhibit menisci whose lengths range from hundreds of microns in microfoams to several centimeters in macroscopic bubble arrangements. These menisci are known to thin under gravity until reaching a steady thickness profile, where hydrostatic and capillary pressures are balanced. However, current drainage models neglect the liquid exchanges between the menisci and the adjacent soap films, assuming the latter provide a negligible liquid reservoir. Using controlled experiments, we systematically measure the shape of an isolated meniscus placed in a vertical soap film. By increasing the film thickness, we identify a flowing regime in which the flux from the film significantly enlarges the meniscus. We present an analytical model that extends the drainage equation to incorporate this dynamical effect and introduce a gravito-exchange length, which sets the minimum meniscus thickness. The model is in quantitative agreement with experiments, capturing the transition between hydrostatic and flowing menisci. This Letter has implications for flowing or rearranging foams, where thick films are commonly observed.}, archive = {J_PRL}, author = {Alexandre Vigna-Brummer and Antoine Monier and Isabelle Cantat and Christophe Brouzet and Christophe Raufaste}, doi = {10.1103/gfxm-67mm}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {094001}, shortjournal = {Phys. Rev. Lett.}, title = {Flowing menisci: Coupled dynamics and liquid exchange with soap films}, volume = {135}, year = {2025}, }
• (2025). Identifying and anticipating the threshold bifurcation of a complex laser with permutation entropy. PRL, 135(9), 093802. (www)

  @article{ , abstract = {The permutation entropy (PE) is a statistical indicator that allows the quantification of the complexity of a signal. Here, we show that it is able to identify and anticipate the threshold bifurcation of a complex laser, where thousands of modes compete for gain at the onset of lasing. In our experimental setup, the cavity round-trip time is several orders of magnitude longer than the temporal resolution of the detection system, which enables a high statistical sampling of the intensity dynamics per round trip. We show that the PE experiences a clear decrease far below the threshold and reaches a sharp minimum at the threshold bifurcation point, which reveals an abrupt increase of the temporal correlations. The evolution of the entropy is compared with standard quantifiers of approaching bifurcations. While lag-1 autocorrelation gradually grows as the threshold is approached, the PE shows a steep decrease that captures the emergence of nonlinear correlations and thus, it allows a clearer identification of the threshold.}, archive = {J_PRL}, author = {Juan Gancio and Cristina Masoller and Mathias Marconi}, doi = {10.1103/8lhf-51kv}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093802}, shortjournal = {Phys. Rev. Lett.}, title = {Identifying and anticipating the threshold bifurcation of a complex laser with permutation entropy}, volume = {135}, year = {2025}, }
• (2025). Self-injection locking dynamics with raman actions in aluminum nitride microresonators. PRL, 135(9), 093801. (www)

  @article{ , abstract = {Self-injection locking (SIL) of semiconductor lasers to on-chip microcavities enables significant laser noise purification and diverse nonlinear optical actions. Realizing nonlinear SIL in new material platforms is essential for advancing photonic integrated circuits. Here, we demonstrate nonlinear SIL in AlN microcavities that generates stimulated Raman lasers (SRLs) and microcombs. We achieve SRL emission with an output power exceeding 10 mW and a fundamental linewidth below 70 Hz in the 1750 nm band. The Kerr effect further mediates stimulated emissions at the second-Stokes and anti-Stokes frequencies. Multi-timescale thermal relaxations during turnkey SIL enable GHz-level frequency sweeps of the SRL and pump. Raman actions also render a Stokes platicon microcomb state with coemission in the pump and Stokes bands. Hybrid-integrated crystalline microresonators can be a versatile platform to investigate nonlinear photon-phonon interactions.}, archive = {J_PRL}, author = {Yulei Ding and Yifei Wang and Shunyu Yao and Yanan Guo and Jianchang Yan and Junxi Wang and Changxi Yang and Chengying Bao}, doi = {10.1103/pxqr-mps4}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093801}, shortjournal = {Phys. Rev. Lett.}, title = {Self-injection locking dynamics with raman actions in aluminum nitride microresonators}, volume = {135}, year = {2025}, }
• (2025). All-optical radio-frequency phase detection for rydberg atom sensors using oscillatory dynamics. PRL, 135(9), 093602. (www)

  @article{ , abstract = {Rydberg atom radio-frequency sensors are a unique platform for precision electromagnetic field measurement; e.g., they have extraordinary carrier bandwidth spanning MHz to THz and can be self-calibrated. These photonic sensors use lasers to prepare and read out the atomic response to a radio-frequency electromagnetic field. Most work on Rydberg atom sensors centers on radio-frequency electric field strength because the sensor functions as a square law detector, unless an external radio-frequency heterodyning field is used. A heterodyning field acts as a local oscillator and enables phase readout at the expense of the radio-frequency equipment necessary to generate it. In order to overcome the disadvantages of a radio-frequency local oscillator, we investigate all-optical phase-sensitive detection using a five-level closed-loop excitation scheme. We show that under finite detuning of the loop fields, the atomic response oscillates at the frequency of the detuning. The oscillation is transferred to a probe laser absorption signal. The phase, frequency, and amplitude of the radio-frequency signal are imprinted on the oscillatory dynamics and can be determined using demodulation and matched filter techniques applied to the probe laser transmission signal.}, archive = {J_PRL}, author = {Matthias Schmidt and Stephanie M. Bohaichuk and Vijin Venu and Ruoxi Wang and Harald Kübler and James P. Shaffer}, doi = {10.1103/23kb-7h7q}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093602}, shortjournal = {Phys. Rev. Lett.}, title = {All-optical radio-frequency phase detection for rydberg atom sensors using oscillatory dynamics}, volume = {135}, year = {2025}, }
• (2025). Incoherent measurement of a sub-10 kHz optical linewidth. PRL, 135(9), 093601. (www)

  @article{ , abstract = {Quantum state lifetimes T 2 , or equivalently homogeneous linewidths Γ h = 1 / π T 2 , are a key parameter for understanding decoherence processes in quantum systems and assessing their potential for applications in quantum technologies. The most common tool for measuring narrow optical homogeneous linewidths, i.e., long T 2 , is the measurement of coherent photon echo emissions, which however gives very weak signal when the number of emitters is small. This strongly hampers the development of nanomaterials, such as those based on rare earth ions, for quantum communication and processing. In this work, we propose, and demonstrate in an erbium doped crystal, a measurement of photon echoes based on incoherent fluorescence detection and its variance analysis. It gives access to T 2 through a much larger signal than direct photon echo detection, and, importantly, with a laser which is incoherent over the measurement timescale, on the order of a few T 2 . Our results thus open the way to efficiently assess the properties of a broad range of emitters and materials for applications in quantum nanophotonics.}, archive = {J_PRL}, author = {Félix Montjovet-Basset and Jayash Panigrahi and Diana Serrano and Alban Ferrier and Emmanuel Flurin and Patrice Bertet and Alexey Tiranov and Philippe Goldner}, doi = {10.1103/xkp5-v9m8}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093601}, shortjournal = {Phys. Rev. Lett.}, title = {Incoherent measurement of a sub-10 kHz optical linewidth}, volume = {135}, year = {2025}, }
• (2025). Observation of near-critical kibble-zurek scaling in rydberg atom arrays. PRL, 135(9), 093403. (www)

  @article{ , abstract = {The Kibble-Zurek scaling reveals the universal dynamics when a system is linearly ramped across a symmetry-breaking phase transition. However, in reality, inevitable finite-size effects or symmetry-breaking perturbations can often smear out the critical point and render the phase transition into a smooth crossover. In this Letter, we show experimentally that the precise Kibble-Zurek scaling can be retained in the near-critical crossover regime, not necessarily crossing the critical point strictly. The key ingredient to achieving this near-critical Kibble-Zurek scaling is that the system size and the symmetry-breaking field must be appropriately scaled following the variation of ramping speeds. The experiment is performed in a reconfigurable Rydberg atom array platform, where the Rydberg blockade effect induces a symmetry-breaking transition. The atom array platform enables precise control of the system size and the zigzag geometry as a symmetry-breaking field. Therefore, we can demonstrate notable differences in the precision of the Kibble-Zurek scaling with or without properly scaling the system size and the zigzag geometry. Our results strengthen the Kibble-Zurek scaling as an increasingly valuable tool for investigating phase transition in quantum simulation platforms.}, archive = {J_PRL}, author = {Tao Zhang and Hanteng Wang and Wenjun Zhang and Yuqing Wang and Angrui Du and Ziqi Li and Yujia Wu and Chengshu Li and Jiazhong Hu and Hui Zhai and Wenlan Chen}, doi = {10.1103/2gwz-65w1}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093403}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of near-critical kibble-zurek scaling in rydberg atom arrays}, volume = {135}, year = {2025}, }
• (2025). Cavity-enabled real-time observation of individual atomic collisions. PRL, 135(9), 093402. (www)

  @article{ , abstract = {Using the strong dispersive coupling to a high-cooperativity cavity, we demonstrate fast and nondestructive number-resolved detection of atoms in optical tweezers. We observe individual atom-atom collisions, quantum state jumps, and atom loss events with a time resolution of through continuous measurement of cavity transmission. Using adaptive feedback control in combination with the nondestructive measurements, we further prepare a single atom with 92(2)% probability.}, archive = {J_PRL}, author = {Matthew L. Peters and Guoqing Wang (王国庆 and David C. Spierings and Niv Drucker and Beili Hu and Meng-Wei Chen and Yu-Ting Chen and Vladan Vuletić}, doi = {10.1103/941q-5sdq}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093402}, shortjournal = {Phys. Rev. Lett.}, title = {Cavity-enabled real-time observation of individual atomic collisions}, volume = {135}, year = {2025}, }
• (2025). Vortex nucleations in spinor bose condensates under localized synthetic magnetic fields. PRL, 135(9), 093401. (www)

  @article{ , abstract = {Gauge fields are ubiquitous in modern quantum physics. In superfluids, quantized vortices can be induced by gauge fields. Here we demonstrate the first experimental observation of vortex nucleations in light-dressed spinor Bose-Einstein condensates under radially localized synthetic magnetic fields. The light-induced spin-orbital-angular-momentum coupling creates azimuthal gauge potentials for the lowest-energy spinor branch dressed eigenstate. The observation of the atomic wave function in the lowest-energy dressed eigenstate reveals that vortices nucleate from the cloud center of a vortex-free state with canonical momentum . This is because a large circulating azimuthal velocity field at the condensate center results in a dynamically unstable localized excitation that initiates vortex nucleations. Furthermore, the long-time dynamics to reach the ground state stops in a metastable state when is not sufficiently large. Our observation has reasonable agreement with the time-dependent Gross-Pitaevskii simulations.}, archive = {J_PRL}, author = {L.-R. Liu and S.-C. Wu and T.-W. Liu and H.-Y. Hsu and T.-K. Shen and S.-K. Yip and Y. Kawaguchi and Y.-J. Lin}, doi = {10.1103/zj34-15bk}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093401}, shortjournal = {Phys. Rev. Lett.}, title = {Vortex nucleations in spinor bose condensates under localized synthetic magnetic fields}, volume = {135}, year = {2025}, }
• (2025). Finding the ultranarrow P32→P30 electric quadrupole transition in ni12+ ion for an optical clock. PRL, 135(9), 093002. (www)

  @article{ , abstract = {The ion features an electronic transition with a natural width of only 8 mHz, allowing for a highly stable optical clock. We predict that the energy of this strongly forbidden electric quadrupole transition is . For this, we use both a hybrid approach combining configuration interaction with a coupled-cluster method and a pure configuration interaction calculation for the complete 16-electron system, ensuring convergence. The resulting very small theoretical uncertainty of only 0.05% allowed us to find the transition experimentally in a few hours, yielding an energy of . This level of agreement for a 16-electron system is unprecedented and qualifies our method for future calculations of many other complex atomic systems. While paving the way for a high-precision optical clock based on , our theory and code development will also enable better predictions for other highly charged ions and other complex atomic systems.}, archive = {J_PRL}, author = {Charles Cheung and Sergey G. Porsev and Dmytro Filin and Marianna S. Safronova and Malte Wehrheim and Lukas J. Spieß and Shuying Chen and Alexander Wilzewski and José R. Crespo López-Urrutia and Piet O. Schmidt}, doi = {10.1103/flwf-c2m1}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093002}, shortjournal = {Phys. Rev. Lett.}, title = {Finding the ultranarrow P32→P30 electric quadrupole transition in ni12+ ion for an optical clock}, volume = {135}, year = {2025}, }
• (2025). Amplification of spontaneous emission from doubly excited he atoms. PRL, 135(9), 093001. (www)

  @article{ , abstract = {We have observed amplification of weak fluorescence from He atoms in the 3a P o 1 autoionizing state, which decay by spontaneous emission of 40.74 eV photons in one out of 1600 cases. On average, a 4.1 ± 1.6 % conversion of 63.67 eV photons was detected in the forward direction at 20 μ J pump pulse energy and 40 mbar He gas pressure. A comparison with state-of-the-art theoretical simulations shows an unexpected spectral line shift at high gas pressure that is ascribed to transient molecular and electron scattering effects.}, archive = {J_PRL}, author = {J. Turnšek and Š. Krušič and A. Mihelič and K. Bučar and L. Foglia and R. Mincigrucci and M. Krstulović and M. Coreno and G. Bonano and K. C. Prince and C. Callegari and A. Simoncig and Z. Ebrahimpour and E. Paltanin and A. Benediktovitch and R. Osellame and A. G. Ciriolo and R. Martínez Vázquez and C. Vozzi and E. Principi and M. Žitnik}, doi = {10.1103/mg5s-xvct}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {093001}, shortjournal = {Phys. Rev. Lett.}, title = {Amplification of spontaneous emission from doubly excited he atoms}, volume = {135}, year = {2025}, }
• (2025). Observation of the charged-particle multiplicity dependence of σψ(2S)/σJ/ψ in p-pb collisions at 8.16 TeV. PRL, 135(9), 092301. (www)

  @article{ , abstract = {Bound states of charm and anticharm quarks, known as charmonia, have a rich spectroscopic structure that can be used to probe the dynamics of hadron production in high-energy hadron collisions. Here, the cross section ratio of excited and ground state vector mesons is measured as a function of the charged-particle multiplicity in proton-lead ( ) collisions at a center-of-mass (CM) energy per nucleon pair of 8.16 TeV. The data corresponding to an integrated luminosity of were collected using the CMS detector. The ratio is measured separately for prompt and nonprompt charmonia in the transverse momentum range and in four rapidity ranges spanning . For the first time, a statistically significant multiplicity dependence of the prompt cross section ratio is observed in proton-nucleus collisions. There is no clear rapidity dependence in the ratio. The prompt measurements are compared with a theoretical model which includes interactions with nearby particles during the evolution of the system. These results provide additional constraints on hadronization models of heavy quarks in nuclear collisions.}, archive = {J_PRL}, author = {CMS Collaboration and V. Chekhovsky and A. Hayrapetyan and V. Makarenko and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and H. Kwon and T. Van Laer and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and Y. Hong and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and A. Khalilzadeh and F. A. Khan and K. Lee and A. Malara and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and J. Knolle and L. Lambrecht and D. Marckx and K. Mota Amarilo and K. Skovpen and N. Van Den Bossche and J. van der Linden and L. Wezenbeek and S. Bein and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and S. Turkcapar and G. A. Alves and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and E. J. Tonelli Manganote and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and T. Laux Kuhn and M. Macedo and J. Martins and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and D. Laroze and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and H. Wang and K. Yi and J. Zhang and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and J. Jaramillo and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and H. Abdalla and Y. Assran and B. El-mahdy and M. Abdullah Al-Mashad and M. A. Mahmoud and K. Ehataht and M. Kadastik and T. Lange and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and K. Osterberg and M. Voutilainen and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Myllymäki and M. m. Rantanen and J. Tuominiemi and H. Kirschenmann and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and A. Cappati and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Nguyen and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and G. Sokmen and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and G. Adamov and I. Lomidze and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and D. Noll and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and A. Cardini and F. Colombina and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and S. Zakharov and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and T. Chwalek and A. Dierlamm and G. G. Dincer and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and O. Lavoryk and J. M. Lawhorn and M. Link and A. Lintuluoto and S. Maier and S. Mitra and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and B. Topko and N. Trevisani and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and G. Melachroinos and Z. Painesis and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and P. Major and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Baradia and S. Barman and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and T. Mishra and B. Parida and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and S. Bhowmik and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and B. M. Joshi and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and K. Naskar and A. Nayak and S. Nayak and K. Pal and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and D. Bisello and P. Bortignon and G. Bortolato and A. Bragagnolo and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and F. Gasparini and S. Giorgetti and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and F. Montecassiano and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and V. K. Muraleedharan Nair Bindhu and M. Musich and S. Nandan and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and P. Barria and C. Basile and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and R. Gargiulo and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and J. Yoo and J. Goh and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and K. Hwang and B. Kim and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and C. A. Mondragon Herrera and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and F. E. Neri Huerta and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and A. Bellora and L. Forthomme and L. Grzanka and M. Malawski and K. Piotrzkowski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and M. Stojanovic and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and C. Martin Perez and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and E. Palencia Cortezon and J. Prado Pico and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and A. A. Bin Anuar and A. Bocci and L. Borgonovi and C. Botta and E. Brondolin and C. E. Brown and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and G. Karathanasis and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and M. Magherini and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and Y. Maghrbi and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and Y. Komurcu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and E. Uslan and I. S. Zorbakir and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and V. J. Smith and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and O. Buchmuller and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and V. Hegde and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and C. Cosby and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and L. Gouskos and M. Hadley and U. Heintz and K. W. Ho and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and J. Luo and S. Mondal and T. Russell and S. Sagir and X. Shen and M. Stamenkovic and N. Venkatasubramanian and S. Abbott and B. Barton and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and S. Yoo and F. Zhang and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and D. Primosch and M. Quinnan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and M. M. Hussain and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and X. Yan and D. Zhang and A. Bornheim and O. Cerri and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and N. Manganelli and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and X. Chen and D. J. Cranshaw and J. Dickinson and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and I. Dutta and V. D. Elvira and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and K. Maeshima and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and T. Roy and S. Rudrabhatla and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Wang and L. Zhang and C. Baldenegro Barrera and J. Bendavid and S. Bright-Thonney and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and A. Rohilla and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and P. Levchenko and J. Li and M. Lu and R. Mccarthy and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and E. Tsai and D. Wood and S. Dittmer and K. A. Hahn and D. Li and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and F. Simpson and D. Stickland and C. Tully and L. H. Vage and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and V. Scheurer and J. F. Schulte and A. K. Virdi and F. Wang and A. Wildridge and W. Xie and Y. Yao and J. Dolen and N. Parashar and A. Pathak and D. Acosta and A. Agrawal and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and I. Krommydas and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and J. Reichert and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and A. Safonov and N. Akchurin and J. Damgov and Y. Feng and N. Gogate and Y. Kazhykarim and K. Lamichhane and C. Madrid and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and D. Rathjens and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Mantilla and C. Neu and C. Ramón Álvarez and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and D. Budkouski and I. Golutvin and I. Gorbunov and V. Karjavine and O. Kodolova and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and A. Nikitenko and V. Palichik and V. Perelygin and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and V. Smirnov and O. Teryaev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and Yu. Andreev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and I. Tlisova and A. Toropin and T. Aushev and K. Ivanov and V. Gavrilov and N. Lychkovskaya and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and A. Ershov and A. Gribushin and A. Kaminskiy and L. Khein and V. Korotkikh and S. Obraztsov and S. Petrushanko and V. Savrin and A. Snigirev and I. Vardanyan and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and Y. Skovpen and V. Kachanov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin}, doi = {10.1103/c9wp-5tq3}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {092301}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of the charged-particle multiplicity dependence of σψ(2S)/σJ/ψ in p-pb collisions at 8.16 TeV}, volume = {135}, year = {2025}, }
• (2025). Longitudinal short-distance constraints on hadronic light-by-light scattering and tensor-meson contributions to the muon g−2. PRL, 135(9), 091901. (www)

  @article{ , abstract = {Short-distance constraints from the operator product expansion in QCD play an important role in the evaluation of the hadronic light-by-light scattering contribution to the anomalous magnetic moment of the muon. Holographic QCD has been shown to naturally incorporate the Melnikov-Vainshtein constraint on the longitudinal amplitude following from the triangle anomaly in the asymmetric limit, where one photon virtuality remains small compared to the others. This is saturated by an infinite tower of axial vector mesons, and their numerical contribution to the muon in AdS/QCD models agrees rather well with a recent dispersive analysis. However, in AdS/QCD, the longitudinal short-distance constraint where all virtualities are large turns out to be matched only at the level of 81%. In this Letter we show that tensor mesons, whose contribution to the muon has recently been found to be underestimated, can fill this gap because in holographic QCD their infinite tower of excited mesons only contributes to the symmetric longitudinal short-distance constraint. Numerically, they give rise to a sizeable positive contribution from the low-energy region below 1.5 GeV, a small one from the mixed region, and a negligible one from the high-energy region, which could explain the remaining gap between the most recent dispersive and lattice results for the complete hadronic light-by-light contribution.}, archive = {J_PRL}, author = {Jonas Mager and Luigi Cappiello and Josef Leutgeb and Anton Rebhan}, doi = {10.1103/dxwr-gpsl}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091901}, shortjournal = {Phys. Rev. Lett.}, title = {Longitudinal short-distance constraints on hadronic light-by-light scattering and tensor-meson contributions to the muon g−2}, volume = {135}, year = {2025}, }
• (2025). Axion dark matter search with sensitivity near the kim-shifman-vainshtein-zakharov benchmark using the TM020 mode. PRL, 135(9), 091804. (www)

  @article{ , abstract = {Axions, originally proposed to resolve the problem in the strong interaction, remain a leading dark matter candidate. While cavity haloscopes offer the most sensitive technique for detecting axions, searches have largely been limited to masses below . We report a sensitive search for axion dark matter with masses around , utilizing the mode of a cylindrical cavity equipped with an innovative tuning mechanism. Our search achieved a sensitivity of the Kim-Shifman-Vainshtein-Zakharov benchmark over a 100-MHz range, representing a significant advance in this mass range. These results demonstrate that higher-order modes provide a viable strategy for extending haloscope searches into previously unexplored higher-mass regions.}, archive = {J_PRL}, author = {Sungjae Bae and Junu Jeong and Younggeun Kim and SungWoo Youn and Jinsu Kim and Arjan F. van Loo and Yasunobu Nakamura and Seonjeong Oh and Taehyeon Seong and Sergey Uchaikin and Jihn E. Kim and Yannis K. Semertzidis}, doi = {10.1103/f11t-qy8z}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091804}, shortjournal = {Phys. Rev. Lett.}, title = {Axion dark matter search with sensitivity near the kim-shifman-vainshtein-zakharov benchmark using the TM020 mode}, volume = {135}, year = {2025}, }
• (2025). Muon colliders and the neutrino slice. PRL, 135(9), 091803. (www)

  @article{ , abstract = {Muon colliders provide an exciting new direction to expand the energy frontier of particle physics. We point out a new use of these facilities for neutrino and beyond the standard model physics using their main detectors. Muon decays along the accelerator rings create an intense and highly collimated neutrino beam that crosses a thin slice of the kt-scale detector. As a result, it would induce an unprecedented number of neutrino interactions, with O ( 10 4 ) events per second for a 10 TeV μ + μ − collider. These interactions are highly energetic and possess a distinct timing signature and a large transverse displacement. We discuss promising applications of these events for instrumentation, electroweak, and beyond-the-standard model physics. For instance, a subpercent measurement of the neutrino-electron scattering rate enables new precision measurements of the Weak angle and a novel detection of the neutrino charge radius.}, archive = {J_PRL}, author = {Luc Bojorquez-Lopez and Matheus Hostert and Carlos A. Argüelles and Zhen Liu}, doi = {10.1103/4sj1-ycft}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091803}, shortjournal = {Phys. Rev. Lett.}, title = {Muon colliders and the neutrino slice}, volume = {135}, year = {2025}, }
• (2025). Measurement of WWZ and ZH production cross sections at s=13 and 13.6 TeV. PRL, 135(9), 091802. (www)

  @article{ , abstract = {A measurement is presented of the cross section in proton-proton collisions for the production of two bosons and one boson. It is based on data recorded by the CMS experiment at the CERN LHC at center-of-mass energies and 13.6 TeV, corresponding to an integrated luminosity of . Events with four charged leptons (electrons or muons) in the final state are selected. Both nonresonant production and production, with the Higgs boson decaying into two bosons, are reported. For the first time, the two processes are measured separately in a simultaneous fit. Combining the two modes, signal strengths relative to the standard model (SM) predictions of and are measured for and 13.6 TeV, respectively. The observed (expected) significance for the triboson signal is 3.8 (2.5) standard deviations for , thus providing the first evidence for triboson production at this center-of-mass energy. Combining the two modes and the two center-of-mass energies, the inclusive signal strength relative to the SM prediction is measured to be , with an observed (expected) significance of 4.5 (5.0) standard deviations.}, archive = {J_PRL}, author = {CMS Collaboration and A. Hayrapetyan and V. Makarenko and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and K. Damanakis and M. Dragicevic and C. Giordano and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Shooshtari and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and H. Kwon and D. Ocampo Henao and T. Van Laer and P. Van Mechelen and J. Bierkens and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and Y. Hong and P. Kashko and S. Lowette and I. Makarenko and D. Müller and J. Song and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and A. Khalilzadeh and F. A. Khan and A. Malara and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and F. Zhang and M. De Coen and D. Dobur and G. Gokbulut and J. Knolle and L. Lambrecht and D. Marckx and K. Skovpen and N. Van Den Bossche and J. van der Linden and J. Vandenbroeck and L. Wezenbeek and S. Bein and A. Benecke and A. Bethani and G. Bruno and A. Cappati and J. De Favereau De Jeneret and C. Delaere and A. Giammanco and A. O. Guzel and V. Lemaitre and J. Lidrych and P. Malek and P. Mastrapasqua and S. Turkcapar and G. A. Alves and M. Barroso Ferreira Filho and E. Coelho and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and E. J. Tonelli Manganote and A. Vilela Pereira and W. L. Aldá Júnior and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and M. Costa Reis and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and S. S. Jesus and T. Laux Kuhn and M. Macedo and K. Mota Amarilo and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and F. Torres Da Silva De Araujo and C. A. Bernardes and T. R. Fernandez Perez Tomei and E. M. Gregores and B. Lopes Da Costa and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and V. Scheurer and A. Aleksandrov and G. Antchev and P. Danev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and S. Keshri and D. Laroze and S. Thakur and W. Brooks and T. Cheng and T. Javaid and L. Wang and L. Yuan and Z. Hu and Z. Liang and J. Liu and X. Wang and G. M. Chen and H. S. Chen and M. Chen and Y. Chen and Q. Hou and X. Hou and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and G. Liu and Z.-A. Liu and J. N. Song and S. Song and J. Tao and C. Wang and J. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and Q. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and M. Zhang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and H. Wang and K. Yi and J. Zhang and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and Y. Assran and B. El-mahdy and M. Abdullah Al-Mashad and A. Hussein and H. Mohammed and K. Ehataht and M. Kadastik and T. Lange and C. Nielsen and J. Pata and M. Raidal and N. Seeba and L. Tani and A. Milieva and K. Osterberg and M. Voutilainen and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and R. Kumar Verma and T. Lampén and K. Lassila-Perini and B. Lehtela and S. Lehti and T. Lindén and N. R. Mancilla Xinto and M. Myllymäki and M. m. Rantanen and S. Saariokari and N. T. Toikka and J. Tuominiemi and H. Kirschenmann and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and P. Devouge and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and S. Ronchi and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and T. Debnath and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and L. Kalipoliti and M. Manoni and M. Nguyen and S. Obraztsov and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and G. Sokmen and L. Urda Gómez and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and G. Coulon and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd’huy and I. B. Laktineh and M. Lethuillier and B. Massoteau and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and J. Xiao and A. Khvedelidze and I. Lomidze and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and P. Nattland and V. Oppenländer and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and C. Daumann and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and N. Kumar and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and F. Nowotny and A. Pozdnyakov and W. Redjeb and H. Reithler and U. Sarkar and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and V. Vaulin and S. Zaleski and M. R. Beckers and C. Dziwok and G. Flügge and N. Hoeflich and T. Kress and A. Nowack and O. Pooth and A. Stahl and A. Zotz and H. Aarup Petersen and A. Abel and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and I. Andreev and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and S. Chatterjee and L. X. Coll Saravia and G. Eckerlin and D. Eckstein and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K.-Y. Lin and K. Lipka and W. Lohmann and J. Malvaso and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and L. Rygaard and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and M. Torkian and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and S. Zakharov and A. Zimermmane Castro Santos and A. Albrecht and A. R. Alves Andrade and M. Antonello and S. Bollweg and M. Bonanomi and K. El Morabit and Y. Fischer and M. Frahm and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and L. Moureaux and M. Mrowietz and A. Nigamova and K. Nikolopoulos and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and N. Prouvost and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and R. Ward and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and Y. M. Chen and T. Chwalek and A. Dierlamm and G. G. Dincer and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and R. Kunnilan Muhammed Rafeek and O. Lavoryk and J. M. Lawhorn and A. Lintuluoto and S. Maier and M. Mormile and Th. Müller and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and R. Schmieder and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and B. Topko and N. Trevisani and C. Verstege and T. Voigtländer and R. F. Von Cube and J. Von Den Driesch and M. Wassmer and R. Wolf and W. D. Zeuner and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and G. Melachroinos and Z. Painesis and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and T. Chatzistavrou and G. Karapostoli and K. Kousouris and E. Siamarkou and G. Tsipolitis and I. Bestintzanos and I. Evangelou and C. Foudas and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and D. Druzhkin and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and I. Szanyi and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and S. Phor and K. Ranjan and M. K. Saini and S. Acharya and B. Gomber and B. Sahu and S. Mukherjee and S. Baradia and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and G. Dash and A. Dattamunsi and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and T. Mishra and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and B. K. Sirasva and L. Bhatt and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and S. Barman and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and B. M. Joshi and M. Maity and G. Majumder and K. Mazumdar and S. Parolia and R. Saxena and A. Thachayath and S. Bahinipati and D. Maity and P. Mal and K. Naskar and A. Nayak and S. Nayak and K. Pal and R. Raturi and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and A. Alpana and S. Dube and P. Hazarika and B. Kansal and A. Laha and R. Sharma and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and V. Sedighzadeh Dalavi and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and M. Barbieri and M. Buonsante and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and F. Nenna and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and D. Fasanella and P. Giacomelli and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and J. Altork and P. Assiouras and G. Barbagli and G. Bardelli and M. Bartolini and A. Calandri and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and L. Damenti and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and V. Camagni and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and G. Lavizzari and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and C. Di Fraia and F. Fabozzi and L. Favilla and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and D. Bisello and P. Bortignon and G. Bortolato and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and F. Gasparini and U. Gasparini and S. Giorgetti and E. Lusiani and M. Margoni and J. Pazzini and P. Ronchese and R. Rossin and M. Sgaravatto and F. Simonetto and M. Tosi and A. Triossi and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and P. Montagna and M. Pelliccioni and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Della Penna and L. Fanò and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and L. Calligaris and R. Castaldi and F. Cattafesta and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and R. Forti and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and V. K. Muraleedharan Nair Bindhu and S. Nandan and F. Palla and M. Riggirello and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and F. Tenchini and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and P. Akrap and C. Basile and S. C. Behera and F. Cavallari and L. Cunqueiro Mendez and F. De Riggi and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and L. Frosina and R. Gargiulo and B. Harikrishnan and F. Lombardi and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and N. Palmeri and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and D. Dattola and N. Demaria and L. Finco and M. Grippo and B. Kiani and L. Lanteri and F. Legger and F. Luongo and C. Mariotti and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Ruspa and F. Siviero and V. Sola and A. Solano and C. Tarricone and D. Trocino and G. Umoret and E. Vlasov and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and R. Delli Gatti and S. Dogra and J. Hong and J. Kim and T. Kim and D. Lee and H. Lee and J. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and J. Seo and E. Asilar and F. Carnevali and J. Choi and T. J. Kim and Y. Ryou and S. Ha and S. Han and B. Hong and K. Lee and K. S. Lee and S. Lee and J. Yoo and J. Goh and J. Shin and Y. Kang and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and D. Kim and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and J. A. Merlin and I. C. Park and Y. Roh and I. J. Watson and G. Cho and K. Hwang and B. Kim and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and O. M. Eberlins and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and R. Plese and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and S. Nargelas and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and A. Cota Rodriguez and L. E. Cuevas Picos and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and R. Lopez-Fernandez and J. Mejia Guisao and R. Reyes-Almanza and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and F. E. Neri Huerta and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and W. A. Khan and V. Avati and L. Forthomme and L. Grzanka and M. Malawski and K. Piotrzkowski and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and L. Markovic and P. Milenovic and V. Milosevic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and M. Stojanovic and M. Alcalde Martinez and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and J. Cuchillo Ortega and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and M. Gonzalez Hernandez and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and C. Martin Perez and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and R. Paz Herrera and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Ayllon Torresano and A. Cardini and J. Cuevas and J. Del Riego Badas and D. Estrada Acevedo and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and M. Obeso Menendez and E. Palencia Cortezon and J. Prado Pico and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and C. Quintana San Emeterio and L. Scodellaro and I. Vila and R. Vilar Cortabitarte and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and J. Baechler and D. Barney and M. Bianco and A. Bocci and L. Borgonovi and C. Botta and A. Bragagnolo and C. E. Brown and C. Caillol and G. Cerminara and P. Connor and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and W. Funk and A. Gaddi and S. Giani and D. Gigi and K. Gill and F. Glege and M. Glowacki and A. Gruber and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and G. Karathanasis and S. Laurila and P. Lecoq and C. Lourenço and A.-M. Lyon and M. Magherini and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and M. Migliorini and F. Monti and F. Moortgat and M. Mulders and M. Musich and I. Neutelings and S. Orfanelli and F. Pantaleo and M. Pari and G. Petrucciani and A. Pfeiffer and M. Pierini and M. Pitt and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and P. Rosado and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and E. Vernazza and J. Wanczyk and S. Wuchterl and M. Zarucki and P. Zehetner and P. Zejdl and G. Zevi Della Porta and T. Bevilacqua and L. Caminada and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and U. Langenegger and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D’archiacchiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and W. Lustermann and M. Malucchi and R. A. Manzoni and M. Marchegiani and L. Marchese and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and F. Bilandzija and M. F. Canelli and G. Celotto and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and T. H. Kwok and S. Leontsinis and V. Lukashenko and A. Macchiolo and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and D. Bhowmik and C. M. Kuo and P. K. Rout and S. Taj and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and Y. Maghrbi and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and Y. Komurcu and G. Onengut and K. Ozdemir and B. Tali and U. G. Tok and E. Uslan and I. S. Zorbakir and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and M. A. Sarkisla and S. Tekten and A. Cakir and K. Cankocak and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and A. A. Guvenli and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and O. Dadazhanova and B. Grynyov and L. Levchuk and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and D. Dharmender and H. Flacher and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and M. S. Sanjrani and J. Segal and V. J. Smith and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and J. Gajownik and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and M. Moallemi and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and O. Buchmuller and C. A. Carrillo Montoya and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and H. R. Hoorani and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and E. Leutgeb and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and A. Mastronikolis and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and L. Russell and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and V. Hegde and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and J. M. Hogan and R. Bartek and A. Dominguez and S. Raj and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and S. Campbell and R. Chudasama and S. I. Cooper and C. Crovella and G. Fidalgo and S. V. Gleyzer and A. Khukhunaishvili and K. Matchev and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and S. Cholak and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and J. Fulcher and F. Golf and S. Jeon and J. O’Cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and E. Wurtz and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and S. Ellis and L. Gouskos and M. Hadley and U. Heintz and K. W. Ho and T. Kwon and G. Landsberg and K. T. Lau and J. Luo and S. Mondal and J. Roloff and T. Russell and S. Sagir and X. Shen and M. Stamenkovic and N. Venkatasubramanian and S. Abbott and B. Barton and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and O. Kukral and G. Mocellin and S. Ostrom and W. Wei and S. Yoo and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and V. Krutelyov and R. Lee and J. Letts and H. Li and M. Masciovecchio and F. Mokhtar and M. Pieri and D. Primosch and M. Quinnan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and A. Yagil and Z. Zhao and A. Barzdukas and L. Brennan and C. Campagnari and S. Carron Montero and K. Downham and C. Grieco and M. M. Hussain and J. Incandela and M. W. K. Lai and A. J. Li and P. Masterson and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and X. Yan and D. Zhang and A. Albert and A. Bornheim and O. Cerri and R. Kansal and J. Mao and H. B. Newman and G. Reales Gutiérrez and T. Sievert and M. Spiropulu and J. R. Vlimant and R. A. Wynne and S. Xie and J. Alison and S. An and M. Cremonesi and V. Dutta and E. Y. Ertorer and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and M. Kanemura and C. Liu and P. Meiring and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and S. Kwan and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and X. Chen and D. J. Cranshaw and J. Dickinson and J. Fan and X. Fan and J. Grassi and S. Hogan and P. Kotamnives and J. Monroy and G. Niendorf and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and L. Zygala and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and C. Cosby and G. Cummings and I. Dutta and V. D. Elvira and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and K. Maeshima and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and C. E. Perez Lara and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and M. Dittrich and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and V. Sulimov and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and M. Mazza and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and S. Butalla and S. Das and M. Hohlmann and M. Lavinsky and E. Yanes and M. R. Adams and N. Barnett and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and H. Gupta and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and C. Mills and S. Nanda and G. Nigmatkulov and B. Ozek and T. Phan and D. Pilipovic and R. Pradhan and E. Prifti and P. Roy and T. Roy and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and M. Alhusseini and D. Blend and K. Dilsiz and O. K. Köseyan and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and S. Sekhar and M. V. Srivastav and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and S. Popescu and C. Rogan and C. Royon and S. Rudrabhatla and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and N. Islam and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and S. Lascio and P. Major and A. C. Mignerey and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Zhang and C. Baldenegro Barrera and J. Bendavid and H. Bossi and S. Bright-Thonney and I. A. Cali and Y. c. Chen and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and G. M. Innocenti and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and T. a. Sheng and G. S. F. Stephans and D. Walter and Z. Wang and B. Wyslouch and T. J. Yang and B. Crossman and W. J. Jackson and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and O. Sancar and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and A. Rohilla and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and A. Mandal and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and D. Yu and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and J. Li and M. Lu and N. Manganelli and R. Mccarthy and D. M. Morse and T. Orimoto and A. Parker and L. Skinnari and C. S. Thoreson and E. Tsai and D. Wood and S. Dittmer and K. A. Hahn and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and A. Ehnis and R. Goldouzian and M. Hildreth and K. Hurtado Anampa and T. Ivanov and C. Jessop and A. Karneyeu and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and A. Basnet and M. Carrigan and R. De Los Santos and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and M. Galli and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and Y. Lai and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and F. Simpson and D. Stickland and C. Tully and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and D. Kondratyev and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and J. F. Schulte and F. Wang and A. Wildridge and W. Xie and Y. Yao and Y. Zhong and J. Dolen and N. Parashar and A. Pathak and E. Shumka and D. Acosta and A. Agrawal and C. Arbour and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and T. Huang and I. Krommydas and N. Lewis and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and O. Bessidskaia Bylund and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and H. S. Hare and O. Hindrichs and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and S. Donnelly and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and J. Martins and B. Rand and J. Reichert and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and D. Ally and A. G. Delannoy and S. Fiorendi and J. Harris and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and J. Lawless and L. Lee and E. Nibigira and B. Skipworth and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and A. Bolshov and O. Bouhali and R. Eusebi and P. Flanagan and J. Gilmore and Y. Guo and T. Kamon and S. Luo and R. Mueller and A. Safonov and N. Akchurin and J. Damgov and Y. Feng and N. Gogate and Y. Kazhykarim and K. Lamichhane and C. Madrid and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and D. Rathjens and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and M. Jose and A. Ledovskoy and C. Mantilla and C. Neu and C. Ramón Álvarez and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and S. Lomte and R. Loveless and A. Mallampalli and A. Mohammadi and T. Nelson and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and Yu. Andreev and T. Aushev and D. Budkouski and R. Chistov and M. Danilov and T. Dimova and A. Ershov and S. Gninenko and I. Gorbunov and A. Gribushin and A. Kamenev and V. Karjavine and M. Kirsanov and V. Klyukhin and O. Kodolova and V. Korenkov and A. Kozyrev and N. Krasnikov and A. Lanev and A. Malakhov and V. Matveev and A. Nikitenko and V. Palichik and V. Perelygin and S. Petrushanko and S. Polikarpov and O. Radchenko and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and Y. Skovpen and V. Smirnov and O. Teryaev and I. Tlisova and A. Toropin and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and L. Dudko and K. Ivanov and V. Kim and V. Murzin and V. Oreshkin and D. Sosnov and E. Boos and V. Bunichev and M. Dubinin and V. Savrin and A. Snigirev}, doi = {10.1103/6z3d-zjw4}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091802}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of WWZ and ZH production cross sections at s=13 and 13.6 TeV}, volume = {135}, year = {2025}, }
• (2025). First measurement of the decay dynamics in the semileptonic transition of d+(0) into the axial-vector meson k¯1(1270). PRL, 135(9), 091801. (www)

  @article{ , abstract = {Using data taken at the center-of-mass energy of 3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of , we report the first measurement of the decay dynamics of the semileptonic decays . The amplitude analysis gives the hadronic form factors of the semileptonic transitions into the axial-vector meson to be and . This is the first in the semileptonic decays of heavy mesons into axial-vector mesons. The angular analysis yields an up-down asymmetry , which is consistent with the standard model prediction. In addition, the branching fractions of and are determined with improved precision to be and , respectively. No significant signals of and are observed and their branching fraction upper limits are set as and at 90% confidence level, respectively.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Y. Y. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and F. M. Melendi and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and L. F. Tang and M. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/xj42-xgzf}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091801}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of the decay dynamics in the semileptonic transition of d+(0) into the axial-vector meson k¯1(1270)}, volume = {135}, year = {2025}, }
• (2025). Reflected multientropy and its holographic dual. PRL, 135(9), 091604. (www)

  @article{ , abstract = {We introduce a mixed-state generalization of the multientropy through the canonical purification, which we call “reflected multientropy.” We propose the holographic dual of this measure. For the tripartite case, a field-theoretical calculation is performed using a six-point function of twist operators at large limit. At both zero and finite temperature, the field-theoretical results match the holographic results, supporting our holographic conjecture of this new measure.}, archive = {J_PRL}, author = {Ma-Ke Yuan and Mingyi Li and Yang Zhou}, doi = {10.1103/76vs-rxcs}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091604}, shortjournal = {Phys. Rev. Lett.}, title = {Reflected multientropy and its holographic dual}, volume = {135}, year = {2025}, }
• (2025). Tying knots in particle physics. PRL, 135(9), 091603. (www)

  @article{ , abstract = {Knots emerge in various fields of mathematics and physics today. We show that knots indeed appear as stable solitons in a realistic extension of the standard model of particle physics that provides the QCD axion and right-handed neutrinos. This result suggests that, during the early Universe, a “knot dominated era” may have existed, where knots were a dominant component of the Universe, and this scenario can be tested through gravitational wave observations. Furthermore, we propose that the end of this era involves the collapse of the knots via quantum tunneling, leading to the generation of matter-antimatter asymmetry in the Universe.}, archive = {J_PRL}, author = {Minoru Eto and Yu Hamada and Muneto Nitta}, doi = {10.1103/s3vd-brsn}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091603}, shortjournal = {Phys. Rev. Lett.}, title = {Tying knots in particle physics}, volume = {135}, year = {2025}, }
• (2025). Temperature-resistant order in 2+1 dimensions. PRL, 135(9), 091602. (www)

  @article{ , abstract = {High temperatures are typically thought to increase disorder. Here we examine this idea in quantum field theory in 2 + 1 dimensions. For this sake we explore a novel class of tractable models, consisting of nearly-mean-field scalars interacting with critical scalars. We identify UV-complete, local, unitary models in this class and show that symmetry breaking Z 2 → ∅ occurs at any temperature in some regions of the phase diagram. This phenomenon, previously observed in models with fractional dimensions, or in the strict planar limits, or with nonlocal interactions, is now exhibited in a local, unitary 2 + 1 dimensional model with a finite number of fields.}, archive = {J_PRL}, author = {Zohar Komargodski and Fedor K. Popov}, doi = {10.1103/yb7d-6tvc}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091602}, shortjournal = {Phys. Rev. Lett.}, title = {Temperature-resistant order in 2+1 dimensions}, volume = {135}, year = {2025}, }
• (2025). Quasinormal modes of nonthermal fixed points. PRL, 135(9), 091601. (www)

  @article{ , abstract = {Quasinormal modes play a prominent role in the relaxation of diverse physical systems to equilibria, ranging from astrophysical black holes to tiny droplets of quark-gluon plasma at the RHIC and LHC accelerators. We propose that a novel kind of quasinormal mode governs the direct approach to self-similar time evolution of nonthermal fixed points, whose relevance ranges from high-energy physics to cold atom gases. We utilize black hole perturbation theory techniques to compute the spectrum of these far-from-equilibrium quasinormal modes for a kinetic theory with a Fokker-Planck collision kernel in isotropic and homogeneous states. Our conclusion is that quasinormal modes of nonthermal fixed points give rise to a tower of progressively more decaying power-law contributions. A by-product of our analysis is a precise determination and improved understanding of the distribution function characterizing nonthermal fixed points.}, archive = {J_PRL}, author = {Matisse De Lescluze and Michal P. Heller}, doi = {10.1103/tz78-jfbw}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091601}, shortjournal = {Phys. Rev. Lett.}, title = {Quasinormal modes of nonthermal fixed points}, volume = {135}, year = {2025}, }
• (2025). Equation of state of decompressed quark matter, and observational signatures of quark-star mergers. PRL, 135(9), 091402. (www)

  @article{ , abstract = {Quark stars are challenging to confirm or exclude observationally because they can have similar masses and radii as neutron stars. By performing the first calculation of the nonequilibrium equation of state of decompressed quark matter at finite temperature, we determine the properties of the ejecta from binary quark-star or quark star–black hole mergers. We account for all relevant physical processes during the ejecta evolution, including quark nugget evaporation and cooling, and weak interactions. We find that these merger ejecta can differ significantly from those in neutron star mergers, depending on the binding energy of quark matter. For relatively high binding energies, quark star mergers are unlikely to produce -process elements and kilonova signals. We propose that future observations of binary mergers and kilonovae could impose stringent constraints on the binding energy of quark matter and the existence of quark stars.}, archive = {J_PRL}, author = {Zhiqiang Miao and Zhenyu Zhu and Dong Lai}, doi = {10.1103/zklh-27mr}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091402}, shortjournal = {Phys. Rev. Lett.}, title = {Equation of state of decompressed quark matter, and observational signatures of quark-star mergers}, volume = {135}, year = {2025}, }
• (2025). Neutrino flavor transformation in neutron star mergers. PRL, 135(9), 091401. (www)

  @article{ , abstract = {We present the first numerical relativity simulations including neutrino flavor transformations that could result from flavor instabilities, quantum many-body effects, or potential beyond standard model physics in neutron star mergers. We find that neutrino flavor transformations impact the composition and structure of the remnant, potentially leaving an imprint on the postmerger gravitational-wave signal. They also have a significant impact on the composition and nucleosynthesis yields of the ejecta.}, archive = {J_PRL}, author = {Yi Qiu and David Radice and Sherwood Richers and Maitraya Bhattacharyya}, doi = {10.1103/h2q7-kn3v}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {091401}, shortjournal = {Phys. Rev. Lett.}, title = {Neutrino flavor transformation in neutron star mergers}, volume = {135}, year = {2025}, }
• (2025). Spectral gap optimization for enhanced adiabatic state preparation. PRL, 135(9), 090602. (www)

  @article{ , abstract = {The preparation of nontrivial states is crucial to the study of quantum many-body physics. Such states can be prepared with adiabatic quantum algorithms, which are restricted by the minimum spectral gap along the path. In this Letter, we propose an efficient method to adiabatically prepare tensor network states (TNSs). We maximize the spectral gap leveraging degrees of freedom in the parent Hamiltonian construction. We demonstrate this efficient adiabatic algorithm for preparing TNSs, through examples of random TNSs in one dimension, AKLT (Affleck-Kennedy-Lieb-Tasaki), and GHZ states. The Hamiltonian optimization applies to both injective and non-injective tensors, in the latter case by exploiting symmetries present in the tensors.}, archive = {J_PRL}, author = {Kshiti Sneh Rai and Jin-Fu Chen and Patrick Emonts and Jordi Tura}, doi = {10.1103/cslt-x32n}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090602}, shortjournal = {Phys. Rev. Lett.}, title = {Spectral gap optimization for enhanced adiabatic state preparation}, volume = {135}, year = {2025}, }
• (2025). Error-corrected fermionic quantum processors with neutral atoms. PRL, 135(9), 090601. (www)

  @article{ , abstract = {Many-body fermionic systems can be simulated in a hardware-efficient manner using a fermionic quantum processor. Neutral atoms trapped in optical potentials can realize such processors, where nonlocal fermionic statistics are guaranteed at the hardware level. Implementing quantum error correction in this setup is, however, challenging, due to the atom-number superselection present in atomic systems, that is, the impossibility of creating coherent superpositions of different particle numbers. In this Letter, we overcome this constraint and present a blueprint for an error-corrected fermionic quantum processor that can be implemented using current experimental capabilities. To achieve this, we first consider an ancillary set of fermionic modes and design a fermionic reference , which we then use to construct superpositions of different numbers of referenced fermions . This allows us to build logical fermionic modes that can be error corrected using standard atomic operations. Here, we focus on phase errors, which we expect to be a dominant source of errors in neutral-atom quantum processors. We then construct logical fermionic gates, and show their implementation for the logical particle-number conserving processes relevant for quantum simulation. Finally, our protocol is illustrated with a minimal fermionic circuit, where it leads to a quadratic suppression of the logical error rate.}, archive = {J_PRL}, author = {Robert Ott and Daniel González-Cuadra and Torsten V. Zache and Peter Zoller and Adam M. Kaufman and Hannes Pichler}, doi = {10.1103/zkpl-hh28}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090601}, shortjournal = {Phys. Rev. Lett.}, title = {Error-corrected fermionic quantum processors with neutral atoms}, volume = {135}, year = {2025}, }
• (2025). Scheme to detect the strong-to-weak symmetry breaking via randomized measurements. PRL, 135(9), 090403. (www)

  @article{ , abstract = {Symmetry breaking plays a central role in classifying the phases of quantum many-body systems. Recent developments have highlighted a novel symmetry-breaking pattern, in which the strong symmetry of a density matrix spontaneously breaks to the weak symmetry. This strong-to-weak symmetry breaking is typically detected using multireplica correlation functions, such as the Rényi-2 correlator. In this Letter, we propose a practical protocol for detecting strong-to-weak symmetry breaking in experiments using the randomized measurement toolbox. Our scheme involves collecting the results of random Pauli measurements for (i) the original quantum state and (ii) the quantum state after evolution with the charged operators. Based on the measurement results, with a large number of samples, we can obtain an unbiased estimate of the Rényi-2 correlator. With a small sample size, we can still provide an alternative approach to estimate the phase boundary to a decent accuracy. We perform numerical simulations of Ising chains with all-to-all decoherence as an exemplary demonstration. Our result opens the opportunity for the experimental studies of the novel quantum phases in mixed quantum states.}, archive = {J_PRL}, author = {Ning Sun and Pengfei Zhang and Lei Feng}, doi = {10.1103/7p5x-7yqb}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090403}, shortjournal = {Phys. Rev. Lett.}, title = {Scheme to detect the strong-to-weak symmetry breaking via randomized measurements}, volume = {135}, year = {2025}, }
• (2025). Enhancing revivals via projective measurements in a quantum scarred system. PRL, 135(9), 090402. (www)

  @article{ , abstract = {Quantum many-body scarred systems exhibit atypical dynamical behavior, evading thermalization and featuring periodic state revivals. In this Letter, we investigate the impact of projective measurements on the dynamics in the scar subspace for the paradigmatic PXP model, revealing that they can either disrupt or enhance the revivals. Local measurements performed at random times rapidly erase the system’s memory of its initial conditions, leading to fast steady state relaxation. In contrast, a periodic monitoring amplifies recurrences and preserves the coherent dynamics over extended timescales. We identify a measurement-induced phase resynchronization, countering the natural dephasing of quantum scars, as the key mechanism underlying this phenomenon.}, archive = {J_PRL}, author = {Alessio Paviglianiti and Alessandro Silva}, doi = {10.1103/jf2f-wqkx}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090402}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing revivals via projective measurements in a quantum scarred system}, volume = {135}, year = {2025}, }
• (2025). Probing topological entanglement on large scales. PRL, 135(9), 090401. (www)

  @article{ , abstract = {Topologically ordered quantum matter exhibits intriguing long-range patterns of entanglement, which reveal themselves in subsystem entropies. However, measuring such entropies, which can be used to certify topological order, on large partitions is challenging and becomes practically unfeasible for large systems. We propose a protocol based on local adiabatic deformations of the Hamiltonian which extracts the universal features of long-range topological entanglement from measurements on small subsystems of finite size, trading an exponential number of measurements against a polynomial-time evolution. Our protocol is general and readily applicable to various quantum simulation architectures. We apply our method to various string-net models representing both Abelian and non-Abelian topologically ordered phases and illustrate its application to neutral atom tweezer arrays with numerical simulations.}, archive = {J_PRL}, author = {Robert Ott and Torsten V. Zache and Nishad Maskara and Mikhail D. Lukin and Peter Zoller and Hannes Pichler}, doi = {10.1103/mdsf-wrbj}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090401}, shortjournal = {Phys. Rev. Lett.}, title = {Probing topological entanglement on large scales}, volume = {135}, year = {2025}, }
• (2025). Quantum bayes’ rule and petz transpose map from the minimum change principle. PRL, 135(9), 090203. (www)

  @article{ , abstract = {Bayes’ rule, which is routinely used to update beliefs based on new evidence, can be derived from a principle of minimum change. This principle states that updated beliefs must be consistent with new data, while deviating minimally from the prior belief. Here, we introduce a quantum analog of the minimum change principle and use it to derive a quantum Bayes’ rule by minimizing the change between two quantum input-output processes, not just their marginals. This is analogous to the classical case, where Bayes’ rule is obtained by minimizing several distances between the joint input-output distributions. When the change maximizes the fidelity, the quantum minimum change principle has a unique solution, and the resulting quantum Bayes’ rule recovers the Petz transpose map in many cases.}, archive = {J_PRL}, author = {Ge Bai and Francesco Buscemi and Valerio Scarani}, doi = {10.1103/5n4p-bxhm}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090203}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum bayes’ rule and petz transpose map from the minimum change principle}, volume = {135}, year = {2025}, }
• (2025). No practical quantum broadcasting: Even virtually. PRL, 135(9), 090202. (www)

  @article{ , abstract = {Quantum information cannot be broadcast—an intrinsic limitation imposed by quantum mechanics. However, recent advances in virtual operations offer new insights into the no-broadcasting theorem. Here, we focus on the practical utility and introduce sample efficiency as a fundamental constraint, requiring any practical broadcasting protocol perform no worse than the naive approach of direct preparation and distribution. We prove that no linear process—whether quantum or beyond—can simultaneously uphold sample efficiency, unitary covariance, permutation invariance, and classical consistency. This leads to a no-practical-broadcasting theorem , which places strict limits on the practical distribution of quantum information. By applying Schur-Weyl duality, we establish the uniqueness of the canonical 1-to- N virtual broadcasting map that satisfies the latter three conditions, provide its construction, and determine its sample complexity through semidefinite programming. Finally, we explore the interplay between virtual broadcasting and a quantum spacetime framework, known as the pseudodensity operator, showing that their correspondence holds only in the 1-to-2 case, underscoring the fundamental asymmetry between spatial and temporal statistics in the quantum world.}, archive = {J_PRL}, author = {Yunlong Xiao and Xiangjing Liu and Zhenhuan Liu}, doi = {10.1103/z2pr-zbwl}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090202}, shortjournal = {Phys. Rev. Lett.}, title = {No practical quantum broadcasting: Even virtually}, volume = {135}, year = {2025}, }
• (2025). Minimal example of quantum nonclassicality without freedom of choice. PRL, 135(9), 090201. (www)

  @article{ , abstract = {Bell’s theorem is often considered the most stringent notion of nonclassicality. The generalization of Bell’s theorem to causal networks offers interesting new perspectives on the phenomenon of quantum nonclassicality and prompts us with a fundamental inquiry: what is the simplest scenario leading to the incompatibility between quantum correlations and the classical theory of causality? Here, we demonstrate that quantum nonclassicality is possible in an entanglement swapping network consisting of only three dichotomic variables, without the need for the locality assumption or external measurement choices. We also show that interventions, a central tool in the field of causal inference, significantly improve the noise robustness of this new kind of nonclassical behavior, making it feasible for experimental tests with current technology.}, archive = {J_PRL}, author = {Pedro Lauand and Davide Poderini and Rafael Rabelo and Rafael Chaves}, doi = {10.1103/3854-r395}, journal = {Physical Review Letters}, month = {8}, number = {9}, pages = {090201}, shortjournal = {Phys. Rev. Lett.}, title = {Minimal example of quantum nonclassicality without freedom of choice}, volume = {135}, year = {2025}, }
• (2025). Erratum: Nonrelativistic holography from AdS5/CFT4 [Phys. rev. lett. 133, 151601 (2024)]. PRL, 135(8), 089901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 089901 (2025)}, archive = {J_PRL}, author = {Andrea Fontanella and Juan Miguel Nieto García}, doi = {10.1103/jr1v-74l8}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {089901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Nonrelativistic holography from AdS5/CFT4 [Phys. rev. lett. 133, 151601 (2024)]}, volume = {135}, year = {2025}, }
• (2025). Ordering and defect cloaking in nonreciprocal lattice XY models. PRL, 135(8), 088303. (www)

  @article{ , abstract = {We present a detailed analytical and numerical examination, on square and triangular lattices, of the nonreciprocal planar spin model introduced in Dadhichi et al. [ Phys. Rev. E 101 , 052601 (2020) ]. We show that the effect of lattice anisotropy should persist at large scales, leading to a “mass” for the angle field of the spins, and behavior not in the “Malthusian Toner-Tu” [ Phys. Rev. Lett. 108 , 088102 (2012) ] universality class. Numerically, we find evidence of this mass at large values of our nonreciprocity parameter; for smaller values, we find power-law scaling of long-wavelength equal-time correlators in the polar-ordered phase of our lattice model over the system sizes and wave number range explored. Focussing on topological defects, we show numerically that defect interactions are highly anisotropic with respect to the mean ordering direction. In particular, the constituents of a ± 1 pair are shielded from each other in a class of configurations, deferring their annihilation and allowing time for the nucleation of further defects. The result, we show numerically, is the destruction of the polarized phase via an aster apocalypse reminiscent of that found by Besse et al. [ Phys. Rev. Lett. 129 , 268003 (2022) ] for flocks without number conservation.}, archive = {J_PRL}, author = {Pankaj Popli and Ananyo Maitra and Sriram Ramaswamy}, doi = {10.1103/2yky-45sr}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {088303}, shortjournal = {Phys. Rev. Lett.}, title = {Ordering and defect cloaking in nonreciprocal lattice XY models}, volume = {135}, year = {2025}, }
• (2025). Inescapable anisotropy of nonreciprocal XY models. PRL, 135(8), 088302. (www)

  @article{ , abstract = {We investigate nonreciprocal XY (NRXY) models defined on two-dimensional lattices in which the coupling strength of a spin with its neighbors varies with their position in the frame defined by the current spin orientation. As expected from the seminal work of Dadhichi et al. , [Nonmutual torques and the unimportance of motility for long-range order in two-dimensional flocks, Phys. Rev. E 101 , 052601 (2020) ], we first show that nonreciprocity is akin to a self-propulsion: we derive a mean-field continuous theory identical to that of constant-density flocks. Like the latter, NRXY models exhibit a long-range ordered phase that is metastable to the nucleation of topological defects, and their asymptotic state is a dynamic foam of asters. We then show that in the metastable ordered phase, the lattice always induces anisotropy on large scales, pinning the direction of order and imposing a finite correlation length. Crucially, we demonstrate that this anisotropy is inescapable since, even when not explicitly present in the interaction rule, it is generated by fluctuations. In short, the ordered phase of lattice NRXY models is that of active clock models.}, archive = {J_PRL}, author = {Dawid Dopierala and Hugues Chaté and Xia-qing Shi and Alexandre Solon}, doi = {10.1103/r3dx-7lrd}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {088302}, shortjournal = {Phys. Rev. Lett.}, title = {Inescapable anisotropy of nonreciprocal XY models}, volume = {135}, year = {2025}, }
• (2025). Optimal closed-loop control of active particles and a minimal information engine. PRL, 135(8), 088301. (www)

  @article{ , abstract = {We study the elementary problem of moving an active particle by a trap with minimum work input. We show analytically that (open-loop) optimal protocols are not affected by activity, but work fluctuations are always increased. For closed-loop protocols, which rely on initial measurements of the self-propulsion, the average work has a minimum for a finite persistence time. Using these insights, we derive an optimal periodic active information engine, which is found to have higher precision and information efficiency when operated with a run-and-tumble particle than for an active Ornstein-Uhlenbeck particle and, we argue, than for any other type of active particle.}, archive = {J_PRL}, author = {Rosalba Garcia-Millan and Janik Schüttler and Michael E. Cates and Sarah A. M. Loos}, doi = {10.1103/fbgp-qpvv}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {088301}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal closed-loop control of active particles and a minimal information engine}, volume = {135}, year = {2025}, }
• (2025). Rigidity criteria for chainmail consisting of tessellations of torus knots. PRL, 135(8), 088201. (www)

  @article{ , abstract = {Interlocked and polycatenated material systems, consisting of discrete, nonconvex particles linked to their nearest neighbors, such as chainmail fabrics, have been shown to undergo a jamming transition that increases their rigidity under boundary compression. This rigidity transition is associated with an increase in contact number between particles. In architected materials, rigidity is described by theories such as the Maxwell criterion. In this Letter, we propose a rigidity theory for a type of interlocked material system: the torus knot tessellation. Torus knot tessellations are structured fabrics composed of particles shaped as torus knots. In these fabrics, we theoretically demonstrate that in-plane rigidity is governed by a modified Maxwell criterion, while out-of-plane rigidity is governed by a crease line criterion. These theories provide a framework for the design of rigidity of these fabrics.}, archive = {J_PRL}, author = {Hujie Yan and Zhiqiang Meng and Ziran Zhou and Wenjie Zhou and Chiara Daraio}, doi = {10.1103/q4k4-x2zm}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {088201}, shortjournal = {Phys. Rev. Lett.}, title = {Rigidity criteria for chainmail consisting of tessellations of torus knots}, volume = {135}, year = {2025}, }
• (2025). Core-periphery detection in multilayer networks. PRL, 135(8), 087402. (www)

  @article{ , abstract = {Multilayer networks provide a powerful framework for modeling complex systems that capture different types of interactions between the same set of entities across multiple layers. Core-periphery detection involves partitioning the nodes of a network into core nodes, which are highly connected across the network, and peripheral nodes, which are densely connected to the core but sparsely connected among themselves. In this paper, we propose a new model of core-periphery structure in multilayer networks and a nonlinear spectral method that simultaneously detects the corresponding core and periphery structures of both nodes and layers in weighted and directed multilayer networks. Our method reveals novel structural insights in three empirical multilayer networks from distinct application areas: the citation network of complex network scientists, the European airlines transport network, and the world trade network.}, archive = {J_PRL}, author = {Kai Bergermann and Francesco Tudisco}, doi = {10.1103/yr23-71yc}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {087402}, shortjournal = {Phys. Rev. Lett.}, title = {Core-periphery detection in multilayer networks}, volume = {135}, year = {2025}, }
• (2025). Self-reinforcing cascades: A spreading model for beliefs or products of varying intensity or quality. PRL, 135(8), 087401. (www)

  @article{ , abstract = {Models of how things spread often assume that transmission mechanisms are fixed over time. However, social contagions—the spread of ideas, beliefs, innovations—can lose or gain in momentum as they spread: ideas can get reinforced, beliefs strengthened, products refined. We study the impacts of such self-reinforcement mechanisms in cascade dynamics. We use different mathematical modeling techniques to capture the recursive, yet changing nature of the process. We find a critical regime with a range of power-law cascade size distributions with nonuniversal scaling exponents. This regime clashes with classic models, where criticality requires fine-tuning at a precise critical point. Self-reinforced cascades produce critical-like behavior over a wide range of parameters, which may help explain the ubiquity of power-law distributions in empirical social data.}, archive = {J_PRL}, author = {Laurent Hébert-Dufresne and Juniper Lovato and Giulio Burgio and James P. Gleeson and S. Redner and P. L. Krapivsky}, doi = {10.1103/5mph-sws5}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {087401}, shortjournal = {Phys. Rev. Lett.}, title = {Self-reinforcing cascades: A spreading model for beliefs or products of varying intensity or quality}, volume = {135}, year = {2025}, }
• (2025). Sparse learning enabled by constraints on connectivity and function. PRL, 135(8), 087301. (www)

  @article{ , abstract = {Sparse connectivity is a hallmark of the brain and a desired property of artificial neural networks. It promotes energy efficiency, simplifies training, and enhances the robustness of network function. Thus, a detailed understanding of how to achieve sparsity without jeopardizing network performance is beneficial for neuroscience, deep learning, and neuromorphic computing applications. We used an exactly solvable model of associative learning to evaluate the effects of various sparsity-inducing constraints on connectivity and function. We determine the optimal level of sparsity achieved by the norm constraint and find that nearly the same efficiency can be obtained by eliminating weak connections. We show that this method of achieving sparsity can be implemented online, making it compatible with neuroscience and machine learning applications.}, archive = {J_PRL}, author = {Mirza M. Junaid Baig and Armen Stepanyants}, doi = {10.1103/918k-x6np}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {087301}, shortjournal = {Phys. Rev. Lett.}, title = {Sparse learning enabled by constraints on connectivity and function}, volume = {135}, year = {2025}, }
• (2025). Compact metaplate with bound state in the continuum: From quasisymmetry to symmetry. PRL, 135(8), 087201. (www)

  @article{ , abstract = {Building localized states with high quality factors in compact dynamic systems could enhance the performance of wave control devices such as elastic filters and high-precision sensing devices. Here, we report on the theoretical and experimental investigation of symmetry-protected bound states in the continuum (BICs) in a compressed metaplate. The proposed theory establishes a Bessel-zero-directed multipolarization design that enables precise modulation for the frequencies and modes of BICs. Experimental results reveal a critical threshold for symmetric protection, beyond which the polarization mode of BICs still exists despite leakage modes. The measured quality factor of BICs in the cylindrical-shelled metaplate rises to 720 via symmetry translation. The metaplate shows an enhanced performance over conventional defect and topological modes. This work opens a route toward compact elastic devices for applications in fields like on-chip communication, elastic wave filtering, and high-precision sensing within tight environments.}, archive = {J_PRL}, author = {Zhihui Wen and Penglin Gao and Jiawei Mao and Shoubo Dai and Marc Marti-Sabaté and Yabin Jin and Daniel Torrent and Yegao Qu}, doi = {10.1103/sbk1-szl7}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {087201}, shortjournal = {Phys. Rev. Lett.}, title = {Compact metaplate with bound state in the continuum: From quasisymmetry to symmetry}, volume = {135}, year = {2025}, }
• (2025). Probing the quantum capacitance of rydberg transitions of surface electrons on liquid helium via microwave frequency modulation. PRL, 135(8), 087001. (www)

  @article{ , abstract = {We present a method for probing the quantum capacitance associated with the Rydberg transition of surface electrons on liquid helium using radio-frequency (rf) reflectometry. Resonant microwave excitation of the Rydberg transition induces a redistribution of image charges on capacitively coupled electrodes, giving rise to a quantum capacitance originating from adiabatic state transitions and the finite curvature of the energy bands. By applying frequency-modulated resonant microwaves to drive the Rydberg transition, we systematically measured a capacitance sensitivity of 0.34 aF / Hz for our rf reflectometry scheme. This sensitivity is sufficient to detect the Rydberg transition of a single electron, offering a scalable pathway toward qubit readout schemes based on surface electrons on helium.}, archive = {J_PRL}, author = {Asher Jennings and Ivan Grytsenko and Yiran Tian and Oleksiy Rybalko and Jun Wang and Itay Josef Barabash and Erika Kawakami}, doi = {10.1103/5y8p-qhb4}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {087001}, shortjournal = {Phys. Rev. Lett.}, title = {Probing the quantum capacitance of rydberg transitions of surface electrons on liquid helium via microwave frequency modulation}, volume = {135}, year = {2025}, }
• (2025). On-chip emitter-coupled meta-optics for versatile photon sources. PRL, 135(8), 086902. (www)

  @article{ , abstract = {Controlling the spontaneous emission of nanoscale quantum emitters (QEs) is crucial for developing advanced photon sources required in many areas of modern nanophotonics, including quantum information technologies. Conventional approaches to shaping photon emission are based on using bulky configurations, while approaches recently developed in quantum metaphotonics suffer from limited capabilities in achieving desired polarization states and directionality, failing to provide on-demand photon sources tailored precisely to technological needs. Here, we propose a universal approach to designing versatile photon sources using on-chip QE-coupled meta-optics that enable direct transformations of QE-excited surface plasmon polaritons into spatially propagating photon streams with arbitrary polarization states, directionality, and amplitudes via both resonance and geometric phases supplied by scattering meta-atoms. Leveraging this platform, we experimentally demonstrate the independent engineering of polarization states, directionality, and relative amplitudes of photon emission in single and multiple radiation channels. The developed universal approach represents a major step toward the realization of versatile quantum sources, highlighting the potential of integrated photon sources with superior properties for both classical and quantum information technologies.}, archive = {J_PRL}, author = {Sören im Sande and Yinhui Kan and Danylo Komisar and Cuo Wu and Shailesh Kumar and Sergey I. Bozhevolnyi and Fei Ding}, doi = {10.1103/klq1-wjjg}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086902}, shortjournal = {Phys. Rev. Lett.}, title = {On-chip emitter-coupled meta-optics for versatile photon sources}, volume = {135}, year = {2025}, }
• (2025). Unveiling three types of fermions in a nodal ring topological semimetal through magneto-optical transitions. PRL, 135(8), 086901. (www)

  @article{ , abstract = {We investigate the quasiparticles of a single nodal ring semimetal through axis-resolved magneto-optical measurements. We observe three types of Landau levels scaling as , and that correspond to Dirac, semi-Dirac, and classical fermions, respectively. Through theoretical analysis, we identify the distinct origins of these three types of fermions present within the nodal ring. In particular, semi-Dirac fermions—a novel type of fermion that can give rise to a range of unique quantum phenomena—emerge from the end points of the nodal ring where the energy band disperses linearly along one direction and quadratically along the perpendicular direction, a feature not achievable in nodal point or line structures. The capacity of the nodal ring to simultaneously host multiple fermion types, including semi-Dirac fermions, establishes it as a valuable platform to expand the understanding of topological semimetals.}, archive = {J_PRL}, author = {Jiwon Jeon and Taehyeok Kim and Jiho Jang and Hoil Kim and Mykhaylo Ozerov and Jun Sung Kim and Hongki Min and Eunjip Choi}, doi = {10.1103/wfzd-7r9n}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086901}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling three types of fermions in a nodal ring topological semimetal through magneto-optical transitions}, volume = {135}, year = {2025}, }
• (2025). Terahertz and high-harmonic radiation from ultrafast light subgap or above-gap driving of spin-orbit proximitized antiferromagnetic mott insulator. PRL, 135(8), 086704. (www)

  @article{ , abstract = {Ultrafast light-driven strongly correlated antiferromagnetic insulators, such as prototypical NiO with a large Mott energy gap ≃ 4 eV , have recently attracted experimental attention using photons of both subgap [H. Qiu et al. , Nat. Phys. 17 , 388 (2021) ] and above-gap energy [K. Gillmeister et al. , Nat. Commun. 11 , 4095 (2020) ]. In the former context, which is also of great interest to applications, emission of terahertz (THz) radiation is observed from NiO/Pt bilayers, where heavy metal (HM) Pt introduces strong spin-orbit coupling (SOC) effects. However, in contrast to amply studied spintronic THz emitters using femtosecond laser pulse (fsLP)-driven FM/HM (where FM represents a ferromagnetic metal of the conventional type, such as Fe, Ni, or Co) bilayers, where ultrafast demagnetization takes place and is directly related to THz emission, microscopic mechanisms of electromagnetic (EM) radiation from NiO/HM bilayers remain obscure, as the total magnetization of NiO is zero before fsLP application. We employ the two-orbital Hubbard-Hund-Heisenberg model and study, via numerically exact quantum many-body methods, the dynamics of its Néel vector and nonequilibrium magnetization. This reveals nonclassical (i.e., not describable by the Landau-Lifshitz equation) dynamics of Néel vector and nonequilibrium magnetization, changing only in length while not rotating, where the former is substantially reduced in the case of above-gap fsLPs. Additionally, we compute EM radiation by time dependence of magnetization or of local charge currents, finding that both contributions are significant in the THz frequency range only in NiO with proximity SOC introduced by the HM layer. Outside the THz range, we find an integer high-harmonic generation, as well as unusual noninteger harmonics for the above-gap fsLP pump.}, archive = {J_PRL}, author = {Federico Garcia-Gaitan and Adrian E. Feiguin and Branislav K. Nikolić}, doi = {10.1103/8dhn-dh55}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086704}, shortjournal = {Phys. Rev. Lett.}, title = {Terahertz and high-harmonic radiation from ultrafast light subgap or above-gap driving of spin-orbit proximitized antiferromagnetic mott insulator}, volume = {135}, year = {2025}, }
• (2025). Strong magnon-phonon coupling in the kagome antiferromagnets. PRL, 135(8), 086703. (www)

  @article{ , abstract = {Magnon-phonon hybridization in ordered materials is a crucial phenomenon with significant implications for spintronics, magnonics, and quantum materials research. We present direct experimental evidence and theoretical insights into magnon-phonon coupling in , a kagome antiferromagnet with noncollinear spin order. Using inelastic x-ray scattering and ab initio modeling, we uncover strong hybridization between planar spin fluctuations and transverse optical phonons, resulting in a large hybridization gap of . This coupling is driven by interlayer Heisenberg exchange interactions and is enhanced by the material’s symmetry and magnetic frustration. The simplicity of the structure enables clear identification of the hybridized modes, bridging theoretical predictions and experimental observations. Our findings establish as a model system for exploring magnon-phonon interactions and offer a pathway for designing materials with tunable magnetoelastic properties.}, archive = {J_PRL}, author = {A. S. Sukhanov and O. I. Utesov and A. N. Korshunov and N. D. Andriushin and M. S. Pavlovskii and S. E. Nikitin and A. A. Kulbakov and K. Manna and C. Felser and M. C. Rahn}, doi = {10.1103/gymx-jk1g}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086703}, shortjournal = {Phys. Rev. Lett.}, title = {Strong magnon-phonon coupling in the kagome antiferromagnets}, volume = {135}, year = {2025}, }
• (2025). Two-peak heat capacity accounts for rln(2) entropy and ground state access in the dipole-octupole pyrochlore Ce2Hf2O7. PRL, 135(8), 086702. (www)

  @article{ , abstract = {Magnetic heat capacity measurements of a high-quality single crystal of the dipole-octupole pyrochlore Ce 2 Hf 2 O 7 down to a temperature of T = 0.02 K are reported. These show a two-peaked structure, with a Schottky-like peak at T 1 ∼ 0.065 K , similar to what is observed in its sister Ce pyrochlores Ce 2 Zr 2 O 7 and Ce 2 Sn 2 O 7 . However, a second sharper peak is observed at T 2 ∼ 0.025 K , signifying the entrance to the ground state. The ground state appears to have gapped excitations, as even the most abrupt extrapolation to C P = 0 at T = 0 K fully accounts for the R ln ( 2 ) entropy associated with the pseudospin- 1 / 2 doublet for Ce 3 + in this environment. The ground state could be conventionally ordered, although theory predicts a much larger anomaly in C P at much higher temperatures than the measured T 2 for expectations from an all-in, all-out ground state of the XYZ Hamiltonian for Ce 2 Hf 2 O 7 . The sharp low-temperature peak could also signify a crossover from a classical spin liquid to a quantum spin liquid (QSL). For both scenarios, comparison of the measured C P with NLC calculations suggests that weak interactions beyond the nearest-neighbor XYZ Hamiltonian become relevant below T ∼ 0.25 K . The diffuse magnetic neutron scattering observed from Ce 2 Hf 2 O 7 at low temperatures between T 2 and T 1 resembles that observed from Ce 2 Zr 2 O 7 , which is well established as a π -flux quantum spin ice (QSI). Together with the peak in the heat capacity at T 2 , this diffuse scattering from Ce 2 Hf 2 O 7 is suggestive of a classical spin liquid regime above T 2 that is distinct from the zero-entropy quantum ground state below T 2 .}, archive = {J_PRL}, author = {E. M. Smith and A. Fitterman and R. Schäfer and B. Placke and A. Woods and S. Lee and S. H.-Y. Huang and J. Beare and S. Sharma and D. Chatterjee and C. Balz and M. B. Stone and A. I. Kolesnikov and A. R. Wildes and E. Kermarrec and G. M. Luke and O. Benton and R. Moessner and R. Movshovich and A. D. Bianchi and B. D. Gaulin}, doi = {10.1103/4qxy-l8pg}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086702}, shortjournal = {Phys. Rev. Lett.}, title = {Two-peak heat capacity accounts for rln(2) entropy and ground state access in the dipole-octupole pyrochlore Ce2Hf2O7}, volume = {135}, year = {2025}, }
• (2025). Emergent self-propulsion of skyrmionic matter in synthetic antiferromagnets. PRL, 135(8), 086701. (www)

  @article{ , abstract = {Self-propulsion plays a crucial role in biological processes and nanorobotics, enabling small systems to move autonomously in noisy environments. Here, we theoretically demonstrate that a bound skyrmion-skyrmion pair in a synthetic antiferromagnetic bilayer can function as a self-propelled topological object, reaching speeds of up to a hundred million body lengths per second—far exceeding those of any known synthetic or biological self-propelled particles. The propulsion mechanism is triggered by the excitation of back-and-forth relative motion of the skyrmions, which generates nonreciprocal gyrotropic forces, driving the skyrmion pair in a direction perpendicular to their bond. Remarkably, thermal noise induces spontaneous reorientations of the pair and momentary reversals of the propulsion, mimicking behaviors observed in motile bacteria and microalgae.}, archive = {J_PRL}, author = {Clécio C. de Souza Silva and Matheus V. Correia and J. C. Piña Velásquez}, doi = {10.1103/c2y9-3cc9}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086701}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent self-propulsion of skyrmionic matter in synthetic antiferromagnets}, volume = {135}, year = {2025}, }
• (2025). Extracting topological spins from bulk multipartite entanglement. PRL, 135(8), 086601. (www)

  @article{ , abstract = {We address the problem of identifying a topologically ordered phase using measurements on the ground-state wave function. For nonchiral topological order, we describe a series of bulk multipartite entanglement measures that extract the invariants for any , where and are the quantum dimension and topological spin of an anyon , respectively. These invariants are obtained as expectation values of permutation operators between replicas of the wave function, applying different permutations on four distinct regions of the plane. Our proposed measures provide a refined tool for distinguishing topological phases, capturing information beyond conventional entanglement measures such as the topological entanglement entropy. We argue that any operator capable of extracting the above invariants must act on at least replicas, making our procedure optimal in terms of the required number of replicas. We discuss the generalization of our results to chiral states.}, archive = {J_PRL}, author = {Yarden Sheffer and Ady Stern and Erez Berg}, doi = {10.1103/h53w-64dy}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086601}, shortjournal = {Phys. Rev. Lett.}, title = {Extracting topological spins from bulk multipartite entanglement}, volume = {135}, year = {2025}, }
• (2025). Attosecond all-optical retrieval of valley polarization via circular dichroism in transient absorption. PRL, 135(8), 086404. (www)

  @article{ , abstract = {We propose a scheme for retrieving the ultrafast valley polarization (VP) dynamics in two-dimensional hexagonal materials via attosecond circular dichroism (CD) transient absorption spectroscopy. This approach builds on the CD transition between the first and higher conduction bands induced by the circularly polarized probe pulses. The population imbalance at nonequivalent valleys in the first conduction band is proportionally mapped onto the difference in absorption coefficients of two probe pulses with opposite helicities, supporting an unprecedented quantitative retrieval of the corresponding VP dynamics with subfemtosecond time resolution. We theoretically demonstrate the scheme for h -BN and MoS 2 through ab initio calculations, achieving an accurate retrieval of the VP dynamics, particularly the transient VP switching processes, with a time resolution of 250 as.}, archive = {J_PRL}, author = {Wenqing Li and Xiaosong Zhu and Pengfei Lan and Liang Li and Kai Wang and Wanzhu He and Hannes Hübener and Umberto De Giovannini and Peixiang Lu}, doi = {10.1103/7n3p-cq9f}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086404}, shortjournal = {Phys. Rev. Lett.}, title = {Attosecond all-optical retrieval of valley polarization via circular dichroism in transient absorption}, volume = {135}, year = {2025}, }
• (2025). Microscopic mechanism of coexisting electron spin resonance and kondo resonance in a single iron phthalocyanine molecule. PRL, 135(8), 086403. (www)

  @article{ , abstract = {The multiplicity of orbitals in quantum systems significantly influences the competition between Kondo screening and local spin magnetization. The identification of orbital-specific processes is essential for advancing spintronic devices, as well as for enhancing the understanding of many-body quantum phenomena, but it remains a great challenge. Here, we use a combination of scanning tunneling microscopy/spectroscopy and electron spin resonance (ESR) spectroscopy to investigate single iron phthalocyanine (FePc) molecules on . We observe the coexistence of ESR and Kondo resonance from the Fe(II) ion center at a temperature well below the Kondo temperature , where the magnetic moments are determined to be 1 Bohr magneton ( ), corresponding to a spin state in either of the ESR and Kondo resonance channels. On the basis of the observed in-plane twofold symmetry in the spatial distribution of ESR linewidths, in combination with density functional theory calculations, we attribute one spin state in the degeneracy-lifted orbital to the ESR channel, and the other in the highly screenable orbital to the Kondo resonance, respectively, within the framework of the two-channel Kondo model of an ordinary Fermi liquid.}, archive = {J_PRL}, author = {Qi Chen and Hongjian Du and Xinyong Meng and Jufeng Wang and Jingzun Liao and Bin Li and Wei Hu and Qitang Fan and Shijing Tan and Chuanxu Ma and Jinlong Yang and J. G. Hou and Bing Wang}, doi = {10.1103/cgq3-dyxb}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086403}, shortjournal = {Phys. Rev. Lett.}, title = {Microscopic mechanism of coexisting electron spin resonance and kondo resonance in a single iron phthalocyanine molecule}, volume = {135}, year = {2025}, }
• (2025). Multistate ferroelectricity enabled by electrically controlled phase transition of two-dimensional ices. PRL, 135(8), 086402. (www)

  @article{ , abstract = {Multistate ferroelectric polarization holds promise for realizing high-density nonvolatile memory devices, but so far is restricted to a few traditional ferroelectrics. Here, we show that nanoconfined two-dimensional (2D) ferroelectric ice can achieve phase-dependent multistate polarization through extensive classical and ab initio molecular dynamics simulations. An in-plane electric field is found to induce the reversible transition between a low-polarization -stacked hexagonal ice phase and an unprecedented high-polarization -stacked ice phase, resulting in a four-state ferroelectric switching pathway. The findings highlight the potential of 2D ice as a functional material for the development of multistate ferroelectric memory devices.}, archive = {J_PRL}, author = {Junjie Fang and Wanlin Guo and Hu Qiu}, doi = {10.1103/ng9v-kxvd}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086402}, shortjournal = {Phys. Rev. Lett.}, title = {Multistate ferroelectricity enabled by electrically controlled phase transition of two-dimensional ices}, volume = {135}, year = {2025}, }
• (2025). Universal wilson loop bound of quantum geometry. PRL, 135(8), 086401. (www)

  @article{ , abstract = {We define the absolute Wilson loop winding and prove that it bounds the (integrated) quantum metric from below. This Wilson loop lower bound naturally reproduces the known Chern and Euler bounds of the integrated quantum metric and provides an explicit lower bound of the integrated quantum metric due to the time-reversal protected Z 2 index, answering a hitherto open question. In general, the Wilson loop lower bound can be applied to any other topological invariants characterized by Wilson loop winding, such as the particle-hole Z 2 index. As physical consequences of the Z 2 bound, we show that the time-reversal Z 2 index bounds superfluid weight and optical conductivity from below and bounds the direct gap of a band insulator from above.}, archive = {J_PRL}, author = {Jiabin Yu and Jonah Herzog-Arbeitman and B. Andrei Bernevig}, doi = {10.1103/mp2c-zzkt}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal wilson loop bound of quantum geometry}, volume = {135}, year = {2025}, }
• (2025). Co and CoPc molecular kondo box on gold surface. PRL, 135(8), 086201. (www)

  @article{ , abstract = {We demonstrate a class of Co and CoPc molecular Kondo boxes on the Au(111) surface through scanning tunneling microscopy experiments and first-principles calculations. The -electron states of the CoPc molecule hybridize with the conduction electron states of the Au(111) substrate, imparting itinerantlike electron characteristics. Because of the high symmetry matching between the orbitals of Co adatoms and the orbitals of CoPc, the large orbital overlap predominates the formation of a Kondo singlet within the molecular complexes that prevail over the competition from the metal substrate, enabling them effectively as the molecular Kondo boxes. Furthermore, increasing the number of Co adatoms and modulating the overall symmetry of the molecular Kondo box can effectively tune the Kondo temperature .}, archive = {J_PRL}, author = {Xiangyang Li and Liang Zhu and Aidi Zhao and Yi Luo and J. G. Hou and Bin Li and Bing Wang and Jinlong Yang}, doi = {10.1103/65qq-dknn}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086201}, shortjournal = {Phys. Rev. Lett.}, title = {Co and CoPc molecular kondo box on gold surface}, volume = {135}, year = {2025}, }
• (2025). Vortex lattice states of bilayer electron-hole fluids in quantizing magnetic fields. PRL, 135(8), 086002. (www)

  @article{ , abstract = {We show that the ground state of a weakly charged two-dimensional electron-hole fluid in a strong magnetic field is a broken translation symmetry state with interpenetrating lattices of localized vortices and antivortices in the electron-hole-pair field. The vortices and antivortices carry fractional charges of equal sign but unequal magnitude and have a honeycomb-lattice structure that contrasts with the triangular lattices of superconducting electron-electron-pair vortex lattices. We predict that increasing charge density or a weakening magnetic field drives a vortex delocalization transition that would be signaled experimentally by an abrupt increase in counterflow transport resistance.}, archive = {J_PRL}, author = {Bo Zou and A. H. MacDonald}, doi = {10.1103/83f9-pln9}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086002}, shortjournal = {Phys. Rev. Lett.}, title = {Vortex lattice states of bilayer electron-hole fluids in quantizing magnetic fields}, volume = {135}, year = {2025}, }
• (2025). Spontaneous lattice distortion in the spin-triplet superconductor CuxBi2Se3. PRL, 135(8), 086001. (www)

  @article{ , abstract = {The doped topological insulator Cu x Bi 2 Se 3 has attracted considerable attention as a new platform for studying novel properties of spin-triplet and topological superconductivity. In this work, we performed synchrotron x-ray diffraction measurements on Cu x Bi 2 Se 3 ( 0.24 ≤ x ≤ 0.46 ) to investigate the coupling between the superconducting order parameter and crystal lattice. In the crystals in which the vector order parameter ( d vector) is tilted from the crystal high-symmetry directions as evidenced by nematic diamagnetic susceptibility, we find a sizable lattice distortion ( ∼ 100 pp m ) associated with the onset of superconductivity. In contrast, in crystals with the d vector aligned along the high-symmetry directions, we find no appreciable change in lattice constant. Together with a pronounced vestigial behavior of the distortion, the results are clear evidence for an odd-parity E u order parameter that couples with trigonal lattice. Furthermore, in the crystal with x = 0.46 where diamagnetic susceptibility is isotropic in the plane, no lattice distortion accompanying the superconducting transition is found, which is in line with a chiral superconducting state in the highly doped region. Our work shows that lattice distortion can be a powerful diagnosing quantity for nematic superconductivity with two-component order parameter.}, archive = {J_PRL}, author = {K. Matano and S. Takayanagi and K. Ito and S. Nita and M. Yokoyama and M. Mihaescu and H. Nakao and Guo-qing Zheng}, doi = {10.1103/ddvn-8c9n}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {086001}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous lattice distortion in the spin-triplet superconductor CuxBi2Se3}, volume = {135}, year = {2025}, }
• (2025). Demonstration of a novel radiochemical mix diagnostic for fusion implosions at the national ignition facility. PRL, 135(8), 085101. (www)

  @article{ , abstract = {Mixing of the ablator material into the fuel of an inertial confinement fusion implosion reduces compression and enhances radiative losses, preventing ignition. We describe a novel use of charged-particle radiochemistry to measure the ablator mix in contact with the fusion hot spot. The capsule uses a graded Be-Cr layer to increase the confinement of the hot spot. and isotopes are collected from the implosion and counted, and the ratio is related to the amount of Cr mixed into the hot spot. Thus, a new diagnostic to determine the degradation due to mix on fusion implosions has been developed.}, archive = {J_PRL}, author = {S. A. MacLaren and E. L. Dewald and D. A. Martinez and N. Gharibyan and K. Moody and C. Horwood and P. J. Bedrossian and R. D. Hoffman and G. B. Zimmerman and H. W. Xu and C. Kong and K. Sequoia and J. E. Pino and R. E. Tipton and D. D.-M. Ho and C. V. Young and J. D. Despotopulos and K. N. Kmak and D. A. Shaughnessy and S. Prisbrey and H. Huang and M. Ratledge and N. Rice}, doi = {10.1103/p72v-xs9d}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {085101}, shortjournal = {Phys. Rev. Lett.}, title = {Demonstration of a novel radiochemical mix diagnostic for fusion implosions at the national ignition facility}, volume = {135}, year = {2025}, }
• (2025). Meniscus-driven modulation of surface wave transmission across a barrier. PRL, 135(8), 084001. (www)

  @article{ , abstract = {Meniscus oscillations at interfaces between liquids, solids, and air significantly impact fluid dynamics and control. While idealized models exist, experimental data on capillary–gravity wave scattering involving meniscus effects remain limited. In this Letter, we systematically measured wave transmission past a surface-piercing barrier, focusing on meniscus effects. By varying the barrier’s surface properties and the wave frequencies, we explored how meniscus deformation influences wave transmission. The results are compared with simulations and limiting-case theories. We interpret that the meniscus water column formed beneath the barrier enhances flow coupling and increases wave transmission, while meniscus surface bending suppresses it by constraining motion. These competing effects explain the observed frequency and contact angle dependencies. Our findings provide insights into how meniscus dynamics govern surface wave behavior.}, archive = {J_PRL}, author = {Zhengwu Wang and Guoqin Liu and Likun Zhang}, doi = {10.1103/qb1x-qv6x}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {084001}, shortjournal = {Phys. Rev. Lett.}, title = {Meniscus-driven modulation of surface wave transmission across a barrier}, volume = {135}, year = {2025}, }
• (2025). Programmable all-optical spin simulator with artificial gauge fields. PRL, 135(8), 083804. (www)

  @article{ , abstract = {The coupling of lasers plays an important role in a variety of research activities, from generating high-power lasers to investigating out-of-equilibrium coupled systems. This Letter presents our investigations of Hermitian coupling in arrays of lasers, where it is possible to control both the amplitude and phase of the coupling and generate artificial gauge fields. The Hermitian coupling is demonstrated in three laser array geometries: a square array of 100 lasers with controlled laser coupling for obtaining continuous control over the phase-locked state, a triangular array of 130 lasers with controlled chirality of the lasers, and a ring array of eight lasers with a controlled topological charge. In the square array, we implemented arbitrary laser coupling with a precision of 2 π / 120 radians, enabling the attainment of arbitrary phase-locking states. In the triangular array, we controlled the chirality of the lasers with 99% purity. In the ring array, the introduction of an artificial gauge field revealed discrete quantized first-order transitions between distinct topological phase-locking states. The results pave the way for exploring spin systems with programmable coupling in an all-optical spin simulator.}, archive = {J_PRL}, author = {Simon Mahler and Eran Bernstein and Sagie Gadasi and Geva Arwas and Asher A. Friesem and Nir Davidson}, doi = {10.1103/chxf-fq9v}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {083804}, shortjournal = {Phys. Rev. Lett.}, title = {Programmable all-optical spin simulator with artificial gauge fields}, volume = {135}, year = {2025}, }
• (2025). Far-field excitation of a photonic flat band via a tailored anapole mode. PRL, 135(8), 083803. (www)

  @article{ , abstract = {The photonic flat band, defined by minimal dispersion and near-zero group velocity, has facilitated significant advances in optical technologies. The practical applications of flat bands, such as enhanced light-matter interactions, require efficient coupling to far-field radiation. However, achieving controlled coupling between flat bands and their corresponding localized modes with far-field radiation remains challenging and elusive. Here, we achieve the tunable far-field excitation of a flat band in the near-infrared spectral range by coupling it to a photonic anapole mode. Distinct from conventional multipolar resonances in both its physical nature and unique radiation dynamics, the anapole mode offers highly localized field distributions and tunable emission characteristics, enabling the realization of a photonic flat band and precise control over its transition from a nonradiative to a radiative state. We directly observed the flat band within ± 25 ° experimentally by angle-resolved far-field transmissivity spectroscopy. Simulation results extending to 90° confirm the persistence of the band’s flatness across all incident angles, validating the inherent flatness of the band. Our findings not only provide a viable approach to accessing photonic flat bands but also significantly advance the field of nanoscale photonic manipulation, offering broad potential applications in optical technologies.}, archive = {J_PRL}, author = {Peiwen Ren and Junrong Zheng and Zhuo Huang and Yan Liu and Long Zhang and Hua Zhang and Jingwen Ma and Zhanghai Chen and Jian-Feng Li and Jun Yi and Zhilin Yang}, doi = {10.1103/bzpw-7h2x}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {083803}, shortjournal = {Phys. Rev. Lett.}, title = {Far-field excitation of a photonic flat band via a tailored anapole mode}, volume = {135}, year = {2025}, }
• (2025). Multiple exceptional rings in one-dimensional perovskite photonic crystals. PRL, 135(8), 083802. (www)

  @article{ , abstract = {Exceptional rings (ERs) are high-dimensional non-Hermitian topologies formed by exceptional points, significantly enriching the topological properties of non-Hermitian systems. Because of the intricate topology and symmetry requirements, the realization of ERs generally demands complex structures and precise parameter tuning, resulting in relatively few experimental observations in high-dimensional periodic systems. Here, we show that even the simplest 1D non-Hermitian periodic systems can support multiple ERs, enabled by the system’s multiple degrees of freedom which naturally accommodate diverse non-Hermitian perturbations. The proposed system can host one to four ERs as well as hybrid ER by simply tuning the non-Hermitian loss, with a bulk Fermi torus in momentum space serving as the fundamental origin of this tunability. Through experiments using 1D perovskite photonic crystals, we observe the ERs associated bulk Fermi torus at visible frequencies. Our work establishes a simple platform for realizing complex non-Hermitian topologies, enabling optical-frequency applications harnessing non-Hermitian physics.}, archive = {J_PRL}, author = {Zhi-Hang Na and Xu-Lin Zhang and Jing Feng}, doi = {10.1103/clbx-mh6y}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {083802}, shortjournal = {Phys. Rev. Lett.}, title = {Multiple exceptional rings in one-dimensional perovskite photonic crystals}, volume = {135}, year = {2025}, }
• (2025). Space-time optical hopfion crystals. PRL, 135(8), 083801. (www)

  @article{ , abstract = {Hopfions—higher-dimensional topological quasiparticles with sophisticated 3D knotted spin textures discovered in condensed matter and photonic systems—show promise in high-density data storage and transfer. Here, we present crystalline structures of hopfions lying in space-time constructed by spatiotemporally structured light. Practical methodologies using bichromatic structured light beams or dipole arrays to assemble 1D and higher dimensional hopfion lattices are proposed, and a technique for tailoring topological orders is elucidated. Optical hopfion crystals constitute a new platform for high-dimensional topological information transfer.}, archive = {J_PRL}, author = {Wenbo Lin and Nilo Mata-Cervera and Yasutomo Ota and Yijie Shen and Satoshi Iwamoto}, doi = {10.1103/hh5s-cprt}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {083801}, shortjournal = {Phys. Rev. Lett.}, title = {Space-time optical hopfion crystals}, volume = {135}, year = {2025}, }
• (2025). Quantum delocalization of a levitated nanoparticle. PRL, 135(8), 083601. (www)

  @article{ , abstract = {Matter waves have been observed in double-slit experiments with microscopic objects, such as atoms or molecules. The wave function describing the motion of these objects must extend over a distance comparable to the slit separation, much larger than the characteristic size of the objects. Preparing such states for more massive objects, such as mechanical oscillators, remains an outstanding challenge. Here we delocalize the quantum ground state of an optically levitated nanosphere by modulating the stiffness of the confining potential. We show a more than threefold increase of the initial coherence length, which corresponds to mechanical momentum squeezing of more than 7 dB. Our work is a stepping stone toward the generation of coherence lengths comparable to the object size, a crucial regime for macroscopic quantum experiments.}, archive = {J_PRL}, author = {M. Rossi and A. Militaru and N. Carlon Zambon and A. Riera-Campeny and O. Romero-Isart and M. Frimmer and L. Novotny}, doi = {10.1103/2yzc-fsm3}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {083601}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum delocalization of a levitated nanoparticle}, volume = {135}, year = {2025}, }
• (2025). Imaging valence electron rearrangement in a chemical reaction using hard X-ray scattering. PRL, 135(8), 083001. (www)

  @article{ , abstract = {We have observed the signatures of valence electron rearrangement in photoexcited ammonia using ultrafast hard x-ray scattering. Time-resolved x-ray scattering is a powerful tool for imaging structural dynamics in molecules because of the strong scattering from the core electrons localized near each nucleus. Such core-electron contributions generally dominate the differential scattering signal, masking any signatures of rearrangement in the chemically important valence electrons. Ammonia represents an exception to the typically high core-to-valence electron ratio. We measured 9.8 keV x-ray scattering from gas-phase deuterated ammonia following photoexcitation via a 200 nm pump pulse to the 3s Rydberg state. We observed changes in the recorded scattering patterns due to the initial photoexcitation and subsequent deuterium dissociation. Ab initio calculations confirm that the observed signal is sensitive to the rearrangement of the single photoexcited valence electron as well as the interplay between adiabatic and nonadiabatic dissociation channels. The use of ultrafast hard x-ray scattering to image the structural rearrangement of single valence electrons constitutes an important advance in tracking valence electronic structure in photoexcited atoms and molecules.}, archive = {J_PRL}, author = {Ian Gabalski and Alice Green and Philipp Lenzen and Felix Allum and Matthew Bain and Surjendu Bhattacharyya and Mathew A. Britton and Elio G. Champenois and Xinxin Cheng and James P. Cryan and Taran Driver and Ruaridh Forbes and Douglas Garratt and Aaron M. Ghrist and Martin Graßl and Matthias F. Kling and Kirk A. Larsen and Mengning Liang and Ming-Fu Lin and Yusong Liu and Michael P. Minitti and Silke Nelson and Joseph S. Robinson and Philip H. Bucksbaum and Thomas J. A. Wolf and Nanna H. List and James M. Glownia}, doi = {10.1103/53h3-vykl}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {083001}, shortjournal = {Phys. Rev. Lett.}, title = {Imaging valence electron rearrangement in a chemical reaction using hard X-ray scattering}, volume = {135}, year = {2025}, }
• (2025). Half-life and precision shape measurement of the 2νββ decay of te130. PRL, 135(8), 082501. (www)

  @article{ , abstract = {We present a new measurement of the half-life of ( ) using the first complete model of the CUORE data, based on 1038 kg yr of collected exposure. Thanks to optimized data selection, we achieve a factor of two improvement in precision, obtaining . The signal-to-background ratio is increased by 70% compared to our previous results, enabling the first application of the improved formalism to . Within this framework, we determine a credibility interval for the effective axial coupling in the nuclear medium as a function of nuclear matrix elements. We also extract values for the higher-order nuclear matrix element ratios: second-to-first and third-to-first. The second-to-first ratio agrees with nuclear model predictions, while the third-to-first ratio deviates from theoretical expectations. These findings provide essential tests of nuclear models and key inputs for future searches.}, archive = {J_PRL}, author = {CUORE Collaboration and D. Q. Adams and C. Alduino and K. Alfonso and A. Armatol and F. T. Avignone, III and O. Azzolini and G. Bari and F. Bellini and G. Benato and M. Beretta and M. Biassoni and A. Branca and C. Brofferio and C. Bucci and J. Camilleri and A. Caminata and A. Campani and J. Cao and C. Capelli and S. Capelli and L. Cappelli and L. Cardani and P. Carniti and N. Casali and E. Celi and D. Chiesa and M. Clemenza and S. Copello and O. Cremonesi and R. J. Creswick and A. D’Addabbo and I. Dafinei and S. Dell’Oro and S. Di Domizio and S. Di Lorenzo and T. Dixon and D. Q. Fang and M. Faverzani and E. Ferri and F. Ferroni and E. Fiorini and M. A. Franceschi and S. J. Freedman and S. H. Fu and B. K. Fujikawa and S. Ghislandi and A. Giachero and M. Girola and L. Gironi and A. Giuliani and P. Gorla and C. Gotti and P. V. Guillaumon and T. D. Gutierrez and K. Han and E. V. Hansen and K. M. Heeger and D. L. Helis and H. Z. Huang and M. T. Hurst and G. Keppel and Yu. G. Kolomensky and R. Kowalski and R. Liu and L. Ma and Y. G. Ma and L. Marini and R. H. Maruyama and D. Mayer and Y. Mei and M. N. Moore and T. Napolitano and M. Nastasi and C. Nones and E. B. Norman and A. Nucciotti and I. Nutini and T. O’Donnell and M. Olmi and B. T. Oregui and S. Pagan and C. E. Pagliarone and L. Pagnanini and M. Pallavicini and L. Pattavina and M. Pavan and G. Pessina and V. Pettinacci and C. Pira and S. Pirro and E. G. Pottebaum and S. Pozzi and E. Previtali and A. Puiu and S. Quitadamo and A. Ressa and C. Rosenfeld and B. Schmidt and R. Serino and A. Shaikina and V. Sharma and V. Singh and M. Sisti and D. Speller and P. T. Surukuchi and L. Taffarello and C. Tomei and A. Torres and J. A. Torres and K. J. Vetter and M. Vignati and S. L. Wagaarachchi and B. Welliver and J. Wilson and K. Wilson and L. A. Winslow and F. Xie and T. Zhu and S. Zimmermann and S. Zucchelli and D. Castillo and J. Kotila and J. Menéndez and O. Niţescu and F. Šimkovic}, doi = {10.1103/jdhf-hn4l}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {082501}, shortjournal = {Phys. Rev. Lett.}, title = {Half-life and precision shape measurement of the 2νββ decay of te130}, volume = {135}, year = {2025}, }
• (2025). Search for an anomalous production of charged-current νe interactions without visible pions across multiple kinematic observables in MicroBooNE. PRL, 135(8), 081802. (www)

  @article{ , abstract = {This Letter presents an investigation of low-energy electron-neutrino interactions in the Fermilab Booster Neutrino Beam by the MicroBooNE experiment, motivated by the excess of electron-neutrino-like events observed by the MiniBooNE experiment. This is the first measurement to use data from all five years of operation of the MicroBooNE experiment, corresponding to an exposure of protons on target, a 70% increase on past results. Two samples of electron neutrino interactions without visible pions are used, one with visible protons and one without any visible protons. The MicroBooNE data show reasonable agreement with the nominal prediction, with values when the two samples are combined, though the prediction exceeds the data in limited regions of phase space. The data are further compared to two empirical models that modify the predicted rate of electron-neutrino interactions in different variables in the simulation to match the unfolded MiniBooNE low energy excess. In the first model, this unfolding is performed as a function of electron neutrino energy, while the second model aims to match the observed shower energy and angle distributions of the MiniBooNE excess. This measurement excludes an electronlike interpretation of the MiniBooNE excess based on these models at in all kinematic variables.}, archive = {J_PRL}, author = {MicroBooNE Collaboration and P. Abratenko and D. Andrade Aldana and L. Arellano and J. Asaadi and A. Ashkenazi and S. Balasubramanian and B. Baller and A. Barnard and G. Barr and D. Barrow and J. Barrow and V. Basque and J. Bateman and O. Benevides Rodrigues and S. Berkman and A. Bhat and M. Bhattacharya and M. Bishai and A. Blake and B. Bogart and T. Bolton and M. B. Brunetti and L. Camilleri and D. Caratelli and F. Cavanna and G. Cerati and A. Chappell and Y. Chen and J. M. Conrad and M. Convery and L. Cooper-Troendle and J. I. Crespo-Anadón and R. Cross and M. Del Tutto and S. R. Dennis and P. Detje and R. Diurba and Z. Djurcic and K. Duffy and S. Dytman and B. Eberly and P. Englezos and A. Ereditato and J. J. Evans and C. Fang and W. Foreman and B. T. Fleming and D. Franco and A. P. Furmanski and F. Gao and D. Garcia-Gamez and S. Gardiner and G. Ge and S. Gollapinni and E. Gramellini and P. Green and H. Greenlee and L. Gu and W. Gu and R. Guenette and P. Guzowski and L. Hagaman and M. D. Handley and O. Hen and C. Hilgenberg and G. A. Horton-Smith and A. Hussain and B. Irwin and M. S. Ismail and C. James and X. Ji and J. H. Jo and R. A. Johnson and Y.-J. Jwa and D. Kalra and G. Karagiorgi and W. Ketchum and M. Kirby and T. Kobilarcik and N. Lane and J.-Y. Li and Y. Li and K. Lin and B. R. Littlejohn and L. Liu and W. C. Louis and X. Luo and T. Mahmud and C. Mariani and D. Marsden and J. Marshall and N. Martinez and D. A. Martinez Caicedo and S. Martynenko and A. Mastbaum and I. Mawby and N. McConkey and L. Mellet and J. Mendez and J. Micallef and A. Mogan and T. Mohayai and M. Mooney and A. F. Moor and C. D. Moore and L. Mora Lepin and M. M. Moudgalya and S. Mulleriababu and D. Naples and A. Navrer-Agasson and N. Nayak and M. Nebot-Guinot and C. Nguyen and J. Nowak and N. Oza and O. Palamara and N. Pallat and V. Paolone and A. Papadopoulou and V. Papavassiliou and H. B. Parkinson and S. F. Pate and N. Patel and Z. Pavlovic and E. Piasetzky and K. Pletcher and I. Pophale and X. Qian and J. L. Raaf and V. Radeka and A. Rafique and M. Reggiani-Guzzo and J. Rodriguez Rondon and M. Rosenberg and M. Ross-Lonergan and I. Safa and D. W. Schmitz and A. Schukraft and W. Seligman and M. H. Shaevitz and R. Sharankova and J. Shi and E. L. Snider and M. Soderberg and S. Söldner-Rembold and J. Spitz and M. Stancari and J. St. John and T. Strauss and A. M. Szelc and N. Taniuchi and K. Terao and C. Thorpe and D. Torbunov and D. Totani and M. Toups and A. Trettin and Y.-T. Tsai and J. Tyler and M. A. Uchida and T. Usher and B. Viren and J. Wang and M. Weber and H. Wei and A. J. White and S. Wolbers and T. Wongjirad and M. Wospakrik and K. Wresilo and W. Wu and E. Yandel and T. Yang and L. E. Yates and H. W. Yu and G. P. Zeller and J. Zennamo and C. Zhang}, doi = {10.1103/x259-z6mf}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081802}, shortjournal = {Phys. Rev. Lett.}, title = {Search for an anomalous production of charged-current νe interactions without visible pions across multiple kinematic observables in MicroBooNE}, volume = {135}, year = {2025}, }
• (2025). Toward a robust confirmation or refutation of the sterile-neutrino explanation of short-baseline anomalies. PRL, 135(8), 081801. (www)

  @article{ , abstract = {The sterile neutrino interpretation of the LSND and MiniBooNE neutrino anomalies is currently being tested at three liquid argon detectors: MicroBooNE, SBND, and ICARUS. It has been argued that a degeneracy between ν μ → ν e and ν e → ν e oscillations significantly degrades their sensitivity to sterile neutrinos. Through an independent study, we show two methods to eliminate this concern. First, we resolve this degeneracy by including external constraints on ν e disappearance from the PROSPECT reactor experiment. Second, by properly analyzing the full three-dimensional parameter space, we demonstrate that the stronger-than-sensitivity exclusion from MicroBooNE alone already covers the entire 2 σ preferred regions of MiniBooNE at the level of 2 − 3 σ . We show that upcoming searches at SBND and ICARUS can improve on this beyond the 4 σ level, thereby providing a rigorous test of short-baseline anomalies.}, archive = {J_PRL}, author = {Ohana Benevides Rodrigues and Matheus Hostert and Kevin J. Kelly and Bryce Littlejohn and Pedro A. N. Machado and Ibrahim Safa and Tao Zhou}, doi = {10.1103/4fn7-svnh}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081801}, shortjournal = {Phys. Rev. Lett.}, title = {Toward a robust confirmation or refutation of the sterile-neutrino explanation of short-baseline anomalies}, volume = {135}, year = {2025}, }
• (2025). Giant graviton correlators as defect systems. PRL, 135(8), 081602. (www)

  @article{ , abstract = {We consider correlation functions of two maximal giant gravitons and two light 1 2 -BPS (Bogomol’nyi–Prasad–Sommerfield) operators in 4D N = 4 SYM (super Yang-Mills). Viewed as two-point correlators in the presence of a zero-dimensional defect, they can be completely fixed at strong coupling using analytic bootstrap techniques. We determine all infinitely such correlators for arbitrary light 1 2 -BPS operators and find that the result can be repackaged into a simple generating function thanks to a hidden higher-dimensional symmetry. We also find evidence that the same symmetry holds at weak coupling for loop correction integrands.}, archive = {J_PRL}, author = {Junding Chen (陈俊定 and Yunfeng Jiang (江云峰 and Xinan Zhou (周稀楠}, doi = {10.1103/hg9p-hblr}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081602}, shortjournal = {Phys. Rev. Lett.}, title = {Giant graviton correlators as defect systems}, volume = {135}, year = {2025}, }
• (2025). Resurgence of TT¯-deformed partition function. PRL, 135(8), 081601. (www)

  @article{ , abstract = {We study nonperturbative effects of torus partition function of the -deformed 2D conformal field theory (CFT) by resurgence in this Letter and a companion paper. The deformed partition function can be written as an infinite series of the deformation parameter . We develop highly efficient methods to compute perturbative coefficients in the expansion. To exemplify, the first 600 coefficients for the -deformed free boson and free fermion are computed. The method can be generalized to any rational CFTs; we present the key idea in this Letter while relegating details and results to the companion paper. Equipped with the large order perturbative data, we provide convincing numerical evidence that the series is asymptotic and not Borel resummable. We extract the nonperturbative contribution by resurgence and propose that they originate from new complex saddle points after analytically continuing the modular parameters in the integral representation of the partition function. The proposal is checked by comparing the predicted asymptotic behavior of the coefficients and large order perturbative data, which match nicely. The implications of these nonperturbative contributions for the Stokes phenomenon, which relates the positive and negative signs of , as well as possible comparisons with holography, is also discussed.}, archive = {J_PRL}, author = {Jie Gu and Yunfeng Jiang and Huajia Wang}, doi = {10.1103/nlmd-b57j}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081601}, shortjournal = {Phys. Rev. Lett.}, title = {Resurgence of TT¯-deformed partition function}, volume = {135}, year = {2025}, }
• (2025). Interface modes in inspiralling neutron stars: A gravitational-wave probe of first-order phase transitions. PRL, 135(8), 081402. (www)

  @article{ , abstract = {At the extreme densities in neutron stars, a phase transition to deconfined quark matter is anticipated. Yet masses, radii, and tidal deformabilities offer only indirect measures of a first-order phase transition, requiring many detections to resolve or being ineffective observables if the discontinuity exists at lower densities. We report on a smoking-gun gravitational-wave signature of a first-order transition: the resonant tidal excitation of an interface mode. Using relativistic perturbation theory with an equation-of-state family informed by chiral effective field theory, we show that such a resonance may be detectable with next-generation interferometers and possibly already with LIGO A + for sufficiently loud events.}, archive = {J_PRL}, author = {A. R. Counsell and F. Gittins and N. Andersson and I. Tews}, doi = {10.1103/8hvq-6dy7}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081402}, shortjournal = {Phys. Rev. Lett.}, title = {Interface modes in inspiralling neutron stars: A gravitational-wave probe of first-order phase transitions}, volume = {135}, year = {2025}, }
• (2025). Multimessenger detection of black hole binaries in dark matter spikes. PRL, 135(8), 081401. (www)

  @article{ , abstract = {We investigate the inspiral of a high mass-ratio black hole binary located in the nucleus of a galaxy, where the primary central black hole is surrounded by a dense dark matter spike formed through accretion during the black hole growth phase. Within this spike, dark matter undergoes strong self-annihilation, producing a compact source of γ -ray radiation that is highly sensitive to spike density, while the binary emits gravitational waves at frequencies detectable by LISA. As the inspiraling binary interacts with the surrounding dark matter particles, it alters the density of the spike, thereby influencing the γ -ray flux from dark matter annihilation. We demonstrate that the spike self-annihilation luminosity decreases by 10% to 90% of its initial value, depending on the initial density profile and binary mass ratio, as the binary sweeps through the LISA band. This presents a new opportunity to indirectly probe dark matter through multimessenger observations of galactic nuclei.}, archive = {J_PRL}, author = {Fani Dosopoulou and Joseph Silk}, doi = {10.1103/hysg-5273}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081401}, shortjournal = {Phys. Rev. Lett.}, title = {Multimessenger detection of black hole binaries in dark matter spikes}, volume = {135}, year = {2025}, }
• (2025). Positive neutrino masses with DESI DR2 via matter conversion to dark energy. PRL, 135(8), 081003. (www)

  @article{ , abstract = {The Dark Energy Spectroscopic Instrument (DESI) is a massively parallel spectroscopic survey on the Mayall telescope at Kitt Peak, which has released measurements of baryon acoustic oscillations determined from over 14 million extragalactic targets. We combine DESI Data Release 2 with CMB datasets to search for evidence of matter conversion to dark energy (DE), focusing on a scenario mediated by stellar collapse to cosmologically coupled black holes (CCBHs). In this physical model, which has the same number of free parameters as Λ CDM , DE production is determined by the cosmic star formation rate density (SFRD), allowing for distinct early- and late-time cosmologies. Using two SFRDs to bracket current observations, we find that the CCBH model: accurately recovers the cosmological expansion history, agrees with early-time baryon abundance measured by BBN, reduces tension with the local distance ladder, and relaxes constraints on the summed neutrino mass ∑ m ν . For these SFRDs, we find a peaked positive ∑ m ν < 0.149 eV (95% confidence) and ∑ m ν = 0.106 − 0.069 + 0.050 eV , respectively, in good agreement with lower limits from neutrino oscillation experiments. A peak in ∑ m ν > 0 results from late-time baryon consumption in the CCBH scenario and is expected to be a general feature of any model that converts sufficient matter to dark energy during and after reionization.}, archive = {J_PRL}, author = {DESI Collaboration and S. P. Ahlen and A. Aviles and B. Cartwright and K. S. Croker and W. Elbers and D. Farrah and N. Fernandez and G. Niz and J. W. Rohlf and G. Tarlé and R. A. Windhorst and J. Aguilar and U. Andrade and D. Bianchi and D. Brooks and T. Claybaugh and A. de la Macorra and A. de Mattia and B. Dey and P. Doel and J. E. Forero-Romero and E. Gaztañaga and S. Gontcho A. Gontcho and G. Gutierrez and D. Huterer and M. Ishak and R. Kehoe and D. Kirkby and A. Kremin and O. Lahav and C. Lamman and M. Landriau and L. Le Guillou and M. E. Levi and M. Manera and R. Miquel and J. Moustakas and I. Pérez-Ràfols and F. Prada and G. Rossi and E. Sanchez and M. Schubnell and H. Seo and J. Silber and D. Sprayberry and M. Walther and B. A. Weaver and R. H. Wechsler and H. Zou}, doi = {10.1103/yb2k-kn7h}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081003}, shortjournal = {Phys. Rev. Lett.}, title = {Positive neutrino masses with DESI DR2 via matter conversion to dark energy}, volume = {135}, year = {2025}, }
• (2025). First sub-MeV dark matter search with the QROCODILE experiment using superconducting nanowire single-photon detectors. PRL, 135(8), 081002. (www)

  @article{ , abstract = {We present the first results from the Quantum Resolution-Optimized Cryogenic Observatory for Dark matter Incident at Low Energy (QROCODILE). The QROCODILE experiment uses a microwire-based superconducting nanowire single-photon detector (SNSPD) as a target and sensor for dark matter scattering and absorption, and is sensitive to energy deposits as low as 0.11 eV. We introduce the experimental configuration and report new world-leading constraints on the interactions of sub-MeV dark matter particles with masses as low as 30 keV. The thin-layer geometry of the system provides anisotropy in the interaction rate, enabling directional sensitivity. In addition, we leverage the coupling between phonons and quasiparticles in the detector to simultaneously constrain interactions with both electrons and nucleons. We discuss the potential for improvements to both the energy threshold and effective volume of the experiment in the coming years.}, archive = {J_PRL}, author = {Laura Baudis and Alexander Bismark and Noah Brugger and Chiara Capelli and Ilya Charaev and Jose Cuenca García and Guy Daniel Hadas and Yonit Hochberg and Judith K. Hohmann and Alexander Kavner and Christian Koos and Artem Kuzmin and Benjamin V. Lehmann and Severin Nägeli and Titus Neupert and Bjoern Penning and Diego Ramírez García and Andreas Schilling}, doi = {10.1103/4hb6-f6jl}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081002}, shortjournal = {Phys. Rev. Lett.}, title = {First sub-MeV dark matter search with the QROCODILE experiment using superconducting nanowire single-photon detectors}, volume = {135}, year = {2025}, }
• (2025). Assessing cosmological evidence for nonminimal coupling. PRL, 135(8), 081001. (www)

  @article{ , abstract = {The recent observational evidence of deviations from the Lambda cold dark matter model points toward the presence of evolving dark energy. The simplest possibility consists of a cosmological scalar field φ , dubbed “quintessence,” driving the accelerated expansion. We assess the evidence for the existence of such a scalar field. We find that, if the accelerated expansion is driven by quintessence, the data favor a potential energy V ( φ ) that is concave, i.e., m 2 = d 2 V / d φ 2 < 0 . Furthermore, and more significantly, the data strongly favor a scalar field that is nonminimally coupled to gravity [Bayes factor log ( B ) = 7.34 ± 0.6 ], leading to time variations in the gravitational constant on cosmological scales, and the existence of fifth forces on smaller scales. The fact that we do not observe such fifth forces implies that either new physics must come into play on noncosmological scales or that quintessence is an unlikely explanation for the observed cosmic acceleration.}, archive = {J_PRL}, author = {William J. Wolf and Carlos García-García and Theodore Anton and Pedro G. Ferreira}, doi = {10.1103/jysf-k72m}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {081001}, shortjournal = {Phys. Rev. Lett.}, title = {Assessing cosmological evidence for nonminimal coupling}, volume = {135}, year = {2025}, }
• (2025). Photon-interfaced ten-qubit register of trapped ions. PRL, 135(8), 080801. (www)

  @article{ , abstract = {Establishing networks of quantum processors offers a path to scalable quantum computing and applications in communication and sensing. This requires first developing efficient interfaces between photons and multiqubit registers. In this Letter, we show how to entangle each individual matter qubit in a register of ten to a separate traveling photon. The qubits are encoded in a string of cotrapped atomic ions. By switching the trap confinement, ions are brought one at a time into the waist of an optical cavity and emit a photon via a laser-driven cavity-mediated Raman transition. The result is a train of photonic qubits, each near-maximally entangled by their polarization with a different ion qubit in the string. An average ion-photon Bell state fidelity of 92% is achieved, for an average probability for detecting each single photon of 9%. The technique is directly scalable to larger ion-qubit registers and opens up the near-term possibility of entangling distributed networks of trapped-ion quantum processors, sensing arrays, and clocks.}, archive = {J_PRL}, author = {M. Canteri and Z. X. Koong and J. Bate and A. Winkler and V. Krutyanskiy and B. P. Lanyon}, doi = {10.1103/v5k1-whwz}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {080801}, shortjournal = {Phys. Rev. Lett.}, title = {Photon-interfaced ten-qubit register of trapped ions}, volume = {135}, year = {2025}, }
• (2025). Neural quantum embedding via deterministic quantum computation with one qubit. PRL, 135(8), 080603. (www)

  @article{ , abstract = {Quantum computing is expected to provide an exponential speedup in machine learning. However, optimizing the data loading process, commonly referred to as “quantum data embedding,” to maximize classification performance remains a critical challenge. In this Letter, we propose a neural quantum embedding (NQE) technique based on deterministic quantum computation with one qubit (DQC1). Unlike the traditional embedding approach, NQE trains a neural network to maximize the trace distance between quantum states corresponding to different categories of classical data. Furthermore, training is efficiently achieved using DQC1, which is specifically designed for ensemble quantum systems, such as nuclear magnetic resonance (NMR). We validate the NQE-DQC1 protocol by encoding handwritten images into NMR quantum processors, demonstrating a significant improvement in distinguishability compared to traditional methods. Additionally, after training the NQE, we implement a parametrized quantum circuit for classification tasks, achieving 98% classification accuracy, in contrast to the 54% accuracy obtained using traditional embedding. Moreover, we show that the NQE-DQC1 protocol is extendable, enabling the use of the NMR system for NQE training due to its high compatibility with DQC1, while subsequent machine learning tasks can be performed on other physical platforms, such as superconducting circuits. Our Letter opens new avenues for utilizing ensemble quantum systems for efficient classical data embedding into quantum registers.}, archive = {J_PRL}, author = {Hongfeng Liu and Tak Hur and Shitao Zhang and Liangyu Che and Xinyue Long and Xiangyu Wang and Keyi Huang and Yu-ang Fan and Yuxuan Zheng and Yufang Feng and Yu Zhou and Jack Ng and Xinfang Nie and Daniel K. Park and Dawei Lu}, doi = {10.1103/y8wr-yml4}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {080603}, shortjournal = {Phys. Rev. Lett.}, title = {Neural quantum embedding via deterministic quantum computation with one qubit}, volume = {135}, year = {2025}, }
• (2025). Exponential quantum speedup for simulating classical lattice dynamics. PRL, 135(8), 080602. (www)

  @article{ , abstract = {Simulating large-scale lattice dynamics remains a long-standing challenge in condensed matter and materials science, where mechanical and thermal behaviors arise from coupled vibrational modes. We introduce a quantum algorithm that reformulates general harmonic lattice dynamics as a time-dependent Schrödinger equation governed by a sparse, Hermitian Hamiltonian. This enables the use of Hamiltonian simulation techniques on quantum devices, offering exponential speedup in the number of atoms . Our approach applies to arbitrary harmonic lattices with vector-valued dynamics. A key ingredient is a matrix-valued Fejér-Riesz factorization of the phonon dynamical matrix, which preserves translational symmetry and enables efficient assembly of the Hamiltonian operator. We demonstrate the method’s applicability across a broad class of lattice models.}, archive = {J_PRL}, author = {Xiantao Li}, doi = {10.1103/z2jq-1rxp}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {080602}, shortjournal = {Phys. Rev. Lett.}, title = {Exponential quantum speedup for simulating classical lattice dynamics}, volume = {135}, year = {2025}, }
• (2025). Surface-morphology-assisted trapping of strongly coupled electron-on-neon charge states. PRL, 135(8), 080601. (www)

  @article{ , abstract = {Single electrons confined to a free neon surface and manipulated through the circuit quantum electrodynamics architecture is a promising novel quantum computing platform. Understanding the exact physical nature of the electron-on-neon ( e Ne ) charge states is important for realizing this platform’s potential for quantum technologies. We investigate how resonator trench depth and substrate surface properties influence the formation of e Ne charge states and their coupling to microwave resonators. Through experimental observation supported by modeling, we find that shallow-depth etching of the resonator features maximizes coupling strength. By comparing the trapping statistics and surface morphology of devices with altered trench roughness, our Letter reveals the role of fabrication-induced surface features in the formation of strongly coupled e Ne states.}, archive = {J_PRL}, author = {Kaiwen Zheng and Xingrui Song and Kater W. Murch}, doi = {10.1103/8v7d-53x7}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {080601}, shortjournal = {Phys. Rev. Lett.}, title = {Surface-morphology-assisted trapping of strongly coupled electron-on-neon charge states}, volume = {135}, year = {2025}, }
• (2025). Multipartite entanglement structure of monitored quantum circuits. PRL, 135(8), 080401. (www)

  @article{ , abstract = {Monitored quantum circuits have attracted significant interest as an example of synthetic quantum matter, intrinsically defined by their quantum information content. Here, we propose a multipartite entanglement perspective on monitored phases through the lens of quantum Fisher information. Our findings reveal that unstructured monitored random circuits fail to exhibit divergent multipartite entanglement even at criticality, highlighting their departure from standard quantum critical behavior. However, we demonstrate that genuinely multipartite entangled phases can be realized through two-site measurements, provided a protection mechanism is in place. This work positions multipartite entanglement as a valuable perspective for the study of interacting monitored circuits and broader frameworks of noisy quantum dynamics.}, archive = {J_PRL}, author = {Arnau Lira-Solanilla and Xhek Turkeshi and Silvia Pappalardi}, doi = {10.1103/fl34-h1p1}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {080401}, shortjournal = {Phys. Rev. Lett.}, title = {Multipartite entanglement structure of monitored quantum circuits}, volume = {135}, year = {2025}, }
• (2025). Essay: Photonic crystals as a platform to explore new physics. PRL, 135(8), 080001. (www)

  @article{ , abstract = {Photonic crystals are artificial materials characterized by a photonic band structure that governs the propagation of light waves. The photonic gap was originally introduced to inhibit spontaneous emission and facilitate photon localization. In this essay, I will highlight how, despite the established understanding of photonic crystals, they remain highly relevant today. Their design flexibility, the duality symmetry inherent in Maxwell’s equations, and their functionality across a wide frequency range all allow the exploration of new areas in physics, each revealing unique phenomena. Examples include band topology and topological effects in structured light fields, as well as geometric concepts such as quantum geometry and the properties of non-Euclidean spaces. Furthermore, photonic crystals provide a valuable platform for studying non-Hermitian physics, including exceptional points and the non-Hermitian skin effect. Beyond their fundamental significance, these properties hold promise for advancing photonic technologies.}, archive = {J_PRL}, author = {Che Ting Chan}, doi = {10.1103/kglg-yzcm}, journal = {Physical Review Letters}, month = {8}, number = {8}, pages = {080001}, shortjournal = {Phys. Rev. Lett.}, title = {Essay: Photonic crystals as a platform to explore new physics}, volume = {135}, year = {2025}, }
• (2025). Erratum: Enhancement of rydberg blockade via microwave dressing [Phys. rev. lett. 134, 123404 (2025)]. PRL, 135(7), 079902. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 079902 (2025)}, archive = {J_PRL}, author = {Deniz Kurdak and Patrick R. Banner and Yaxin Li and Sean R. Muleady and Alexey V. Gorshkov and S. L. Rolston and J. V. Porto}, doi = {10.1103/bsxt-fp85}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {079902}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Enhancement of rydberg blockade via microwave dressing [Phys. rev. lett. 134, 123404 (2025)]}, volume = {135}, year = {2025}, }
• (2025). Erratum: Thermal area law in long-range interacting systems [Phys. rev. lett. 134, 020402 (2025)]. PRL, 135(7), 079901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 079901 (2025)}, archive = {J_PRL}, author = {Donghoon Kim and Tomotaka Kuwahara and Keiji Saito}, doi = {10.1103/3dm5-5kqc}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {079901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Thermal area law in long-range interacting systems [Phys. rev. lett. 134, 020402 (2025)]}, volume = {135}, year = {2025}, }
• (2025). Coherent dynamics of molecular vibrations in single plasmonic nanogaps. PRL, 135(7), 076901. (www)

  @article{ , abstract = {Coupling with a resonant optical cavity is well known to modify the coherence of molecular vibrations. However, in the case of molecules coupled to a plasmonic nanocavity mode, the local mechanisms of vibrational coherence decay remain unclear. Here, the dynamics of a few hundred molecules of nitrothiophenol (NTP) within a single plasmonic nanocavity are studied by sum-frequency generation. Time-resolved experiments reveal a coherence lifetime sensitive to intermolecular dipole coupling strength, and is found to compete with cavity-induced vibrational dephasing above a threshold . Tuning of the system dipole strength presents a quantitative means to explore the energy landscape of coherent interactions within nanoscale vibrational platforms, relevant for studies from vibrational chemistry to cavity quantum optomechanics.}, archive = {J_PRL}, author = {Fiona Bell and Lukas Jakob and Caleb Todd and Ishaan Lohia and Yeeun Roh and Rakesh Arul and Jeremy J. Baumberg}, doi = {10.1103/txdw-nqvn}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076901}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent dynamics of molecular vibrations in single plasmonic nanogaps}, volume = {135}, year = {2025}, }
• (2025). Local dzyaloshinskii-moriya interactions driving quasi-2D magnetism in a centrosymmetric nanoskyrmion material. PRL, 135(7), 076706. (www)

  @article{ , abstract = {The unabating discovery of nanoskyrmions in centrosymmetric magnets challenges the conventional Dzyaloshinskii-Moriya (DM) skyrmion stabilization mechanism. We investigate Gd 2 PdSi 3 using polarized resonant x-ray scattering and find that the low-field incommensurate modulations are elliptical helices, evolving into spin-density waves at higher fields. Quasi-2D magnetism arises via local DM interactions generated by inversion symmetry breaking around Gd-Gd bonds, which we characterize using atomistic simulations. Our findings suggest a prominent “hidden” role of DM interactions even in centrosymmetric skyrmionic hosts.}, archive = {J_PRL}, author = {S. H. Moody and P. J. Bereciartua and S. Francoual and M. T. Littlehales and M. N. Wilson and M. Gomilšek and M. T. Birch and D. A. Mayoh and G. Balakrishnan and P. D. Hatton}, doi = {10.1103/td2c-dxgj}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076706}, shortjournal = {Phys. Rev. Lett.}, title = {Local dzyaloshinskii-moriya interactions driving quasi-2D magnetism in a centrosymmetric nanoskyrmion material}, volume = {135}, year = {2025}, }
• (2025). Harnessing magnetic octupole hall effect to induce torque in altermagnets. PRL, 135(7), 076705. (www)

  @article{ , abstract = {-wave altermagnets have magnetic octupoles as their order parameters [S. Bhowal and N. A. Spaldin, Ferroically ordered magnetic octupoles in -wave altermagnets, Phys. Rev. X 14 , 011019 (2024) ]. We theoretically show that magnetic octupoles injected from outside generate torque on the -wave altermagnets. The injection can be achieved by the magnetic octupole Hall effect in an adjacent layer. We calculate the magnetic octupole Hall conductivity of the heavy metal and find a sizable value comparable to its spin Hall conductivity. Our work generalizes the spin Hall phenomenology (generation by heavy metals and detection by torque in ferromagnets) to the magnetic octupole Hall phenomenology (generation by heavy metals and detection by torque in altermagnets), which can be utilized to electrically control magnetic configurations of altermagnets.}, archive = {J_PRL}, author = {Seungyun Han and Daegeun Jo and Insu Baek and Suik Cheon and Peter M. Oppeneer and Hyun-Woo Lee}, doi = {10.1103/lxkx-ypbg}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076705}, shortjournal = {Phys. Rev. Lett.}, title = {Harnessing magnetic octupole hall effect to induce torque in altermagnets}, volume = {135}, year = {2025}, }
• (2025). 1/5 and 1/3 magnetization plateaux in the spin 1/2 chain system YbAlO3. PRL, 135(7), 076704. (www)

  @article{ , abstract = {Quasi-one-dimensional magnets can host an ordered longitudinal spin-density wave state (LSDW) in magnetic field at low temperature, when longitudinal correlations are strengthened by Ising anisotropies. In the Heisenberg antiferromagnet this happens via Ising-like interchain interactions. Here, we report the first experimental observation of magnetization plateaux at and of the saturation value via thermal transport and magnetostriction measurements in . We present a phenomenological theory of the plateau states that describes them as islands of commensurability within an otherwise incommensurate LSDW phase and explains their relative positions within the LSDW phase and their relative extent in a magnetic field. Notably, the plateaux are stabilized by ferromagnetic interchain interactions in and consistently are absent in other quasi-1D magnets such as with antiferromagnetic interchain interactions. We also report a small, steplike increase of the magnetostriction coefficient, indicating a weak phase transition of unknown origin in the high-field phase just below the saturation.}, archive = {J_PRL}, author = {P. Mokhtari and S. Galeski and U. Stockert and L. Behera and S. E. Nikitin and R. Wawrzyńczak and R. Küchler and M. Brando and L. Vasylechko and O. A. Starykh and E. Hassinger}, doi = {10.1103/grfl-37g2}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076704}, shortjournal = {Phys. Rev. Lett.}, title = {1/5 and 1/3 magnetization plateaux in the spin 1/2 chain system YbAlO3}, volume = {135}, year = {2025}, }
• (2025). Chiral phonon-induced spin transport via microscopic barnett effect. PRL, 135(7), 076703. (www)

  @article{ , abstract = {Chiral phonons, which are characterized by rotational atomic motion, offer a unique mechanism for transferring angular momentum from phonons to electron spins and other angular momentum carriers. In this Letter, we present a theoretical investigation into the emergence of chiral phonons in a chiral hybrid organic-inorganic perovskite (HOIP) and their critical roles in rigid-body rotation, magnetic moment generation, and spin transport under nonthermal equilibrium conditions. We demonstrate that phonon angular momentum can modify the spin chemical potential via a proposed microscopic Barnett effect, leading to a spatially varying spin chemical potential at the metal/HOIP interface, which subsequently induces spin currents in an adjacent Cu layer, with a magnitude consistent with experimental observations. Additionally, we propose a mechanism for the intrinsic excitation of spin currents driven by chiral phonons under a parabolic temperature profile. Beyond their influence on spin transport, we also outline experimental approaches to probe chiral phonons through their distinctive mechanical and magnetic responses.}, archive = {J_PRL}, author = {Xixi Qin and Cong Yang and Dali Sun and Jun Liu and Volker Blum}, doi = {10.1103/kp6b-2kxz}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076703}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral phonon-induced spin transport via microscopic barnett effect}, volume = {135}, year = {2025}, }
• (2025). Separating terahertz spin and charge contributions from ultrathin antiferromagnetic heterostructures. PRL, 135(7), 076702. (www)

  @article{ , abstract = {Femtosecond laser excitation of nanometer thin heterostructures comprising a heavy metal and a magnetically ordered material is known to result in the emission of terahertz radiation. However, the nature of the emitted radiation from heavy metal/antiferromagnet heterostructures has sparked debates and controversies in the literature. Here, we unambiguously separate spin and charge contributions from Pt/NiO heterostructures by introducing an unprecedented methodology combining high external magnetic fields with a symmetry analysis of the emitted terahertz polarization. We observe two distinct mechanisms of terahertz emission, which we identify as optical difference frequency generation and ultrafast laser-induced quenching of the magnetization. We emphasize the absence of spin transport effects and signatures of coherent magnons. Overall, our Letter provides a general experimental methodology to separate spin and charge contributions to the laser-induced terahertz emission from heterostructures comprising a magnetically ordered material, thus holding great potential for advancing terahertz spintronics and establishing terahertz orbitronics.}, archive = {J_PRL}, author = {T. W. J. Metzger and P. Fischer and T. Kikkawa and E. Saitoh and A. V. Kimel and D. Bossini}, doi = {10.1103/76xj-j9qr}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076702}, shortjournal = {Phys. Rev. Lett.}, title = {Separating terahertz spin and charge contributions from ultrathin antiferromagnetic heterostructures}, volume = {135}, year = {2025}, }
• (2025). Substrate contribution to ultrafast spin dynamics in 2D van der waals magnets. PRL, 135(7), 076701. (www)

  @article{ , abstract = {We propose a model that is able to reproduce the type-II ultrafast demagnetization dynamics observed in 2D magnets. The spin system is coupled to the electronic thermal bath and is treated with atomistic spin dynamics, while the electron and phonon heat baths are described phenomenologically by coupled equations via the two-temperature model. Our proposed two-temperature model takes into account the effect of the heated substrate, which for 2D systems results in a slow demagnetization regime. We applied the framework to a generic 2D system, CrI 3 , and we are able to observe a type-II demagnetization process characterized by two steps, the first step being attributed to the free electrons generated when the system behaves as a quasimetal under optical excitation, and the second step, the slower demagnetization region, due to the heated substrate. Finally, after laser excitation, we are able to observe domain formation in CrI 3 , similar to recent experimental observations. Our generalized two-temperature model enhances the modeling of ultrafast magnetization dynamics processes by effectively describing the quasimetallic behavior of certain magnetic materials and the influence of a heated adjacent layer.}, archive = {J_PRL}, author = {Mara Strungaru and Richard F. L. Evans and Roy W. Chantrell}, doi = {10.1103/9q7b-jxx5}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076701}, shortjournal = {Phys. Rev. Lett.}, title = {Substrate contribution to ultrafast spin dynamics in 2D van der waals magnets}, volume = {135}, year = {2025}, }
• (2025). Hyperbolic spin liquids. PRL, 135(7), 076604. (www)

  @article{ , abstract = {Hyperbolic lattices present a unique opportunity to venture beyond the conventional paradigm of crystalline many-body physics and explore correlated phenomena in negatively curved space. As a theoretical benchmark for such investigations, we extend Kitaev’s spin- honeycomb model to hyperbolic lattices and exploit their non-Euclidean space-group symmetries to solve the model exactly. We elucidate the ground-state phase diagram on the lattice and find a gapped spin liquid with Abelian anyons, a gapped chiral spin liquid with non-Abelian anyons and chiral edge states, and a Majorana metal whose finite low-energy density of states is dominated by non-Abelian Bloch states.}, archive = {J_PRL}, author = {Patrick M. Lenggenhager and Santanu Dey and Tomáš Bzdušek and Joseph Maciejko}, doi = {10.1103/s25y-s4fj}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076604}, shortjournal = {Phys. Rev. Lett.}, title = {Hyperbolic spin liquids}, volume = {135}, year = {2025}, }
• (2025). Anyon theory and topological frustration of high-efficiency quantum low-density parity-check codes. PRL, 135(7), 076603. (www)

  @article{ , abstract = {Quantum low-density parity-check (QLDPC) codes offer a promising path to low-overhead fault-tolerant quantum computation but lack systematic strategies for exploration. In this Letter, we establish a topological framework for studying the bivariate-bicycle codes, a prominent class of QLDPC codes tailored for real-world quantum hardware. Our framework enables the investigation of these codes through universal properties of topological orders. In addition to efficient characterizations using Gröbner bases, we also introduce a novel algebraic-geometric approach based on the Bernstein-Khovanskii-Kushnirenko theorem. This approach allows us to analytically determine how the topological order varies with the generic choices of bivariate-bicycle codes under toric layouts. Novel phenomena are unveiled, including topological frustration , where ground-state degeneracy on a torus deviates from the total anyon number, and quasifractonic mobility , where anyon movement violates energy conservation. We demonstrate their intrinsic link to symmetry-enriched topological orders and derive an efficient method for generating finite-size codes. Furthermore, we extend the connection between anyons and logical operators using Koszul complex theory. Our Letter provides a rigorous theoretical basis for exploring the fault tolerance of QLDPC codes and deepens the interplay among topological order, quantum error correction, and advanced algebraic structures.}, archive = {J_PRL}, author = {Keyang Chen and Yuanting Liu and Yiming Zhang and Zijian Liang and Yu-An Chen and Ke Liu and Hao Song}, doi = {10.1103/86j7-cmsw}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076603}, shortjournal = {Phys. Rev. Lett.}, title = {Anyon theory and topological frustration of high-efficiency quantum low-density parity-check codes}, volume = {135}, year = {2025}, }
• (2025). Anderson delocalization in strongly coupled disordered non-hermitian chains. PRL, 135(7), 076602. (www)

  @article{ , abstract = {Disorder and non-Hermitian effects together can upend how waves localize. In a 1D disordered chain, the non-Hermitian skin effect (NHSE) can induce Anderson delocalization, defying the usual rule that disorder in low dimensions always localizes states. While weak disorder leaves the NHSE intact, strong disorder restores Anderson localization. Here, we study a surprising twist: coupling a strongly disordered Hatano-Nelson chain to a disordered Hermitian chain with their disorder antisymmetrically correlated. Strikingly, once the interchain coupling exceeds a threshold, the system undergoes Anderson delocalization irrespective of disorder strength, reinstating the NHSE with no Hermitian counterpart. This transition arises from the interplay of nonreciprocal hopping, interchain coupling, and engineered disorder correlations, and is captured by a real-space winding number. To confirm this, we build an electrical-circuit analog and directly observe the reemergent NHSE via voltage measurements. Our Letter uncovers unexplored and experimentally accessible physics at the crossroads of non-Hermiticity and disorder.}, archive = {J_PRL}, author = {Wei-Wu Jin and Jin Liu and Xin Wang and Yu-Ran Zhang and Xueqin Huang and Xiaomin Wei and Wenbo Ju and Zhongmin Yang and Tao Liu and Franco Nori}, doi = {10.1103/lpm2-vcb4}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076602}, shortjournal = {Phys. Rev. Lett.}, title = {Anderson delocalization in strongly coupled disordered non-hermitian chains}, volume = {135}, year = {2025}, }
• (2025). Majorana zero modes in the lieb-kitaev model with tunable quantum metric. PRL, 135(7), 076601. (www)

  @article{ , abstract = {The relation between band topology and Majorana zero energy modes (MZMs) in topological superconductors had been well studied in the past decades. However, the relation between the quantum metric and MZMs has yet to be understood. In this Letter, we first construct a three band Lieb-like lattice model with an isolated flat band and tunable quantum metric. By introducing nearest neighbor equal spin pairing, we obtain the Lieb-Kitaev model which supports MZMs. When the Fermi energy is set within the flat band energy, the MZMs, which are supposed to be well localized at the ends of the 1D superconductor due to the flatness of the band, appear. On the contrary, we show both numerically and analytically that the localization length of the MZMs is controlled by a length scale defined by the quantum metric of the flat band, which we call the quantum metric length (QML). The QML can be several orders of magnitude longer than the conventional BCS superconducting coherence length. When the QML is comparable to the length of the superconductor, the two MZMs from the two ends of the superconductor can hybridize and induce ultra long range crossed Andreev reflections. This Letter unveils how the quantum metric can greatly influence the properties of MZMs through the QML, and the results can be generalized to other topological bound states.}, archive = {J_PRL}, author = {Xingyao Guo and Xinglei Ma and Xuzhe Ying and K. T. Law}, doi = {10.1103/l3c7-knqm}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076601}, shortjournal = {Phys. Rev. Lett.}, title = {Majorana zero modes in the lieb-kitaev model with tunable quantum metric}, volume = {135}, year = {2025}, }
• (2025). Direct evidence of intrinsic mott state and its layer-parity oscillation in a breathing kagome crystal down to monolayer. PRL, 135(7), 076503. (www)

  @article{ , abstract = {We report direct spectroscopic evidence of correlation-driven Mott states in layered through combining scanning tunneling microscopy (STM) and dynamical mean-field theory. The Hubbard bands persist down to monolayer, providing the definitive evidence for the Mottness in . While the size of the Mott gap remains almost constant across all layers, a striking layer-parity-dependent oscillation emerges in the local density of states (LDOS) between even ( , 4, 6) and odd layers ( , 3, 5), which arises from the dimerization and correlation modulation of the obstructed atomic states, respectively. Our conclusions are supported by a critical technical advance in atomic-scale LDOS mapping for highly insulating systems. This Letter provides the definitive experimental verification of correlation-driven Mott ground states in , while establishing a general protocol for investigating the interplay of electronic correlation and interlayer coupling in layered insulators by using a low-temperature STM technique.}, archive = {J_PRL}, author = {Huanyu Liu and Wenhui Li and Zishu Zhou and Hongbin Qu and Jiaqi Zhang and Weixiong Hu and Chenhaoping Wen and Ning Wang and Hao Deng and Gang Li and Shichao Yan}, doi = {10.1103/mzyy-thjq}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076503}, shortjournal = {Phys. Rev. Lett.}, title = {Direct evidence of intrinsic mott state and its layer-parity oscillation in a breathing kagome crystal down to monolayer}, volume = {135}, year = {2025}, }
• (2025). Nonlinear transverse conductivity in antiferroic types of magnetic toroidal metal. PRL, 135(7), 076502. (www)

  @article{ , abstract = {We have performed careful measurements of nonlinear transverse conductivity (NLTC) at zero field in the intermetallic compound HoAgGe with two distinct magnetic toroidal (MT) structures. Below 7 K (MT1 phase), the NLTC signal becomes observable and significantly increases with decreasing temperature, whereas between 7 and 11.6 K (MT2 phase), it remains nearly zero. However, this result is incompatible with the previous research, which assigned the former and latter MT phases as antiferro- and ferro-MT structures, respectively. This discrepancy stems from an inappropriate assignment of MT structures in prior studies. Our analysis, based on multipole theory, redefines the MT1 and MT2 phases as ferri- and antiferro-MT structures, respectively, providing a coherent framework to explain the observed NLTC in HoAgGe. These findings not only establish NLTC as a robust diagnostic tool for identifying MT metals but also highlight its potential for exploring phenomena driven by the antiferroic interactions of MT dipoles.}, archive = {J_PRL}, author = {T. Miyamoto and M. Shimozawa and S. Hosoi and M. Yatsushiro and K. Izawa and Y. Ōnuki and D. Aoki and S. Hayami}, doi = {10.1103/gfl2-bsjk}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076502}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear transverse conductivity in antiferroic types of magnetic toroidal metal}, volume = {135}, year = {2025}, }
• (2025). Dimensionality-driven anomalous metallic state with zero-field nonreciprocal transport in layered ising superconductors. PRL, 135(7), 076501. (www)

  @article{ , abstract = {The anomalous metal state (AMS), observed in “failed” superconductors, provides insights into superconductivity and quantum criticality, with studies revealing unconventional quantum phases like the Bose metal. Recently, layered transition metal dichalcogenide (TMD) superconductors approaching the two-dimensional limit have garnered significant attention for the enhanced phase fluctuations and electronic correlations. Investigating AMSs in these systems, particularly in the absence of an external magnetic field, could offer valuable insights into the dimensionality-driven emergence of exotic quantum phenomena, including triplet Cooper pairing, phase fluctuation dynamics, and especially the recently discovered field-free superconducting diode effects. However, the field-free AMS has yet to be observed in TMD superconductors. Here, we report the dimensionality-tunable AMS near the superconducting quantum phase transitions in a layered TMD superconductor . In samples with thicknesses below 10 nm, we demonstrate magnetic field-driven AMS under external magnetic field, characterized by the vanishing of the Hall resistance and the presence of finite longitudinal resistance. Remarkably, an unexpected zero-field AMS emerges as the sample thickness is reduced to 3 nm. This AMS aligns well with the quantum vortex creep model and exhibits nonreciprocal transport behaviors, suggesting the onset of spontaneous time-reversal symmetry breaking accompanied by vortex motion as the system approaches the two-dimensional limit. Our findings open new avenues for exploring dimensionality-driven exotic superconducting quantum critical phases and pave the way for a deeper understanding of zero-field superconducting diode effects.}, archive = {J_PRL}, author = {Yanwei Cui and Zenglin Liu and Qin Liu and Junlin Xiong and Yongqin Xie and Yudi Dai and Ji Zhou and Lizheng Wang and Hanyan Fang and Haiwen Liu and Shi-Jun Liang and Bin Cheng and Feng Miao}, doi = {10.1103/5qvz-d3vl}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076501}, shortjournal = {Phys. Rev. Lett.}, title = {Dimensionality-driven anomalous metallic state with zero-field nonreciprocal transport in layered ising superconductors}, volume = {135}, year = {2025}, }
• (2025). Excitonic effects in phonons: Reshaping the graphene kohn anomalies and lifetimes. PRL, 135(7), 076401. (www)

  @article{ , abstract = {We develop an ab initio framework that captures the impact of electron-electron and electron-hole interactions on phonon properties. This enables the inclusion of excitonic effects in the optical phonon dispersions and lifetimes of graphene, both near the center ( Γ ) and at the border ( K ) of the Brillouin zone, at phonon-momenta relevant for Raman scattering and for the onset of the intrinsic electrical resistivity. Near K , we find a phonon redshift of ∼ 150 cm − 1 and a 10 × enhancement of the group velocity, together with a 5 × increase in linewidths due to a 26 × increase of the electron-phonon matrix elements. These effects persist for doping 2 E F < ℏ ω ph and are quenched at higher dopings. Near Γ , the excitonic effects are minor because of the gauge field nature of the electron-phonon coupling at small phonon momentum.}, archive = {J_PRL}, author = {Alberto Guandalini and Francesco Macheda and Giovanni Caldarelli and Francesco Mauri}, doi = {10.1103/y1dn-m6pc}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076401}, shortjournal = {Phys. Rev. Lett.}, title = {Excitonic effects in phonons: Reshaping the graphene kohn anomalies and lifetimes}, volume = {135}, year = {2025}, }
• (2025). Quantum-size effect induced andreev bound states in ultrathin metallic islands proximitized by a superconductor. PRL, 135(7), 076201. (www)

  @article{ , abstract = {While Andreev bound states (ABSs) have been realized in engineered superconducting junctions, their direct observation in normal metal-superconductor heterostructures—enabled by quantum confinement—remains experimentally elusive. Here, we report the detection of ABSs in ultrathin metallic islands (Bi, Ag, and SnTe) grown on the s -wave superconductor NbN. Using high-resolution scanning tunneling microscopy and spectroscopy, we clearly reveal in-gap ABSs with energies symmetric about the Fermi level. While the energies of these states show no position dependence, their wave functions exhibit spatial oscillations, demonstrating a quantum size effect. Both the energy levels and spatial distribution of the ABSs can be reproduced by our effective model in which a metallic island is coupled to the superconducting substrate via the proximity effect. We demonstrate that the coupling strength plays a critical role in determining the ABS energies. Our work introduces a novel physical platform for implementing ABSs, which hold promise for significant device applications.}, archive = {J_PRL}, author = {Guanyong Wang and Li-Shuo Liu and Zhen Zhu and Yue Zheng and Bo Yang and Dandan Guan and Shiyong Wang and Yaoyi Li and Canhua Liu and Wei Chen and Hao Zheng and Jinfeng Jia}, doi = {10.1103/4mw4-4rfh}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-size effect induced andreev bound states in ultrathin metallic islands proximitized by a superconductor}, volume = {135}, year = {2025}, }
• (2025). Structural evidence for the spin collapse in high pressure solid oxygen. PRL, 135(7), 076101. (www)

  @article{ , abstract = {Single crystal x-ray diffraction measurements have been carried out on epsilon oxygen up to 30 GPa to examine the behavior of the constituent units. An isostructural phase transition is evidenced by lattice parameter and intracluster ( ) distance discontinuities and clear changes in the equation of state at on compression. This transition corresponds well to the predicted collapse of the molecular magnetic moment from spin-liquid, to a spinless, states of the structure. The collapse of the molecular magnetic moment has to date only been supported by spectroscopic data and, until now, has not been substantiated structurally.}, archive = {J_PRL}, author = {Federico Aiace Gorelli and Philip Dalladay-Simpson and Gaston Garbarino and Mohamed Mezouar and Julien Haines and Mario Santoro}, doi = {10.1103/jvd7-v9h9}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {076101}, shortjournal = {Phys. Rev. Lett.}, title = {Structural evidence for the spin collapse in high pressure solid oxygen}, volume = {135}, year = {2025}, }
• (2025). Elastic turbulence hides in the small scales of inertial polymeric turbulence. PRL, 135(7), 074001. (www)

  @article{ , abstract = {Gaining a fundamental understanding of turbulent flows of dilute polymer solutions has been a challenging and outstanding problem for a long time. In this Letter, we examine homogeneous, isotropic polymeric turbulence at large Reynolds and Deborah numbers through direct numerical simulations. While at the largest scales at which the flow inertial turbulence exists, we find that the flow is fundamentally altered from Newtonian turbulence below the Kolmogorov scale. We demonstrate that “elastic turbulence” exists at the smallest scales of polymeric turbulence by quantifying multiple statistical properties of the flow—energy spectrum and flux in Fourier space as well as the spatial statistics of the velocity field—the structure functions and kurtosis, and energy dissipation. Our results show the coexistence of two fundamentally distinct types of turbulence in polymeric fluids and point to the ubiquity of elastic turbulence, which was hitherto only known to exist for negligible inertia.}, archive = {J_PRL}, author = {Piyush Garg and Marco Edoardo Rosti}, doi = {10.1103/pbtf-rn7d}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {074001}, shortjournal = {Phys. Rev. Lett.}, title = {Elastic turbulence hides in the small scales of inertial polymeric turbulence}, volume = {135}, year = {2025}, }
• (2025). Strong coupling and dark modes in the motion of a pair of levitated nanoparticles. PRL, 135(7), 073602. (www)

  @article{ , abstract = {We experimentally investigate a system composed of two levitating nanospheres whose motions are indirectly coupled via coherent scattering in a single optical cavity mode. The nanospheres are loaded into a double longitudinal tweezer created with two lasers at different wavelengths, where chromatic aberration leads to the formation of two separate trapping sites. We achieve strong coupling between each pair of modes in the transverse plane of the tweezer, and we show the emergence of dark modes in the overall coupled motion. The observed features are ubiquitous in a variety of classical and quantum systems. As such, our experiment will allow us to explore the classical analog of typically quantum dynamics, and in further developments to investigate the transition to the quantum domain.}, archive = {J_PRL}, author = {A. Pontin and Q. Deplano and A. Ranfagni and F. Marino and F. Marin}, doi = {10.1103/t33b-f1b2}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {073602}, shortjournal = {Phys. Rev. Lett.}, title = {Strong coupling and dark modes in the motion of a pair of levitated nanoparticles}, volume = {135}, year = {2025}, }
• (2025). Group delay controlled by the decoherence of a single artificial atom. PRL, 135(7), 073601. (www)

  @article{ , abstract = {The ability to slow down light at the single-photon level has applications in quantum information processing and other quantum technologies. We demonstrate two methods, both using just a single artificial atom, enabling dynamic control over microwave light velocities in waveguide quantum electrodynamics (QED). Our methods are based on two distinct mechanisms harnessing the balance between radiative decay and nonradiative decoherence rates of a superconducting artificial atom in front of a mirror. In the first method, we tune the radiative decay of the atom using interference effects due to the mirror; in the second method, we pump the atom to effectively control its nonradiative decoherence. When the half of the radiative decay rate exceeds the nonradiative decoherence rate, we observe positive group delay; conversely, dominance of the nonradiative decoherence results in negative group delay. Our results advance signal-processing capabilities in waveguide QED.}, archive = {J_PRL}, author = {Y.-T. Cheng and K.-M. Hsieh and B.-Y. Wu and Z. Q. Niu and F. Aziz and Y.-H. Huang and P. Y. Wen and K.-T. Lin and Y.-H. Lin and J. C. Chen and A. F. Kockum and G.-D. Lin and Z.-R. Lin and Y. Lu and I.-C. Hoi}, doi = {10.1103/fkzb-fxv4}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {073601}, shortjournal = {Phys. Rev. Lett.}, title = {Group delay controlled by the decoherence of a single artificial atom}, volume = {135}, year = {2025}, }
• (2025). Collapse of a quantum vortex in an attractive two-dimensional bose gas. PRL, 135(7), 073401. (www)

  @article{ , abstract = {We experimentally and numerically study the collapse dynamics of a quantum vortex in a two-dimensional atomic superfluid following a fast interaction ramp from repulsion to attraction. We find the conditions and timescales for a superfluid vortex to radially converge into a quasistationary density profile, demonstrating the spontaneous formation of a vortex solitonlike structure in an atomic Bose gas. We record an emergent self-similar dynamics caused by an azimuthal modulational instability, which amplifies initial density perturbations and leads to the eventual splitting of a solitonic ring profile or direct fragmentation of a superfluid into disordered, but roughly circular arrays of Townes solitonlike wave packets. These dynamics are qualitatively reproduced by simulations based on the Gross-Pitaevskii equation. However, a discrepancy in the magnitude of amplified density fluctuations predicted by our mean-field analysis suggests the presence of effects beyond the mean-field approximation. Our study sets the stage for exploring out-of-equilibrium dynamics of vortex quantum matter quenched to attractive interactions and their universal characteristics.}, archive = {J_PRL}, author = {Sambit Banerjee and Kai Zhou and Shiva Kant Tiwari and Hikaru Tamura and Rongjie Li and Panayotis Kevrekidis and Simeon I. Mistakidis and Valentin Walther and Chen-Lung Hung}, doi = {10.1103/c6wx-zc9x}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {073401}, shortjournal = {Phys. Rev. Lett.}, title = {Collapse of a quantum vortex in an attractive two-dimensional bose gas}, volume = {135}, year = {2025}, }
• (2025). Lifetimes of the metastable 6d d5/22 and 6d d23/2 state of ra+. PRL, 135(7), 073001. (www)

  @article{ , abstract = {We report lifetime measurements of the metastable and states of . The measured lifetimes, and , are important for optical frequency standards and for benchmarking high-precision relativistic atomic theory. Independent of the reported measurements, the D state lifetimes were calculated using the coupled-cluster single double triple method, in which the coupled-cluster equations for both core and valence triple excitations were solved iteratively. The method was designed for precise prediction of atomic properties, especially for heavy elements, where relativistic and correlation corrections become large, making their treatment more challenging. This Letter presents the first tests of the method for transition properties. Our prediction agrees with experimental values within the uncertainties. The ability to accurately predict the atomic properties of heavy elements is important for many applications, from tests of fundamental symmetries to the development of optical clocks.}, archive = {J_PRL}, author = {Haoran Li and Huaxu Dan and Mingyu Fan and Spencer Kofford and Robert Kwapisz and Roy A. Ready and Akshay Sawhney and Merrell Brzeczek and Craig Holliman and Andrew M. Jayich and S. G. Porsev and M. S. Safronova}, doi = {10.1103/5754-4cbv}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {073001}, shortjournal = {Phys. Rev. Lett.}, title = {Lifetimes of the metastable 6d d5/22 and 6d d23/2 state of ra+}, volume = {135}, year = {2025}, }
• (2025). Universal effective charges in the sd and fp shells. PRL, 135(7), 072501. (www)

  @article{ , abstract = {The 247-keV state in , populated in the decay of , is reported here as a nanosecond isomer with a half-life of 26.0(22) ns. The state is interpreted as the member of the spin-coupled multiplet, which decays to the ground state. The new half-life corresponds to a pure transition with a strength of 1.93(16) W.u., providing the most precise, unambiguous value in the neutron-rich region to date for a nucleus with valence protons above . Notably, it is roughly 4 times larger than the value in . The results, as compared to semiempirical and ab initio shell-model calculations, indicate (1) a weak subshell gap relative to , (2) a large enhancement in Sc as compared to Ca due to proton excitations across , and (3) empirical effective proton and neutron charges and , respectively, that are in contrast to reports of and for -shell nuclei near . We demonstrate that these reports are erroneous and that, in fact, a universal set of effective charges can be used across the and shells.}, archive = {J_PRL}, author = {T. H. Ogunbeku and J. M. Allmond and T. J. Gray and W.-J. Ong and B. A. Brown and A. Gargano and R. Grzywacz and J. D. Holt and A. O. Macchiavelli and T. Miyagi and S. Neupane and B. C. Rasco and H. Schatz and B. M. Sherrill and O. B. Tarasov and H. Arora and A. D. Ayangeakaa and H. C. Berg and J. M. Berkman and D. L. Bleuel and K. Bosmpotinis and M. P. Carpenter and G. Cerizza and A. Chester and J. M. Christie and I. Cox and H. L. Crawford and B. P. Crider and J. Davis and A. A. Doetsch and J. G. Duarte and A. Estrade and A. Fijałkowska and C. Frantzis and T. Gaballah and E. C. Good and K. Haak and S. Hanai and J. T. Harke and A. C. Hartley and K. Hermansen and D. E. M. Hoff and D. Hoskins, III and J. Huffman and P. Van Isacker and R. Jain and M. Karny and T. T. King and N. Kitamura and K. Kolos and A. Laminack and S. N. Liddick and B. Longfellow and R. S. Lubna and S. Lyons and M. Madurga and M. J. Mogannam and G. Owens-Fryar and J. R. Palomino and M. M. Rajabali and A. L. Richard and I. J. Richardson and E. K. Ronning and G. E. Rose and T. J. Ruland and K. P. Rykaczewski and N. D. Scielzo and D. P. Scriven and D. Seweryniak and K. Siegl and M. Singh and A. Spyrou and M. Stepaniuk and A. E. Stuchbery and A. Sweet and V. Tripathi and A. Tsantiri and S. Uthayakumaar and W. B. Walters and S. Watters and Z. Xu and R. Yokoyama}, doi = {10.1103/75ry-71sj}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {072501}, shortjournal = {Phys. Rev. Lett.}, title = {Universal effective charges in the sd and fp shells}, volume = {135}, year = {2025}, }
• (2025). Rapidity asymmetry of jet-hadron correlation as a robust signal of diffusion wake induced by dijets in high-energy heavy-ion collisions. PRL, 135(7), 072302. (www)

  @article{ , abstract = {Diffusion wake accompanying a Mach cone is a unique feature of the medium response to projectiles traveling at a speed faster than the velocity of sound. This is also the case for jet-medium interaction inside the quark-gluon plasma in high-energy heavy-ion collisions. It leads to a depletion of soft hadrons in the opposite direction of the propagating jet and, recently, has been observed in -jet events of collisions at LHC. In dijet events, however, the diffusion wake of one jet usually overlaps with the medium-induced hadron enhancement of the other jet without a clear signal except a reduction of the hadron enhancement, unless there is a large rapidity gap between the two jets. We propose to use the rapidity asymmetry of jet-hadron correlations in dijets with a finite rapidity gap relative to that without, as a robust and background-free signal of the diffusion wake. The asymmetry emerges because the diffusion wake of one jet is shifted to a finite rapidity relative to the other jet. Consequently, a depletion of soft hadrons appears in the shifted rapidity region of the diffusion wake and an enhancement in the rapidity region of the other jet whose soft hadron enhancement is no longer or less reduced by the diffusion wake as in dijets without a rapidity gap. We predict the rapidity asymmetry using both theoretical and mixed-event background subtraction for different values of the rapidity gap within the CoLBT-hydro model. Future measurements of this rapidity asymmetry with high statistics data on dijets should provide more precise insights into the jet-induced diffusion wake and properties of the quark-gluon plasma.}, archive = {J_PRL}, author = {Zhong Yang and Xin-Nian Wang}, doi = {10.1103/vv7y-xbrc}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {072302}, shortjournal = {Phys. Rev. Lett.}, title = {Rapidity asymmetry of jet-hadron correlation as a robust signal of diffusion wake induced by dijets in high-energy heavy-ion collisions}, volume = {135}, year = {2025}, }
• (2025). Onset of constituent quark number scaling in heavy-ion collisions at RHIC. PRL, 135(7), 072301. (www)

  @article{ , abstract = {Partonic collectivity is one of the necessary signatures for the formation of quark-gluon plasma in high-energy nuclear collisions. Number of constituent quarks (NCQ) scaling has been observed for hadron elliptic flow in top energy nuclear collisions at the Relativistic Heavy Ion Collider and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this Letter, a systematic analysis of of , and in collisions at , 3.5, 3.9, and 4.5 GeV, with the STAR experiment at the Relativistic Heavy Ion Collider, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of for all hadrons studied provides evidence for the onset of dominant partonic interactions by .}, archive = {J_PRL}, author = {STAR Collaboration and B. E. Aboona and J. Adam and L. Adamczyk and I. Aggarwal and M. M. Aggarwal and Z. Ahammed and A. K. Alshammri and E. C. Aschenauer and S. Aslam and J. Atchison and V. Bairathi and X. Bao and K. Barish and S. Behera and R. Bellwied and P. Bhagat and A. Bhasin and S. Bhatta and S. R. Bhosale and J. Bielcik and J. Bielcikova and J. D. Brandenburg and C. Broodo and X. Z. Cai and H. Caines and M. Calderón de la Barca Sánchez and D. Cebra and J. Ceska and I. Chakaberia and P. Chaloupka and B. K. Chan and Z. Chang and A. Chatterjee and D. Chen and J. Chen and J. H. Chen and Q. Chen and Z. Chen and J. Cheng and Y. Cheng and W. Christie and X. Chu and S. Corey and H. J. Crawford and M. Csanád and G. Dale-Gau and A. Das and I. M. Deppner and A. Deshpande and A. Dhamija and A. Dimri and P. Dixit and X. Dong and J. L. Drachenberg and E. Duckworth and J. C. Dunlop and J. Engelage and G. Eppley and S. Esumi and O. Evdokimov and O. Eyser and R. Fatemi and S. Fazio and Y. Feng and E. Finch and Y. Fisyak and F. A. Flor and C. Fu and T. Fu and C. A. Gagliardi and T. Galatyuk and T. Gao and F. Geurts and N. Ghimire and A. Gibson and K. Gopal and X. Gou and D. Grosnick and A. Gu and A. Gupta and A. Hamed and R. J. Hamilton and X. Han and S. Harabasz and M. D. Harasty and J. W. Harris and H. Harrison-Smith and L. B. Havener and X. H. He and Y. He and N. Herrmann and L. Holub and C. Hu and Q. Hu and Y. Hu and H. Huang and H. Z. Huang and S. L. Huang and T. Huang and Y. Huang and T. J. Humanic and M. Isshiki and W. W. Jacobs and A. Jalotra and C. Jena and A. Jentsch and Y. Ji and J. Jia and C. Jin and N. Jindal and X. Ju and E. G. Judd and S. Kabana and D. Kalinkin and K. Kang and D. Kapukchyan and K. Kauder and D. Keane and M. Kesler and A. Khanal and Y. V. Khyzhniak and D. P. Kikoła and J. Kim and D. Kincses and I. Kisel and A. Kiselev and A. G. Knospe and J. Kołaś and B. Korodi and L. K. Kosarzewski and L. Kumar and M. C. Labonte and R. Lacey and J. M. Landgraf and C. Larson and J. Lauret and A. Lebedev and J. H. Lee and Y. H. Leung and C. Li and D. Li and H-S. Li and H. Li and W. Li and X. Li and Y. Li and Z. Li and X. Liang and Y. Liang and R. Licenik and T. Lin and Y. Lin and M. A. Lisa and C. Liu and G. Liu and H. Liu and L. Liu and Z. Liu and T. Ljubicic and O. Lomicky and R. S. Longacre and E. M. Loyd and T. Lu and J. Luo and X. F. Luo and L. Ma and R. Ma and Y. G. Ma and N. Magdy and D. Mallick and R. Manikandhan and S. Margetis and C. Markert and O. Matonoha and O. Mezhanska and K. Mi and S. Mioduszewski and B. Mohanty and B. Mondal and M. M. Mondal and I. Mooney and J. Mrazkova and M. I. Nagy and C. J. Naim and A. S. Nain and J. D. Nam and M. Nasim and H. Nasrulloh and D. Neff and J. M. Nelson and M. Nie and G. Nigmatkulov and T. Niida and T. Nonaka and G. Odyniec and A. Ogawa and S. Oh and K. Okubo and B. S. Page and S. Pal and A. Pandav and A. Panday and A. K. Pandey and T. Pani and A. Paul and S. Paul and D. Pawlowska and C. Perkins and J. Pluta and B. R. Pokhrel and I. D. Ponce Pinto and M. Posik and E. Pottebaum and S. Prodhan and T. L. Protzman and A. Prozorov and V. Prozorova and N. K. Pruthi and M. Przybycien and J. Putschke and Z. Qin and H. Qiu and C. Racz and S. K. Radhakrishnan and A. Rana and R. L. Ray and R. Reed and C. W. Robertson and M. Robotkova and M. A. Rosales Aguilar and D. Roy and P. Roy Chowdhury and L. Ruan and A. K. Sahoo and N. R. Sahoo and H. Sako and S. Salur and S. S. Sambyal and J. K. Sandhu and S. Sato and B. C. Schaefer and N. Schmitz and F-J. Seck and J. Seger and R. Seto and P. Seyboth and N. Shah and P. V. Shanmuganathan and T. Shao and M. Sharma and N. Sharma and R. Sharma and S. R. Sharma and A. I. Sheikh and D. Shen and D. Y. Shen and K. Shen and S. Shi and Y. Shi and F. Si and J. Singh and S. Singha and P. Sinha and M. J. Skoby and N. Smirnov and Y. Söhngen and Y. Song and T. D. S. Stanislaus and M. Stefaniak and Y. Su and M. Sumbera and X. Sun and Y. Sun and B. Surrow and M. Svoboda and Z. W. Sweger and A. C. Tamis and A. H. Tang and Z. Tang and T. Tarnowsky and J. H. Thomas and A. R. Timmins and D. Tlusty and T. Todoroki and D. Torres Valladares and S. Trentalange and P. Tribedy and S. K. Tripathy and T. Truhlar and B. A. Trzeciak and O. D. Tsai and C. Y. Tsang and Z. Tu and J. Tyler and T. Ullrich and D. G. Underwood and G. Van Buren and J. Vanek and I. Vassiliev and F. Videbæk and S. A. Voloshin and F. Wang and G. Wang and J. S. Wang and J. Wang and K. Wang and X. Wang and Y. Wang and Z. Wang and A. J. Watroba and J. C. Webb and P. C. Weidenkaff and G. D. Westfall and D. Wielanek and H. Wieman and G. Wilks and S. W. Wissink and R. Witt and C. P. Wong and J. Wu and X. Wu and B. Xi and Z. G. Xiao and G. Xie and W. Xie and H. Xu and N. Xu and Q. H. Xu and Y. Xu and Z. Xu and G. Yan and Z. Yan and C. Yang and Q. Yang and S. Yang and Y. Yang and Z. Ye and L. Yi and Y. Yu and H. Zbroszczyk and W. Zha and C. Zhang and D. Zhang and J. Zhang and S. Zhang and W. Zhang and X. Zhang and Y. Zhang and Z. Zhang and F. Zhao and J. Zhao and M. Zhao and S. Zhou and Y. Zhou and X. Zhu and M. Zurek and M. Zyzak}, doi = {10.1103/2qhx-cp79}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {072301}, shortjournal = {Phys. Rev. Lett.}, title = {Onset of constituent quark number scaling in heavy-ion collisions at RHIC}, volume = {135}, year = {2025}, }
• (2025). Low-energy constants of chiral perturbation theory from pion scalar form factors in nf=2+1-flavor lattice QCD with controlled errors. PRL, 135(7), 071904. (www)

  @article{ , abstract = {We determine the low-energy constants , and of SU(3) chiral perturbation theory from a lattice QCD calculation of the scalar form factors of the pion with fully controlled systematics. Lattice results are computed on a large set of gauge ensembles covering four lattice spacings , pion masses , and various large physical volumes. By determining the notorious quark-disconnected contributions with unprecedented precision and using a large range of source-sink separations , we are able for the first time to obtain the scalar radii from a -expansion parametrization of the form factors rather than a simple linear approximation at small momentum transfer. The low-energy constants are obtained from the physical extrapolation of the radii using next-to-leading-order SU(3) next-to-leading-order chiral perturbation theory to parametrize the quark mass dependence. Systematic uncertainties are estimated via model averages based on the Akaike information criterion. Our determination of is the first lattice determination to obtain a result not compatible with zero.}, archive = {J_PRL}, author = {Georg von Hippel and Konstantin Ottnad}, doi = {10.1103/f4x5-frx1}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071904}, shortjournal = {Phys. Rev. Lett.}, title = {Low-energy constants of chiral perturbation theory from pion scalar form factors in nf=2+1-flavor lattice QCD with controlled errors}, volume = {135}, year = {2025}, }
• (2025). Evidence for similar collectivity of high transverse-momentum particles in p-pb and pb-pb collisions. PRL, 135(7), 071903. (www)

  @article{ , abstract = {Charged hadron elliptic anisotropies ( ) are presented over a wide transverse momentum ( ) range for proton-lead ( ) and lead-lead (PbPb) collisions at nucleon-nucleon center-of-mass energies of 8.16 and 5.02 TeV, respectively. The data were recorded by the CMS experiment and correspond to integrated luminosities of 186 and for the and PbPb systems, respectively. A four-particle cumulant analysis is performed using subevents separated in pseudorapidity to effectively suppress noncollective effects. At high ( ), significant positive values that are similar between and PbPb collisions at comparable charged particle multiplicities are observed. This observation suggests a common origin for the multiparticle collectivity for high- particles in the two systems.}, archive = {J_PRL}, author = {CMS Collaboration and V. Chekhovsky and A. Hayrapetyan and V. Makarenko and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and T. Van Laer and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and Y. Hong and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and A. Khalilzadeh and F. A. Khan and K. Lee and A. Malara and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and J. Knolle and L. Lambrecht and D. Marckx and K. Mota Amarilo and K. Skovpen and N. Van Den Bossche and J. van der Linden and L. Wezenbeek and S. Bein and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and S. Turkcapar and G. A. Alves and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and E. J. Tonelli Manganote and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and T. Laux Kuhn and M. Macedo and J. Martins and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and D. Laroze and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and H. Wang and K. Yi and J. Zhang and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and J. Jaramillo and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and H. Abdalla and Y. Assran and B. El-mahdy and M. Abdullah Al-Mashad and M. A. Mahmoud and K. Ehataht and M. Kadastik and T. Lange and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and H. Kirschenmann and K. Osterberg and M. Voutilainen and S. Bharthuar and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Myllymäki and M. m. Rantanen and H. Siikonen and J. Tuominiemi and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and A. Cappati and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Nguyen and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and D. Chokheli and I. Lomidze and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and D. Noll and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and A. Stein and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and A. Cardini and C. Cheng and F. Colombina and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and Y. Otarid and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and A. Saggio and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and S. Zakharov and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and T. Chwalek and A. Dierlamm and A. Droll and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and O. Lavoryk and J. M. Lawhorn and M. Link and A. Lintuluoto and S. Maier and S. Mitra and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and B. Topko and N. Trevisani and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and G. Melachroinos and Z. Painesis and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and P. Major and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Ahmed and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Baradia and S. Barman and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and T. Mishra and B. Parida and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and K. Naskar and A. Nayak and S. Nayak and K. Pal and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and C. Tuve and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and D. Bisello and P. Bortignon and G. Bortolato and A. Bragagnolo and A. C. M. Bulla and P. Checchia and T. Dorigo and F. Gasparini and U. Gasparini and S. Giorgetti and A. Gozzelino and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and M. Magherini and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and V. K. Muraleedharan Nair Bindhu and M. Musich and S. Nandan and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and C. Baldenegro Barrera and P. Barria and C. Basile and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and R. Gargiulo and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and B. Kim and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and J. Yoo and J. Goh and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and H. Kwon and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and K. Hwang and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and C. A. Mondragon Herrera and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and F. E. Neri Huerta and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and L. Grzanka and M. Malawski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and M. Stojanovic and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and C. Martin Perez and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and S. Sánchez Navas and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and E. Palencia Cortezon and J. Prado Pico and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Bhowmik and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and A. A. Bin Anuar and A. Bocci and L. Borgonovi and C. Botta and E. Brondolin and C. E. Brown and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and G. Karathanasis and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and Y. Maghrbi and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and Y. Komurcu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and E. Uslan and I. S. Zorbakir and G. Sokmen and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and G. G. Dincer and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and V. J. Smith and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and O. Buchmuller and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and V. Hegde and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and C. Cosby and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and L. Gouskos and M. Hadley and U. Heintz and K. W. Ho and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and J. Luo and S. Mondal and T. Russell and S. Sagir and X. Shen and F. Simpson and M. Stamenkovic and N. Venkatasubramanian and S. Abbott and B. Barton and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and S. Yoo and F. Zhang and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and D. Primosch and M. Quinnan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and M. M. Hussain and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and X. Yan and D. Zhang and A. Bornheim and O. Cerri and A. Latorre and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and N. Manganelli and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and X. Chen and D. J. Cranshaw and J. Dickinson and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and I. Dutta and V. D. Elvira and Y. Feng and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and C. Madrid and K. Maeshima and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and A. H. Merrit and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and T. Roy and S. Rudrabhatla and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Wang and L. Zhang and J. Bendavid and S. Bright-Thonney and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and A. Rohilla and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and J. Li and M. Lu and R. Mccarthy and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and E. Tsai and D. Wood and J. Bueghly and S. Dittmer and K. A. Hahn and D. Li and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and D. Stickland and C. Tully and L. H. Vage and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and V. Scheurer and J. F. Schulte and J. Thieman and A. K. Virdi and F. Wang and A. Wildridge and W. Xie and Y. Yao and J. Dolen and N. Parashar and A. Pathak and D. Acosta and A. Agrawal and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and I. Krommydas and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and J. Reichert and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and A. Safonov and N. Akchurin and J. Damgov and N. Gogate and A. Hussain and Y. Kazhykarim and K. Lamichhane and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and D. Rathjens and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Mantilla and C. Neu and C. Ramón Álvarez and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and D. Budkouski and I. Golutvin and I. Gorbunov and V. Karjavine and O. Kodolova and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and A. Nikitenko and V. Palichik and V. Perelygin and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and V. Smirnov and O. Teryaev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and P. Levchenko and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and Yu. Andreev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and I. Tlisova and A. Toropin and T. Aushev and K. Ivanov and V. Gavrilov and N. Lychkovskaya and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and A. Demiyanov and A. Ershov and A. Gribushin and L. Khein and V. Korotkikh and S. Obraztsov and S. Petrushanko and V. Savrin and A. Snigirev and I. Vardanyan and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and Y. Skovpen and V. Kachanov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin}, doi = {10.1103/t5kp-vsv7}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071903}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for similar collectivity of high transverse-momentum particles in p-pb and pb-pb collisions}, volume = {135}, year = {2025}, }
• (2025). Flavor nonsinglet splitting functions at four loops in QCD: Fermionic contributions. PRL, 135(7), 071902. (www)

  @article{ , abstract = {We have determined the fourth-order n f contributions to the two splitting functions governing the evolution of all flavor differences of quark distributions of hadrons in perturbative quantum chromodynamics with n f light flavors. The analytic forms of these functions are presented in both Mellin N space and momentum-fraction x space for a general gauge group. In the small- x limit double logarithms occur, but the small- x rise of both splitting functions is confined to extremely small- x values, x ≲ 10 − 6 . The large- x limit includes the n f -part of the four-loop quark virtual anomalous dimension. Using this result we obtain also the n f contributions to the corresponding gluonic quantity and the complete threshold-enhanced logarithms from soft-gluon emission for a large class of inclusive observables, including Higgs boson production in gluon-gluon fusion.}, archive = {J_PRL}, author = {B. A. Kniehl and S. Moch and V. N. Velizhanin and A. Vogt}, doi = {10.1103/hkg5-88hr}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071902}, shortjournal = {Phys. Rev. Lett.}, title = {Flavor nonsinglet splitting functions at four loops in QCD: Fermionic contributions}, volume = {135}, year = {2025}, }
• (2025). Observation of three resonant structures in the cross section of e+e−→π+π−hc. PRL, 135(7), 071901. (www)

  @article{ , abstract = {Using collision data collected with the BESIII detector operating at the Beijing electron positron collider, the cross section of is measured at 59 points with center-of-mass energy ranging from 4.009 to 4.950 GeV with a total integrated luminosity of . The cross section between 4.3 and 4.45 GeV exhibits a plateaulike shape and drops sharply around 4.5 GeV, which cannot be described by two resonances only. Three coherent Breit-Wigner functions are used to parametrize the -dependent cross section line shape. The masses and widths are determined to be , and , and . The first uncertainties are statistical and the second are systematic. The inclusion of the relatively narrower third component proves crucial for reproducing the drop at around 4.5 GeV. The statistical significance of the three-resonance assumption over the two-resonance assumption is greater than .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and X. Y. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. K. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. Cottee-Meldrum and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and L. Feng and Q. X. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. Gao and Y. N. Gao and Y. Y. Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and J. D. Gong and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and Z. M. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Y. P. Li and Z. J. Li and Z. Y. Li and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. B. Liao and M. H. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. K. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and Z. Y. Lv and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Q. A. Malik and H. X. Mao and Y. J. Mao and Z. P. Mao and S. Marcello and A. Marshall and F. M. Melendi and Y. H. Meng and Z. X. Meng and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and C. Normand and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and X. J. Peng and Y. Y. Peng and K. Peters and K. Petridis and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and J. Rademacker and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and F. Rosini and Ch. Rosner and M. Q. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and J. J. Tang and L. F. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and Cong Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. J. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Q. Wang and Z. Y. Wang and D. H. Wei and H. R. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and T. D. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. H. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. H. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Z. J. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and L. Q. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and X. Q. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Y. P. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and C. Zhong and H. Zhou and J. Q. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. X. Zhou and Y. Z. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/ljnf-4jfr}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of three resonant structures in the cross section of e+e−→π+π−hc}, volume = {135}, year = {2025}, }
• (2025). Fractional hall physics from large n interacting fermions. PRL, 135(7), 071601. (www)

  @article{ , abstract = {We solve models of species of fermions in the lowest Landau level with -invariant interactions in the limit. We find saddles of the second quantized path integral at fixed chemical potential corresponding to fractional Hall states with filling , where the integers and depend on the chemical potential and interactions. On a long torus there are such states related by translation symmetry, and -invariant excitations of fractional charge. Remarkably, these saddles and their filling persist as extrema of the second-quantized action at . Our construction gives a first-principles derivation of fractional Hall states from strongly interacting fermions.}, archive = {J_PRL}, author = {Kristan Jensen and Amir Raz}, doi = {10.1103/bn5v-p282}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071601}, shortjournal = {Phys. Rev. Lett.}, title = {Fractional hall physics from large n interacting fermions}, volume = {135}, year = {2025}, }
• (2025). Rapid parameter estimation for pulsar-timing-array datasets with variational inference and normalizing flows. PRL, 135(7), 071401. (www)

  @article{ , abstract = {In the gravitational-wave analysis of pulsar-timing-array datasets, parameter estimation is usually performed using Markov chain Monte Carlo methods to explore posterior probability densities. We introduce an alternative procedure that instead relies on stochastic gradient-descent Bayesian variational inference, whereby we obtain the weights of a neural-network-based approximation of the posterior by minimizing the Kullback–Leibler divergence of the approximation from the exact posterior. This technique is distinct from simulation-based inference with normalizing flows since we train the network for a single dataset, rather than the population of all possible datasets, and we require the computation of the data likelihood and its gradient. Unlike Markov chain methods, our technique can trivially exploit highly parallel computing platforms. This makes it extremely fast on modern graphical processing units, on which it can analyze the NANOGrav 15-yr dataset in a few tens of minutes, depending on the probabilistic model, compared to hours or days with the analysis codes used so far. We expect that this speed will unlock new astrophysical and cosmological explorations of pulsar-timing-array datasets with statistical models that are currently too computationally expensive. Furthermore, this kind of variational inference is viable in other contexts of gravitational-wave data analysis, as long as differentiable and parallelizable likelihoods are available.}, archive = {J_PRL}, author = {Michele Vallisneri and Marco Crisostomi and Aaron D. Johnson and Patrick M. Meyers}, doi = {10.1103/p3f7-rbmv}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071401}, shortjournal = {Phys. Rev. Lett.}, title = {Rapid parameter estimation for pulsar-timing-array datasets with variational inference and normalizing flows}, volume = {135}, year = {2025}, }
• (2025). Energy transfer by feebly interacting particles in supernovae: The trapping regime. PRL, 135(7), 071005. (www)

  @article{ , abstract = {Feebly interacting particles, such as sterile neutrinos, dark photons, and axions, can be abundantly produced in the proto-neutron star (PNS) formed in core-collapse supernovae (CCSNe). These particles can decay into photons or charged leptons, depositing energy outside the PNS. Strong bounds on new particles can thus be derived from the observed luminosity of CCSNe, with even tighter bounds obtained from low-energy SNe observations. For the first time we highlight that, at sufficiently large couplings, particle production outside the PNS must also be considered. Using the prototypical case of axions coupling to two photons, we show that at large couplings the energy transfer from PNS to its surroundings is diffusive rather than ballistic, substantially reducing the deposited energy. Our findings have implications for the parameter space of particles probed in beam dump experiments and for dark matter models involving a sub-GeV mediator.}, archive = {J_PRL}, author = {Damiano F. G. Fiorillo and Tetyana Pitik and Edoardo Vitagliano}, doi = {10.1103/cz94-dqxt}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071005}, shortjournal = {Phys. Rev. Lett.}, title = {Energy transfer by feebly interacting particles in supernovae: The trapping regime}, volume = {135}, year = {2025}, }
• (2025). Novel approach to cosmological nonlinearities as an effective fluid. PRL, 135(7), 071004. (www)

  @article{ , abstract = {We propose a two parameters extension of the flat model to capture the impact of matter inhomogeneities on our cosmological inference. Non virialized but nonlinearly evolving overdense and underdense regions, whose abundance is quantified using the Press-Schechter formalism, are collectively described by two effective perfect fluids , with nonvanishing equation of state parameters . These fluids are coupled to the pressureless dust, akin to an interacting DM-DE scenario. The resulting phenomenology is very rich, and could potentially address a number of inconsistencies of the standard model, including a simultaneous resolution of the Hubble and tensions. To assess the viability of the model, we set initial conditions compatible to the Planck 2018 best fit cosmology and fit its additional parameters using SN Ia observations from DESY5, BAO distances from DESI DR2 and a sample of uncorrelated measurements. Our findings show that backreaction effects from the cosmic web could restore the concordance between early and late Universe cosmological probes.}, archive = {J_PRL}, author = {Leonardo Giani and Rodrigo von Marttens and Ryan Camilleri}, doi = {10.1103/zr92-m7py}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071004}, shortjournal = {Phys. Rev. Lett.}, title = {Novel approach to cosmological nonlinearities as an effective fluid}, volume = {135}, year = {2025}, }
• (2025). Model-independent test of prerecombination new physics: Measuring the sound horizon with gravitational wave standard sirens and the baryon acoustic oscillation angular scale. PRL, 135(7), 071003. (www)

  @article{ , abstract = {In a broad class of cosmological models where spacetime is described by a pseudo-Riemannian manifold, photons propagate along null geodesics, and their number is conserved, upcoming gravitational wave (GW) observations can be combined with measurements of the baryon acoustic oscillation (BAO) angular scale to provide model-independent estimates of the sound horizon at the baryon drag epoch. By focusing on the accuracy expected from forthcoming surveys such as the Laser Interferometer Space Antenna GW standard sirens and dark energy spectroscopic instrument (DESI) or Euclid angular BAO measurements, we forecast a relative precision of σ r d / r d ∼ 1.5 % within the redshift range z ≲ 1 . This approach will offer a unique model-independent measure of a fundamental scale characterizing the early universe, which is competitive with model-dependent values inferred within specific theoretical frameworks. These measurements can serve as a consistency test for Λ CDM , potentially clarifying the nature of the Hubble tension and confirming or ruling out new physics prior to recombination with a statistical significance of ∼ 4 σ .}, archive = {J_PRL}, author = {William Giarè and Jonathan Betts and Carsten van de Bruck and Eleonora Di Valentino}, doi = {10.1103/k6mg-g23d}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071003}, shortjournal = {Phys. Rev. Lett.}, title = {Model-independent test of prerecombination new physics: Measuring the sound horizon with gravitational wave standard sirens and the baryon acoustic oscillation angular scale}, volume = {135}, year = {2025}, }
• (2025). Probing benchmark models of hidden-sector dark matter with DAMIC-M. PRL, 135(7), 071002. (www)

  @article{ , abstract = {We report on a search for sub-GeV dark matter (DM) particles interacting with electrons using the DAMIC-M prototype detector at the Modane Underground Laboratory. The data feature a significantly lower detector single rate (factor 50) compared to our previous search, while also accumulating a 10 times larger exposure of . DM interactions in the skipper charge-coupled devices (CCDs) are searched for as groups of two or three adjacent pixels with a total charge between 2 and . We find 144 candidates of and 1 candidate of , where 141.5 and 0.071, respectively, are expected from background. With no evidence of a DM signal, we place stringent constraints on DM particles with masses between 1 and interacting with electrons through an ultralight or heavy mediator. For large ranges of DM masses below , we exclude theoretically motivated benchmark scenarios where hidden-sector particles are produced as a major component of DM in the Universe through the freeze-in or freeze-out mechanisms.}, archive = {J_PRL}, author = {DAMIC-M Collaboration and K. Aggarwal and I. Arnquist and N. Avalos and X. Bertou and N. Castelló-Mor and A. E. Chavarria and J. Cuevas-Zepeda and A. Dastgheibi-Fard and C. De Dominicis and O. Deligny and J. Duarte-Campderros and E. Estrada and R. Gaïor and E.-L. Gkougkousis and T. Hossbach and L. Iddir and B. J. Kavanagh and B. Kilminster and A. Lantero-Barreda and I. Lawson and A. Letessier-Selvon and H. Lin and P. Loaiza and A. Lopez-Virto and R. Lou and K. J. McGuire and S. Munagavalasa and J. Noonan and D. Norcini and S. Paul and P. Privitera and P. Robmann and B. Roach and M. Settimo and R. Smida and M. Traina and R. Vilar and R. Yajur and D. Venegas-Vargas and C. Zhu and Y. Zhu}, doi = {10.1103/2tcc-bqck}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071002}, shortjournal = {Phys. Rev. Lett.}, title = {Probing benchmark models of hidden-sector dark matter with DAMIC-M}, volume = {135}, year = {2025}, }
• (2025). Constraints on primordial magnetic fields from the lyman-α forest. PRL, 135(7), 071001. (www)

  @article{ , abstract = {We present the first constraints on primordial magnetic fields from the Lyman- forest using full cosmological hydrodynamic simulations. At the scales and redshifts probed by the data, the flux power spectrum is extremely sensitive to the extra power induced by primordial magnetic fields in the linear matter power spectrum, at a scale that we parametrize with . We rely on a set of more than a quarter million flux models obtained by varying thermal and reionization histories and cosmological parameters. We find a hint of extra power that is well fitted by the primordial magnetic field model with , corresponding to . However, when applying very conservative assumptions on the modeling of the noise, we obtain a C.L. lower limit , which translates into the tightest bounds on the strength of primordial intergalactic magnetic fields: (for a fixed, nearly scale-invariant ).}, archive = {J_PRL}, author = {Mak Pavičević and Vid Iršič and Matteo Viel and James S. Bolton and Martin G. Haehnelt and Sergio Martin-Alvarez and Ewald Puchwein and Pranjal Ralegankar}, doi = {10.1103/77rd-vkpz}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {071001}, shortjournal = {Phys. Rev. Lett.}, title = {Constraints on primordial magnetic fields from the lyman-α forest}, volume = {135}, year = {2025}, }
• (2025). Proposed five-electron charge quadrupole qubit. PRL, 135(7), 070803. (www)

  @article{ , abstract = {A charge qubit couples to environmental electric field fluctuations through its dipole moment, resulting in fast decoherence. We propose the p -orbital ( p O ) qubit, formed by the single-electron, p -like valence states of a five-electron Si quantum dot, which couples to charge noise through the quadrupole moment. We demonstrate that the p O qubit offers distinct advantages in quality factor, gate speed, readout, and size. We use a phenomenological, dipole two-level-fluctuator charge noise model to estimate a T 2 * ∼ 80 ns . In conjunction with Rabi frequencies of order 10 GHz, an order of magnitude improvement in qubit quality factor is expected relative to state-of-the-art semiconductor spin qubits. The p O qubit features all-electrical control via modulating the dot’s eccentricity. We also show how to perform two-qubit gates via the 1 / r 5 quadrupole-quadrupole interaction. We find a universal gate set using gradient ascent-based control pulse optimization, subject to 10 GHz maximum allowable bandwidth and 1 ns pulse times.}, archive = {J_PRL}, author = {John H. Caporaletti and J. P. Kestner}, doi = {10.1103/l1x2-n2w9}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070803}, shortjournal = {Phys. Rev. Lett.}, title = {Proposed five-electron charge quadrupole qubit}, volume = {135}, year = {2025}, }
• (2025). Unwanted couplings can induce amplification in quantum memories despite negligible apparent noise. PRL, 135(7), 070802. (www)

  @article{ , abstract = {Theoretical quantum memory design often involves selectively focusing on certain energy levels to mimic an ideal Λ configuration, a common approach that may unintentionally overlook the impact of neighboring levels or undesired couplings. While this simplification may be justified in certain protocols or platforms, it can significantly distort the achievable memory performance. Through numerical semiclassical analysis, we show that the presence of unwanted energy levels and undesired couplings in an absorptive memory based on a nitrogen-vacancy center can significantly amplify the signal, resulting in memory efficiencies exceeding unity, a clear indication of unwanted noise at the quantum level. Strikingly, this effect occurs even when the apparent noise, i.e., output in the absence of an input field, is negligible. We then generalize our results using semianalytical estimations to analyze this amplification, and propose a strategy to reduce its effect. Our findings extend to memory platforms beyond nitrogen-vacancy centers; as an example, we also analyze a cavity-based rubidium memory that experiences the same issue.}, archive = {J_PRL}, author = {Faezeh Kimiaee Asadi and Janish Kumar and Jiawei Ji and Khabat Heshami and Christoph Simon}, doi = {10.1103/pz34-47pw}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070802}, shortjournal = {Phys. Rev. Lett.}, title = {Unwanted couplings can induce amplification in quantum memories despite negligible apparent noise}, volume = {135}, year = {2025}, }
• (2025). Full characterization of genuine 17-qubit entanglement on the superconducting processor. PRL, 135(7), 070801. (www)

  @article{ , abstract = {We present a least square state estimator regularized by state purity to accomplish the task of quantum state tomography and entanglement verification, and report an experimental validation on a superconducting processor. First, a scalable full-state tomography is achieved with state fidelity 0.8217(1) for the 9-qubit state and 0.6817(1) for the 17-qubit Greenberger-Horne-Zeilinger state, with the latter reaching 0.7587(1) under a pure-state assumption. Then, the presence of genuine multiqubit entanglement in the majority of generated states is conclusively certified by violating the corresponding entanglement witness. Finally, it is demonstrated that our method can achieve superior tomography accuracy with limited measurement settings and that mitigating error is essential for leveraging noisy quantum systems in quantum processing tasks. Our results pave the way for more accurate full characterization of larger-scale many-body quantum systems.}, archive = {J_PRL}, author = {Chang-Kang Hu and Yong Wang and YuXuan Zhou and ChiLong Liu and GuiXu Xie and RuiYang Zhou and HaoLan Yuan and Lijun Liu and Li Li and Song Liu and Dian Tan and Shuming Cheng and Dapeng Yu}, doi = {10.1103/qy9y-7ywp}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070801}, shortjournal = {Phys. Rev. Lett.}, title = {Full characterization of genuine 17-qubit entanglement on the superconducting processor}, volume = {135}, year = {2025}, }
• (2025). Color code with a logical control-S gate using transversal t rotations. PRL, 135(7), 070602. (www)

  @article{ , abstract = {The color code has been invaluable for the development of the theory of fault-tolerant logic gates using transversal rotations. Three-dimensional examples of the color code have shown us how its structure, specifically the intersection of the supports of logical operators, can give rise to non-Clifford T and C C Z gates. Here we present a color code with a logical control- S gate that is accomplished with transversal T and T † rotations on its physical qubits.}, archive = {J_PRL}, author = {Benjamin J. Brown}, doi = {10.1103/lwxd-fdlb}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070602}, shortjournal = {Phys. Rev. Lett.}, title = {Color code with a logical control-S gate using transversal t rotations}, volume = {135}, year = {2025}, }
• (2025). Randomized benchmarking with non-markovian noise and realistic finite-time gates. PRL, 135(7), 070601. (www)

  @article{ , abstract = {We analyze the impact of non-Markovian classical noise on single-qubit randomized benchmarking experiments, in a manner that explicitly models the realization of each gate via realistic finite-duration pulses. Our new framework exploits the random nature of each gate sequence to derive expressions for the full survival probability decay curve which are nonperturbative in the noise strength. In the presence of non-Markovian noise, our approach shows that the decay curve can exhibit a strong dependence on the gate implementation method, with regimes of both exponential and power law decays. We discuss how these effects can complicate the interpretation of a randomized benchmarking experiment, but also how to leverage them to probe non-Markovianity.}, archive = {J_PRL}, author = {Antoine Brillant and Peter Groszkowski and Alireza Seif and Jens Koch and Aashish A. Clerk}, doi = {10.1103/tmfd-qc5q}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070601}, shortjournal = {Phys. Rev. Lett.}, title = {Randomized benchmarking with non-markovian noise and realistic finite-time gates}, volume = {135}, year = {2025}, }
• (2025). Detecting many-body scars from fisher zeros. PRL, 135(7), 070402. (www)

  @article{ , abstract = {The far-from-equilibrium dynamics of certain interacting quantum systems still defy precise understanding. One example is the so-called quantum many-body scars (QMBSs), where a set of energy eigenstates evade thermalization to give rise to long-lived oscillations. Despite the success of viewing scars from the perspectives of symmetry, commutant algebra, and quasiparticles, it remains a challenge to elucidate the mechanism underlying all QMBS and to distinguish them from other forms of ergodicity breaking. In this work, we introduce an alternative route to detect and diagnose QMBS based on Fisher zeros, i.e., the patterns of zeros of the analytically continued partition function on the complex (inverse temperature) plane. For systems with scars, a continuous line of Fisher zeros will appear off the imaginary axis and extend upward, separating the plane into regions with distinctive thermalization behaviors. This conjecture is motivated from interpreting the complex as the return amplitude of the thermofield double state, and it is validated by analyzing two models with QMBS, the model and the Ising chain in external fields. These models also illustrate the key difference between QMBS and strong ergodicity breaking including their distinctive renormalization group flows on the complex plane. This “statistical mechanics” approach places QMBS within the same framework of thermal and dynamical phase transitions. It has the advantage of spotting scars without exhaustively examining each individual quantum state.}, archive = {J_PRL}, author = {Yuchen Meng and Songtai Lv and Yang Liu and Zefan Tan and Erhai Zhao and Haiyuan Zou}, doi = {10.1103/glc5-hv2m}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070402}, shortjournal = {Phys. Rev. Lett.}, title = {Detecting many-body scars from fisher zeros}, volume = {135}, year = {2025}, }
• (2025). Exact nonequilibrium steady state of XXZ circuits boundary driven with arbitrary resets or fields. PRL, 135(7), 070401. (www)

  @article{ , abstract = {We propose a spatially inhomogeneous matrix product Ansatz for an exact many-body density operator of a boundary-driven quantum circuit. The Ansatz has formally infinite bond dimension and is fundamentally different from previous constructions. The circuit is driven by a pair of reset quantum channels applied on the boundary qubits, which polarize the qubits to arbitrary pure target states. Moreover, one of the reset channels can be replaced by an arbitrary local unitary gate, thus representing a hybrid case with coherent and incoherent driving. Analyzing the Ansatz , we obtain a family of relatively robust separable nonequilibrium steady states, which can be viewed as a circuit extension of spin-helix states and are particularly suited for experimental investigations.}, archive = {J_PRL}, author = {Vladislav Popkov and Tomaž Prosen}, doi = {10.1103/31p7-lcgh}, journal = {Physical Review Letters}, month = {8}, number = {7}, pages = {070401}, shortjournal = {Phys. Rev. Lett.}, title = {Exact nonequilibrium steady state of XXZ circuits boundary driven with arbitrary resets or fields}, volume = {135}, year = {2025}, }
• (2025). Joint distribution of nuclear and cytoplasmic mRNA levels in stochastic models of gene expression: Analytical results and parameter inference. PRL, 135(6), 068401. (www)

  @article{ , abstract = {Common stochastic models of gene expression predict the gene-specific distribution of total mRNA per cell but lack subcellular resolution. Here, for a broad class of transcription initiation models, we derive an exact steady-state solution for the joint distribution of nuclear and cytoplasmic mRNA, and demonstrate that fitting this solution to spatially resolved mRNA data enhances parameter identifiability. By accounting for extrinsic noise, we use the model to precisely quantify bursty expression across thousands of human genes and link it to their biological functions.}, archive = {J_PRL}, author = {Yiling Wang and Juraj Szavits-Nossan and Zhixing Cao and Ramon Grima}, doi = {10.1103/q5sd-tpms}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {068401}, shortjournal = {Phys. Rev. Lett.}, title = {Joint distribution of nuclear and cytoplasmic mRNA levels in stochastic models of gene expression: Analytical results and parameter inference}, volume = {135}, year = {2025}, }
• (2025). Inferring the isotropic-nematic phase transition with generative machine learning. PRL, 135(6), 068102. (www)

  @article{ , abstract = {Generative machine learning models are capable of learning the phase behavior in condensed matter systems such as the Ising model. We utilize a score-based modeling procedure called thermodynamic maps to describe the isotropic-nematic phase transition in a melt of Gay-Berne ellipsoids. When trained on samples from a single temperature on either side of the phase transition, this generative machine learning approach infers effectively the nematic order parameter at intermediate temperatures. These results demonstrate score-based models’ ability to learn the physics of a nontrivial liquid crystal phase transition.}, archive = {J_PRL}, author = {Eric R. Beyerle and Pratyush Tiwary}, doi = {10.1103/1wdj-ym3s}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {068102}, shortjournal = {Phys. Rev. Lett.}, title = {Inferring the isotropic-nematic phase transition with generative machine learning}, volume = {135}, year = {2025}, }
• (2025). Nematic order from phase synchronization of shape oscillations. PRL, 135(6), 068101. (www)

  @article{ , abstract = {We show that a suspension of noninteracting deformable particles subjected to an oscillatory shear flow leads to development of nematic order that arises from the phenomenon of phase synchronization. The synchronized state corresponds to a unique, stable limit cycle confined in the toroidal state space. The limit cycle exists since, unlike rigid particles, deformable particles can modulate aspect ratio, adjust their tumbling rate, and thus achieve phase synchronization. These synchronized regions emerge as Arnold tongues in the parameter space of the driving amplitude and frequency. Considering the rheological implications of ordering dynamics in soft and active matter, our results motivate oscillatory shear flow experiments with deformable particles.}, archive = {J_PRL}, author = {Ioannis Hadjifrangiskou and Sumesh P. Thampi and Rahil N. Valani}, doi = {10.1103/j19g-c2nh}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {068101}, shortjournal = {Phys. Rev. Lett.}, title = {Nematic order from phase synchronization of shape oscillations}, volume = {135}, year = {2025}, }
• (2025). Real 2D galvanostatic model: Encoding physicochemical heterogeneity into a full battery. PRL, 135(6), 068001. (www)

  @article{ , abstract = {The propagation of physicochemical heterogeneity from particles to electrodes under galvanostatic cycling conditions largely determines battery performance but is often computationally unreachable. We formulate a Real 2D (R2D) full-battery model via an electrode-adaptive mathematical framework that addresses the electrochemically correlated nonlinear current-potential responses of the electrodes. This allows us to quantify the impact of multiphysics coupling on cycling performance in emerging solid-state batteries. R2D advances the modeling efficiency and can be generally applied to heterogeneous battery systems, providing a new pathway for accurate full battery simulations.}, archive = {J_PRL}, author = {Zhe-Tao Sun and Shiwei Chen and Teng Zhao and Yunlong Guo and Zhenli Xu and Shenggao Zhou and Shou-Hang Bo}, doi = {10.1103/4783-dkt8}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {068001}, shortjournal = {Phys. Rev. Lett.}, title = {Real 2D galvanostatic model: Encoding physicochemical heterogeneity into a full battery}, volume = {135}, year = {2025}, }
• (2025). Mach reflection and expansion of two-dimensional dispersive shock waves. PRL, 135(6), 067201. (www)

  @article{ , abstract = {The oblique collisions and dynamical interference patterns of two-dimensional dispersive shock waves are studied numerically and analytically via the temporal dynamics induced by wedge-shaped initial conditions for the Kadomtsev-Petviashvili II equation. Various asymptotic wave patterns are identified, classified, and characterized in terms of the incidence angle and the amplitude of the initial step, which can give rise to either subcritical or supercritical configurations, including the generalization to dispersive shock waves of the Mach reflection and expansion of viscous shocks and line solitons. An eightfold amplification of the amplitude of an obliquely incident flow upon a wall at the critical angle is demonstrated. Applications of the results include bore interactions in geophysical fluid dynamics.}, archive = {J_PRL}, author = {Gino Biondini and Alexander Bivolcic and Mark A. Hoefer}, doi = {10.1103/cdvf-xnfw}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {067201}, shortjournal = {Phys. Rev. Lett.}, title = {Mach reflection and expansion of two-dimensional dispersive shock waves}, volume = {135}, year = {2025}, }
• (2025). Heat diffusion invariant. PRL, 135(6), 067103. (www)

  @article{ , abstract = {Topological invariants have been utilized profoundly to classify the geometric features of electronic, photonic, and phononic structures. However, no invariant has ever been conceptualized to classify the functional properties of diverse thermal structures. Here, we formulate a heat diffusion invariant to reveal the explicit correlation between thermal functionality and diffusivity. The value goes beyond establishing a unified framework for various thermal metamaterials. The heat diffusion invariant offers a forward paradigm for precisely achieving freeform transient thermal metamaterials with isotropic thermal conductivity. We verify the competitiveness and robustness experimentally via a freeform transient thermal cloak. The heat diffusion invariant also paves the way for other functions, such as transient thermal illusion, and applies to thermal convection and radiation. These findings could open up an unprecedented invariant-based gateway to thermal management, metamaterial design, and nonequilibrium energy and mass transport.}, archive = {J_PRL}, author = {Liujun Xu and Pengfei Zhuang and Fubao Yang and Shuihua Yang and Chengmeng Wang and Gaole Dai and Jiping Huang and Cheng-Wei Qiu}, doi = {10.1103/cny8-szn7}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {067103}, shortjournal = {Phys. Rev. Lett.}, title = {Heat diffusion invariant}, volume = {135}, year = {2025}, }
• (2025). Large deviations in switching diffusion: From free cumulants to dynamical transitions. PRL, 135(6), 067102. (www)

  @article{ , abstract = {We study the diffusion of a particle with a time-dependent diffusion coefficient that switches between random values drawn from a distribution at a fixed rate . Using a renewal approach, we compute exactly the moments of the position of the particle at any finite time , and for any with finite moments . For , we demonstrate that the cumulants grow linearly with and are proportional to the free cumulants of a random variable distributed according to . For specific forms of , we compute the large deviations of the position of the particle, uncovering rich behaviors and dynamical transitions of the rate function . Our analytical predictions are validated numerically with high precision, achieving accuracy up to .}, archive = {J_PRL}, author = {Mathis Guéneau and Satya N. Majumdar and Grégory Schehr}, doi = {10.1103/rqsn-bzr6}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {067102}, shortjournal = {Phys. Rev. Lett.}, title = {Large deviations in switching diffusion: From free cumulants to dynamical transitions}, volume = {135}, year = {2025}, }
• (2025). Gambling carnot engine. PRL, 135(6), 067101. (www)

  @article{ , abstract = {We propose a theoretical model for a colloidal heat engine driven by a feedback protocol that is able to fully convert the net heat absorbed by the hot bath into extracted work. The feedback protocol, inspired by gambling strategies, executes a sudden quench at zero work cost when the particle position satisfies a specific first-passage condition. As a result, the engine enhances both power and efficiency with respect to a standard Carnot cycle, surpassing Carnot’s efficiency at maximum power. Using first-passage and martingale theory, we derive analytical expressions for the power and efficiency far beyond the quasistatic limit and provide scaling arguments for their dependency with the cycle duration. Numerical simulations are in perfect agreement with our theoretical findings, and illustrate the impact of the data acquisition rate on the engine’s performance.}, archive = {J_PRL}, author = {Tarek Tohme and Valentina Bedoya and Costantino di Bello and Léa Bresque and Gonzalo Manzano and Édgar Roldán}, doi = {10.1103/w8cx-xx1z}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {067101}, shortjournal = {Phys. Rev. Lett.}, title = {Gambling carnot engine}, volume = {135}, year = {2025}, }
• (2025). Coulomb sensing of single ballistic electrons. PRL, 135(6), 067002. (www)

  @article{ , abstract = {While ballistic electrons are a key tool for applications in sensing and flying qubits, sub-nanosecond propagation times and complicated interactions make control of ballistic single electrons challenging. Recent experiments have revealed Coulomb collisions of counterpropagating electrons in a beam splitter, giving time resolved control of interactions between single electrons. Here we use remote Coulomb interactions to demonstrate a scheme for sensing single ballistic electrons. We show that interactions are highly controllable via electron energy and emission timing. We use a weakly coupled “sensing” regime to characterize the nanoscale potential landscape of the beam splitter and the strength of the Coulomb interaction. We also show multielectron sensing with picosecond resolution.}, archive = {J_PRL}, author = {J. D. Fletcher and W. Park and P. See and J. P. Griffiths and G. A. C. Jones and I. Farrer and D. A. Ritchie and H.-S. Sim and M. Kataoka}, doi = {10.1103/f1gd-3p5m}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {067002}, shortjournal = {Phys. Rev. Lett.}, title = {Coulomb sensing of single ballistic electrons}, volume = {135}, year = {2025}, }
• (2025). Observation of coherent perfect acoustic absorption at an exceptional point. PRL, 135(6), 067001. (www)

  @article{ , abstract = {Non-Hermitian systems have recently shown new possibilities to manipulate wave scattering by exploiting loss, yet coherent perfect absorption at an exceptional point (CPA EP) remains elusive in acoustics. Here, we demonstrate it based on a two-channel waveguide with compact lossy resonators. We realize imbalanced losses crucial for CPA EP by using active components to independently modulate the non-Hermiticity. The CPA EP experimentally manifests as full absorption at a unique real frequency and shows high sensitivity to the incident phase variations. Our findings open an avenue to explore novel non-Hermitian physics for classical waves and develop innovative acoustic singularity-based devices.}, archive = {J_PRL}, author = {Yi-Fei Xia and Zi-Xiang Xu and Yu-Ting Yan and An Chen and Jing Yang and Bin Liang and Jian-Chun Cheng and Johan Christensen}, doi = {10.1103/slhy-f76q}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {067001}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of coherent perfect acoustic absorption at an exceptional point}, volume = {135}, year = {2025}, }
• (2025). Coherent coulomb intra- and intervalley many-body effects in single-layer transition metal dichalcogenides. PRL, 135(6), 066902. (www)

  @article{ , abstract = {The reduced Coulomb screening in single-layer (1L) transition metal dichalcogenides (TMDs) offers an ideal setting to explore excitonic many-body correlations. The interactions between excitons result in intra- and intervalley biexcitonic multiparticle states, whose contributions to the nonlinear optical response have remained elusive so far. Here, by using helicity-resolved transient absorption spectroscopy with sub-10 fs temporal resolution combined with a microscopic theory based on the excitonic Bloch equations we are able to unambiguously disentangle the contribution of two particle exciton and four particle biexciton correlations to the coherent optical response of semiconductor. Upon resonant excitation of valley-polarized A exciton population we observe competing excitation-induced energy shift of the A exciton transition along with a coherent gain in the pumped valley and an instantaneous formation of an additional absorption peak in the unpumped valley, which we attribute to the effect of bound intervalley biexcitons. An excellent agreement between experimental results and calculations allows us to deepen understanding of many-body effects in 1L-TMDs, which is crucial for the development of excitonic and valleytronics devices.}, archive = {J_PRL}, author = {Thomas Deckert and Henry Mittenzwey and Oleg Dogadov and Micol Bertolotti and Giulio Cerullo and Daniele Brida and Andreas Knorr and Stefano Dal Conte}, doi = {10.1103/j5cv-rffq}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066902}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent coulomb intra- and intervalley many-body effects in single-layer transition metal dichalcogenides}, volume = {135}, year = {2025}, }
• (2025). Multistate geometry of shift current and polarization. PRL, 135(6), 066901. (www)

  @article{ , abstract = {The quantum metric and Berry curvature capture essential properties of nontrivial Bloch states and underpin many fascinating phenomena. However, it becomes increasingly evident that a more comprehensive understanding of quantum state geometry is necessary to explain properties involving Bloch states of multiple bands, such as optical transitions. To this end, we employ quantum state projectors to develop an explicitly gauge-invariant formalism and demonstrate its power with applications to nonlinear optics and the theory of electronic polarization. We provide a simple expression for the shift current that resolves its precise relation to the moments of electronic polarization, clarifies the treatment of band degeneracies, and reveals its decomposition into the sum of the skewness of the occupied states and intrinsically multistate geometry. The projector approach is applied to calculate nonlinear optical properties of transition metal dichalcogenides (TMDs) layers, using previously calculated minimal tight-binding models, and demonstrated analytically on a three-band generalization of the Rice-Mele chain to elucidate the different contributions. We close with comments on further applications of the projector operator approach to multistate geometry.}, archive = {J_PRL}, author = {Alexander Avdoshkin and Johannes Mitscherling and Joel E. Moore}, doi = {10.1103/w761-8nf7}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066901}, shortjournal = {Phys. Rev. Lett.}, title = {Multistate geometry of shift current and polarization}, volume = {135}, year = {2025}, }
• (2025). Observation and control of chiral spin frustration in BiYIG thin films. PRL, 135(6), 066705. (www)

  @article{ , abstract = {Chiral interactions within magnetic layers stabilize the formation of noncollinear spin textures, which can be leveraged to design devices with tailored magnetization dynamics. Here, we introduce chiral spin frustration in which energetically degenerate magnetic states frustrate the Dzyaloshinskii-Moriya interaction. We demonstrate magnon-driven switching of the chirally frustrated spin states in Bi-substituted yttrium iron garnet thin films. These states are defined by an in-plane macrospin neighboring two out-of-plane spins on either side with opposing chirality. Using scanning nitrogen-vacancy magnetometry and spin pumping, we identified four degenerate frustrated states and achieved their controllable switching via magnon spin torque. Crucially, the switching is unidirectional, with selectivity determined by the incoming magnon direction. This mechanism provides a powerful approach to manipulate frustrated spin states with magnons. Chiral spin frustration unlocks the geometry constraints of conventional frustration, and therefore opens new horizons for frustrated magnetism, paving the way for energy-efficient spintronic devices based on frustration.}, archive = {J_PRL}, author = {Jinlong Wang and Hanchen Wang and Zhewen Xu and Artim L. Bassant and Junfeng Hu and Wenjie Song and Chaozhong Li and Xiangrui Meng and Mengqi Zhao and Song Liu and Guozhi Chai and Peng Gao and Wanjun Jiang and Desheng Xue and Dapeng Yu and William Legrand and Christian L. Degen and Rembert A. Duine and Pietro Gambardella and Haiming Yu}, doi = {10.1103/wjvv-lp7n}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066705}, shortjournal = {Phys. Rev. Lett.}, title = {Observation and control of chiral spin frustration in BiYIG thin films}, volume = {135}, year = {2025}, }
• (2025). Time-varying strong coupling and the induced time diffraction of magnon modes. PRL, 135(6), 066704. (www)

  @article{ , abstract = {Time-varying media break temporal translation symmetry, enabling advanced wave manipulation. However, this phenomenon remains largely unexplored in magnonic systems due to the challenge of achieving rapid and significant changes in magnon dispersion. Here, we construct a time-varying strong coupling between two magnon modes and observe chirped Rabi-like oscillations near the pulse edges. Developing a time-resolved frequency-comb spectroscopy technique, we characterize the frequency conversion of magnon modes induced by the time-varying strong-coupling effect. Moreover, we construct time slits with adjacent time interfaces and, for the first time, demonstrate the double-slit time diffraction of magnon modes, analogous to the well-known Young’s double-slit experiment. These findings rely solely on the time-varying strong coupling, independent of device reconfiguration. Our results open avenues for applications such as all-magnetic mixers or on-chip gigahertz sources.}, archive = {J_PRL}, author = {Jinwei Rao and Yi-Pu Wang and Zhijian Chen and Bimu Yao and Kaixin Zhao and Chunke Wei and Congyi Wang and Runze Li and Lihui Bai and Wei Lu}, doi = {10.1103/jc1c-k3ll}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066704}, shortjournal = {Phys. Rev. Lett.}, title = {Time-varying strong coupling and the induced time diffraction of magnon modes}, volume = {135}, year = {2025}, }
• (2025). Strong kitaev interaction in BaCo2(AsO4)2. PRL, 135(6), 066703. (www)

  @article{ , abstract = {The inelastic neutron scattering results and their analysis unequivocally point to a dominant Kitaev interaction in the honeycomb-lattice cobaltate . Our anisotropic-exchange model closely describes all available neutron scattering data in the material’s field-polarized phase. The density-matrix renormalization group results for our model are in close accord with the unusual double-zigzag magnetic order and the low in-plane saturation field of .}, archive = {J_PRL}, author = {Pavel A. Maksimov and Shengtao Jiang (蒋晟韬 and L. P. Regnault and A. L. Chernyshev}, doi = {10.1103/k1gq-k8m7}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066703}, shortjournal = {Phys. Rev. Lett.}, title = {Strong kitaev interaction in BaCo2(AsO4)2}, volume = {135}, year = {2025}, }
• (2025). Dynamically induced multiferroic polarization. PRL, 135(6), 066702. (www)

  @article{ , abstract = {We describe a mechanism by which both a ferroelectric polarization and a magnetization can be created in nonpolar, nonmagnetic materials. Using a combination of phenomenological modeling and first-principles calculations, we demonstrate that ferroelectric polarization, magnetization, or both simultaneously can be transiently induced by an ultrashort laser pulse upon linearly, circularly, or elliptically polarized excitation of phonon modes in . The direction and magnitude of the multiferroic polarization can be controlled by the chirality of the laser pulse and the phonon modes, offering a pathway for controlling multiferroicity and magnetoelectricity on ultrafast timescales.}, archive = {J_PRL}, author = {Carolina Paiva and Michael Fechner and Dominik M. Juraschek}, doi = {10.1103/7lm1-wm3y}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066702}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamically induced multiferroic polarization}, volume = {135}, year = {2025}, }
• (2025). Magnetic and ferroelectric phase diagram of twisted CrI3 layers. PRL, 135(6), 066701. (www)

  @article{ , abstract = {Twisting layers provide a rich ore for exotic physics in low dimensions. Despite the abundant discoveries of twistronics from the aspect of electronic structures, ferroic moiré textures are more plain and thus less concerned. Rigid lattice models are straightforward which can give a rough but intuitional description in most cases. However, taking as a model system, here we will demonstrate that the interlayer stacking potential can spontaneously lead to structural relaxation, which plays a vital role to understand the ferroicity in the twisted superlattices. The magnetic ground state is sensitive to the stacking mode and twisting angles, which can be seriously affected by the structural relaxation. In particular, the expected magnetic bubbles are annihilated in its bilayer. In contrast, due to topological protection, the ferroelectric vortices are more robust to structural relaxation, as well as twisting angle and thickness. Because of the universal existence of spontaneous structural relaxation in twisted superlattices, our work may lead to a general revisitation of emerging physics of twistronics.}, archive = {J_PRL}, author = {Haoshen Ye and Shuai Dong}, doi = {10.1103/bwwv-f247}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066701}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic and ferroelectric phase diagram of twisted CrI3 layers}, volume = {135}, year = {2025}, }
• (2025). Creating currents of electric skyrmion bubbles. PRL, 135(6), 066601. (www)

  @article{ , abstract = {The experimental demonstration of electric skyrmion bubbles and the recent prediction of their Brownian motion have brought topological ferroelectrics close to their magnetic counterparts. Electric bubbles (e-bubbles) could potentially be leveraged in applications for which magnetic skyrmions have been proposed (e.g., neuromorphic computing). Yet, we still lack a strategy to create currents of e-bubbles. Here, using predictive atomistic simulations, we illustrate two approaches to induce e-bubble currents by application of suitable electric fields, static or dynamic. We focus on regimes where e-bubbles display spontaneous diffusion, which allows us to generate a current by simply biasing their Brownian motion. Our calculations indicate that e-bubble velocities over can be achieved at room temperature, suggesting that these electric quasiparticles could rival the speeds of magnetic skyrmions upon further optimization.}, archive = {J_PRL}, author = {Jorge Íñiguez-González and Hugo Aramberri}, doi = {10.1103/fb55-3fks}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066601}, shortjournal = {Phys. Rev. Lett.}, title = {Creating currents of electric skyrmion bubbles}, volume = {135}, year = {2025}, }
• (2025). Metastability in coexisting competing orders. PRL, 135(6), 066501. (www)

  @article{ , abstract = {The dynamical phase transition of a system with two coexisting competing order parameters is studied using the time-dependent-Ginzburg-Landau framework. The dynamics are induced by parameters capturing the physics of driving the system with an ultrafast laser pulse. A remarkable enhancement of the order parameter with a smaller mean-field value following the pump and the emergence of an induced metastable state is investigated through analytical and numerical studies. The effect of order parameter fluctuations on the exploration of the nonequilibrium free energy landscape reveals important information about the impact of both thermal and nonthermal fluctuations on the dynamics of the metastable state. Our results provide an interpretation of previously unexplained ultrafast experiments on superconductors with competing charge density wave order. Our formalism is relevant across broad classes of out-of-equilibrium systems beyond the condensed matter context, such as the Kibble-Zurek cosmological model.}, archive = {J_PRL}, author = {Yasamin Masoumi and Alberto de la Torre and Gregory A. Fiete}, doi = {10.1103/3dm4-p2yq}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066501}, shortjournal = {Phys. Rev. Lett.}, title = {Metastability in coexisting competing orders}, volume = {135}, year = {2025}, }
• (2025). Mapping delocalization of impurity bands across archetypal mott-anderson transition. PRL, 135(6), 066302. (www)

  @article{ , abstract = {Tailoring charge transport in solids on demand is the overarching goal of condensed-matter research as it is crucial for electronic applications. Yet, often the proper tuning knob is missing and extrinsic factors such as impurities and disorder impede coherent conduction. Here, we control the very buildup of an electronic band from impurity states within the pseudogap of ternary Fe 2 − x V 1 + x Al Heusler compounds via reducing the Fe content. Our density-functional theory calculations combined with specific heat and electrical resistivity experiments reveal that, initially, these states are Anderson-localized at low V concentrations 0 < x < 0.1 . As x increases, we monitor the formation of mobility edges upon the archetypal Mott-Anderson transition and map the increasing bandwidth of conducting states by thermoelectric measurements. Ultimately, delocalization of charge carriers in fully disordered V 3 Al results in a resistivity exactly at the Mott-Ioffe-Regel limit that is perfectly temperature-independent up to 700 K—more constant than constantan.}, archive = {J_PRL}, author = {M. Parzer and F. Garmroudi and A. Riss and T. Mori and A. Pustogow and E. Bauer}, doi = {10.1103/fz9j-bj87}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066302}, shortjournal = {Phys. Rev. Lett.}, title = {Mapping delocalization of impurity bands across archetypal mott-anderson transition}, volume = {135}, year = {2025}, }
• (2025). Phase-biased andreev diffraction grating. PRL, 135(6), 066301. (www)

  @article{ , abstract = {In optical diffraction, the phase difference between sources in a grating or multislit mask is determined by the angle to the imaging screen, yielding the familiar multilobed diffraction image. Here, we realize a similar phenomenon in a superconductor-semiconductor hybrid circuit configured to allow Andreev scattering from multiple parallel scatterers. Phase differences between scatterers are set by tapping off of a remote superconducting meander. We investigate arrays with two, three, four, and ten Andreev scatterers, examining local and nonlocal diffraction patterns, finding good agreement with a theory of multiple Andreev scattering, not to be confused with multiple Andreev reflection. Adding current-carrying taps to the meander allows individual phase control.}, archive = {J_PRL}, author = {Magnus R. Lykkegaard and Anders Enevold Dahl and Tyler Lindemann and Michael J. Manfra and Karsten Flensberg and Charles M. Marcus}, doi = {10.1103/d4kk-sgmh}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066301}, shortjournal = {Phys. Rev. Lett.}, title = {Phase-biased andreev diffraction grating}, volume = {135}, year = {2025}, }
• (2025). Persistent spin grids with a spin-orbit-coupled 2D electron gas. PRL, 135(6), 066205. (www)

  @article{ , abstract = {We consider the diffusive spin dynamics of a 2D electron gas with spin-orbit coupling confined within a grid of narrow channels. We show that the lifetime of certain spin distributions in such grids greatly exceeds that in an unconfined 2D electron gas and diverges as the channel width approaches zero. Such persistent spin grids are akin to spin crystals and occur if the electron spin orientation remains invariant after diffusion around the grid plaquette. We establish a topological classification for persistent spin grids and show how the grids with spatially varying parameters can simulate non-Abelian lattice gauge theories.}, archive = {J_PRL}, author = {A. V. Poshakinskiy}, doi = {10.1103/ty86-f2yt}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066205}, shortjournal = {Phys. Rev. Lett.}, title = {Persistent spin grids with a spin-orbit-coupled 2D electron gas}, volume = {135}, year = {2025}, }
• (2025). Cold self-lubrication of sliding ice. PRL, 135(6), 066204. (www)

  @article{ , abstract = {The low kinetic friction between ice and numerous counterbodies is commonly attributed to an interfacial water layer, which is believed to originate from preexisting surface water or from melt water induced by high contact pressures or frictional heat. However, even the currently leading theory of frictional melting appears to defy direct experimental verification. Here we present molecular simulations of ice interfaces that reveal that ice surfaces liquefy without melting thermodynamically but predominantly by cold, displacement-driven amorphization. Despite effective self-lubrication, very small ice friction is found to require water to slip past a hydrophobic counterface—or an excess amount of water, produced by, e.g., extreme sliding velocities.}, archive = {J_PRL}, author = {Achraf Atila and Sergey V. Sukhomlinov and Martin H. Müser}, doi = {10.1103/1plj-7p4z}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066204}, shortjournal = {Phys. Rev. Lett.}, title = {Cold self-lubrication of sliding ice}, volume = {135}, year = {2025}, }
• (2025). Electrically induced bulk and edge excitations in the fractional quantum hall regime. PRL, 135(6), 066203. (www)

  @article{ , abstract = {We apply a voltage pulse to electrically excite the incompressible region of a two-dimensional electron liquid in the fractional quantum Hall state and investigate the collective excitations in both the bulk and edge via photoluminescence spectral energy shifts. Introducing an offset in the voltage pulse significantly enhances the excitation signal. Real-space and time-resolved measurements reveal the dynamics of the bulk excitations, with an estimated group velocity of approximately . These bulk excitations align well with the magnetoplasmon model. Because bulk and edge magnetoplasmons are composed of two polarization degrees of freedom of the gauge field, our results highlight a connection that could serve as a resource for their entanglement—similar to the polarization of a photon—and offer a novel approach to exploring solid-state analogs of quantum gravity.}, archive = {J_PRL}, author = {Quentin France and Yunhyeon Jeong and Akinori Kamiyama and Takaaki Mano and Ken-ichi Sasaki and Masahiro Hotta and Go Yusa}, doi = {10.1103/4bp5-9ryg}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066203}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically induced bulk and edge excitations in the fractional quantum hall regime}, volume = {135}, year = {2025}, }
• (2025). Polarons and exciton polarons in two-dimensional polar materials. PRL, 135(6), 066202. (www)

  @article{ , abstract = {We propose a macroscopic theory of optical phonons, Fröhlich polarons, and exciton polarons in two-dimensional (2D) polar crystalline monolayers. Our theory extends the classical macroscopic formulation of the electron-phonon problem in three-dimensional (3D) polar crystals to the new generation of 2D materials. Similarly to the 3D case, in our approach, the effective electron-phonon Hamiltonian is parametrized solely in terms of macroscopic experimentally accessible quantities—2D polarizabilities of the monolayer at low and high frequencies. We derive the dispersion of long wave length longitudinal optical (LO) phonons, which can be viewed as a 2D form of the Lyddane-Sachs-Teller relation, and study the formation of 2D Fröhlich polarons by adopting the intermediate coupling approximation. Finally, we apply this approach to excitons in polar 2D crystals and derive an effective potential of the electron-hole interaction dressed by LO phonons. Because of a specific dispersion of LO phonons, polarons and exciton polarons in 2D materials exhibit unique features not found in their 3D counterparts. As an illustration, the polaron and exciton polaron binding energies are computed for a representative set of 2D polar crystals, demonstrating the interplay between dimensionality, polarizability of materials, and electron-phonon coupling.}, archive = {J_PRL}, author = {V. Shahnazaryan and A. Kudlis and I. V. Tokatly}, doi = {10.1103/84p5-s6lj}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066202}, shortjournal = {Phys. Rev. Lett.}, title = {Polarons and exciton polarons in two-dimensional polar materials}, volume = {135}, year = {2025}, }
• (2025). Visualization of intervalley coherent phase in PtSe2/bilayer graphene heterojunction. PRL, 135(6), 066201. (www)

  @article{ , abstract = {The intervalley coherent (IVC) phase in graphene systems arises from the coherent superposition of wave functions of opposite valleys, whose direct microscopic visualization provides pivotal insight into the emergent physics. Here, we successfully visualize the IVC phase in a heterostructure of monolayer and bilayer-graphene (BLG) on graphite. Using spectroscopic imaging scanning tunneling microscopy, we observe a modulation pattern superimposed on the higher-order moiré superlattice of the heterostructure, which correlates with a gap-opening feature around the Fermi level and displays an antiphase real-space conductance distribution of the two gap edges. Such modulation pattern and small gap vanish on the heterostructure of monolayer on BLG-covered SiC substrate, due to the increased carrier density in the BLG. We provide a theoretical mechanism that the modulation pattern originates from the IVC phase of BLG, which is magnified by the higher-order moiré superlattice. Our work achieves visualization of the IVC phase, and develops an avenue for its generation and amplification via a moiré interface.}, archive = {J_PRL}, author = {Kai Fan and Ting-Fei Guo and Bohao Li and Wen-Xuan Qiu and Jian-Wang Zhou and Wen-Hao Zhang and Chao-Fei Liu and Fengcheng Wu and Ying-Shuang Fu}, doi = {10.1103/mbjb-x6mn}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066201}, shortjournal = {Phys. Rev. Lett.}, title = {Visualization of intervalley coherent phase in PtSe2/bilayer graphene heterojunction}, volume = {135}, year = {2025}, }
• (2025). Elastic amplification from negative capacitance. PRL, 135(6), 066101. (www)

  @article{ , abstract = {Ferroelectrics under suitable electric boundary conditions can present a negative capacitance response, whereby the total voltage drop across the ferroelectric opposes the externally applied bias. When the ferroelectric is in a heterostructure, this behavior yields a voltage amplification in the other elements, an effect that could be leveraged in low-power electronic devices. Interestingly, the mentioned voltage amplification should have an accompanying elastic effect. Specifically, in the typical case in which the materials in contact with the ferroelectric are nonpolar dielectrics, those should present an enhanced electrostrictive response. Here, we use atomistic simulations—of model PbTiO 3 / SrTiO 3 ferroelectric/dielectric superlattices displaying negative capacitance—to show that this is indeed the case: we reveal the enhanced elastic response of the dielectric layer and show that it is clearly linked to the voltage amplification. We argue that this “elastic amplification” could serve as a convenient experimental fingerprint for negative capacitance. Further, we propose that it may be of interest on its own, e.g., for the development of low-power electromechanical actuators.}, archive = {J_PRL}, author = {Mónica Graf and Natalya S. Fedorova and Hugo Aramberri and Jorge Íñiguez-González}, doi = {10.1103/5nqb-xj51}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066101}, shortjournal = {Phys. Rev. Lett.}, title = {Elastic amplification from negative capacitance}, volume = {135}, year = {2025}, }
• (2025). Emergent universal drag law in a model of superflow. PRL, 135(6), 066001. (www)

  @article{ , abstract = {Despite the fundamentally different dissipation mechanisms, many laws and phenomena of classical turbulence equivalently manifest in quantum turbulence. The Reynolds law of dynamical similarity states that two objects of the same geometry across different length scales are hydrodynamically equivalent under the same Reynolds number, leading to a universal drag coefficient law. In this Letter we confirm the existence of a universal drag law in a superfluid wake, facilitated by the nucleation of quantized vortices. We numerically study superfluid flow across a range of Reynolds numbers for the paradigmatic classical hard wall and the Gaussian obstacle, popular in experimental quantum hydrodynamics. In addition, we provide a feasible method for measuring superfluid drag forces in an experimental environment using control volumes.}, archive = {J_PRL}, author = {M. T. M. Christenhusz and A. Safavi-Naini and H. Rubinsztein-Dunlop and T. W. Neely and M. T. Reeves}, doi = {10.1103/s31t-tjl9}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {066001}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent universal drag law in a model of superflow}, volume = {135}, year = {2025}, }
• (2025). Charged particle cross-field transport due to geometric jumps of adiabatic invariant. PRL, 135(6), 065202. (www)

  @article{ , abstract = {We examine energetic electron transport in Earth’s outer radiation belt, presenting a mechanism for rapid (nondiffusive) radial transport. This process relies on electron crossings of an asymmetric separatrix in slow-fast Hamiltonian system, occurring in Earth’s dayside magnetosphere due to interactions with the interplanetary magnetic field. The resulting asymmetry quickly destroys adiabatic invariant through geometric jumps, driving exponential phase-space mixing and enhancing radial transport of ≳ 1 MeV electrons during geomagnetically quiet conditions.}, archive = {J_PRL}, author = {S. R. Kamaletdinov and A. V. Artemyev and A. I. Neishtadt and V. Angelopoulos}, doi = {10.1103/nsg2-scpg}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {065202}, shortjournal = {Phys. Rev. Lett.}, title = {Charged particle cross-field transport due to geometric jumps of adiabatic invariant}, volume = {135}, year = {2025}, }
• (2025). Leaking outside the box: Kinetic turbulence with cosmic-ray escape. PRL, 135(6), 065201. (www)

  @article{ , abstract = {We study particle acceleration in strongly turbulent pair plasmas using novel 3D particle-in-cell simulations, featuring particle injection from an external heat bath and diffusive escape. We demonstrate the formation of steady-state, nonthermal particle distributions with maximum energies reaching the Hillas limit. The steady state is characterized by the equilibration of plasma kinetic and magnetic pressures, which imposes upper limits on the acceleration rate. With growing cold plasma magnetization , nonthermal power-law spectra become harder, and the fraction of energy channeled into escaping cosmic rays increases. At , the escaping cosmic rays amount to more than 50% of the dissipated energy. Our method allows for kinetic studies of particle acceleration under steady-state conditions, with applications to a variety of astrophysical systems.}, archive = {J_PRL}, author = {Evgeny A. Gorbunov and Daniel Grošelj and Fabio Bacchini}, doi = {10.1103/3777-z37m}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {065201}, shortjournal = {Phys. Rev. Lett.}, title = {Leaking outside the box: Kinetic turbulence with cosmic-ray escape}, volume = {135}, year = {2025}, }
• (2025). Direct experimental proof of the principal role of reduced high-mode hydrodynamic mix in recent ignition success on NIF. PRL, 135(6), 065101. (www)

  @article{ , abstract = {This Letter details the role of reduced hydrodynamic mix in achieving the first fusion plasma to satisfy the Lawson criterion for ignition. Using novel 3D measurements of the temperature and density of the burning deuterium-tritium plasma across a series of experiments, we demonstrate that hydrodynamic mixing from small-scale capsule defects was a key degradation mechanism inhibiting ignition. A series of five layered deuterium-tritium experiments using 1.9 MJ of laser energy demonstrates a reduction of the thermonuclear yield when a lower quality capsule, typical of preignition experiments, is used. Radiation hydrodynamic calculations consistent with the observed mix profile show that the mixed fuel’s reduced compression and increased radiative loss explain the yield reduction. A hydroscaling argument suggests that a laser would be needed to reach ignition with such a capsule, well beyond the current capabilities of high energy laser systems. As such, this Letter gives critical insight into the physics of mix in self-heated fusion plasmas and establishes a foundation to evaluate capsule quality needs of future inertial fusion designs that aim at ignition and high gain.}, archive = {J_PRL}, author = {B. Bachmann and L. Divol and A. Pak and N. W. Birge and D. T. Casey and E. L. Dewald and B. Kozioziemski and A. L. Kritcher and A. Nikroo and J. E. Ralph and M. S. Rubery and P. T. Springer and S. Stoupin and K. W. Wong and A. B. Zylstra and S. H. Baxamusa and T. Braun and C. Choate and D. S. Clark and M. Durocher and D. Fittinghoff and M. S. Freeman and S. F. Khan and C. Kong and A. G. MacPhee and E. V. Marley and K. Meaney and A. Moore and M. Ratledge and N. W. Ruof and K. Sequoia and R. Simpson and M. Stadermann and R. Tommasini and C. Trosseille and P. Volegov and C. R. Weber and O. L. Landen and R. P. J. Town}, doi = {10.1103/sznp-zplz}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {065101}, shortjournal = {Phys. Rev. Lett.}, title = {Direct experimental proof of the principal role of reduced high-mode hydrodynamic mix in recent ignition success on NIF}, volume = {135}, year = {2025}, }
• (2025). Polarization faticons: Chiral localized structures in self-defocusing kerr resonators. PRL, 135(6), 063803. (www)

  @article{ , abstract = {We report on numerical predictions and experimental observations of a novel type of temporal localized dissipative structures that manifest themselves in the self-defocusing regime of driven nonlinear optical resonators with two polarization modes. These chiral dissipative solitons, which we term “polarization faticons,” break both temporal and polarization symmetry and consist of two bright lobes of opposite polarization handedness, interlocked by a domain wall. Our study reveals that faticons are connected to a vectorial modulational instability, from which they can be excited through a collapsing dynamic. Faticons could offer a novel pathway for frequency comb generation in normal dispersion resonators. More generally, they offer new fundamental insights into vectorial localized dissipative structures and could be relevant to other multicomponent dissipative systems.}, archive = {J_PRL}, author = {Erwan Lucas and Gang Xu and Pengxiang Wang and Gian-Luca Oppo and Lewis Hill and Pascal Del’Haye and Bertrand Kibler and Yiqing Xu and Stuart G. Murdoch and Miro Erkintalo and Stéphane Coen and Julien Fatome}, doi = {10.1103/ljbj-tz7g}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063803}, shortjournal = {Phys. Rev. Lett.}, title = {Polarization faticons: Chiral localized structures in self-defocusing kerr resonators}, volume = {135}, year = {2025}, }
• (2025). Photonic torons with 3D topology transitions and tunable spin monopoles. PRL, 135(6), 063802. (www)

  @article{ , abstract = {Topological defects and textures play crucial roles in fundamental physics and modern information science. Torons are a class of three-dimensional (3D) chiral topological structures with both skyrmionic quasiparticle textures and monopole point defects, so far only observed in liquid crystals with both polar and nonpolar symmetry. Here, we construct torons with the photonic spin of vector structured light and demonstrate the topological phase transitions among diverse 3D topological states: torons, hopfions, skyrmioniums and monopole pairs. We can also continually tune the toron’s chirality and monopole’s helicity. The generation of photonic torons opens a platform for studying nontrivial light-matter interaction and topological informatics.}, archive = {J_PRL}, author = {Haijun Wu and Nilo Mata-Cervera and Haiwen Wang and Zhihan Zhu and Chengwei Qiu and Yijie Shen}, doi = {10.1103/8pb4-zy7c}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063802}, shortjournal = {Phys. Rev. Lett.}, title = {Photonic torons with 3D topology transitions and tunable spin monopoles}, volume = {135}, year = {2025}, }
• (2025). Ising machine by dimensional collapse of nonlinear polarization oscillators. PRL, 135(6), 063801. (www)

  @article{ , abstract = {Ising machines show promise as ultrafast hardware for optimizations encoded in Ising Hamiltonians but fall short in terms of success rate and performance scaling. Here, we propose a novel Ising machine that exploits the three-dimensional nature of nonlinear polarization oscillators to counteract these limitations. Based on the evolution of the optical polarization in third-order nonlinear media, the high-dimensional machine reaches the Ising ground state by the mechanism of “dimensional collapse”: the dynamics on the Poincaré sphere undergoes a self-induced collapse into polarization fixed points mapping an Ising spin. Collapse from a spherical to a binary spin occurs when the polarization oscillator experiences iterative loss and anisotropic feedback. The photonic setup consists of polarization modulated pulses in a crystal subject to measurement and feedback. We numerically demonstrate the polarization machine achieves enhanced success probability on benchmark graphs and an exponential improvement in performance scaling with respect to coherent Ising machines due to its high-dimensional operation. The proposed Ising machine paves the way for a new class of Ising solvers with enhanced computing capabilities.}, archive = {J_PRL}, author = {Salvatore Chiavazzo and Marcello Calvanese Strinati and Claudio Conti and Davide Pierangeli}, doi = {10.1103/qs29-2xqc}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063801}, shortjournal = {Phys. Rev. Lett.}, title = {Ising machine by dimensional collapse of nonlinear polarization oscillators}, volume = {135}, year = {2025}, }
• (2025). Quantum synchronization of twin limit-cycle oscillators. PRL, 135(6), 063601. (www)

  @article{ , abstract = {Quantum synchronization has been a subject of intensive research in the last decade. In this Letter, we propose a quantum Liénard system whose classical equivalent features two limit cycles to one of which the system will converge. In the quantum case, both limit cycles coexist in a single steady state. Each of these limit cycles localizes to a distinct phase if coupled to an external drive: one quantum state can thus be assigned two phases. Furthermore, coupling two such oscillators leads to the simultaneous appearance of synchronization and a synchronization blockade. To shed light on this apparent paradoxical result, we introduce finer measures of quantum synchronization.}, archive = {J_PRL}, author = {Tobias Kehrer and Christoph Bruder and Parvinder Solanki}, doi = {10.1103/f97j-474c}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063601}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum synchronization of twin limit-cycle oscillators}, volume = {135}, year = {2025}, }
• (2025). Observation of kibble-zurek behavior across topological transitions of a chern band in ultracold atoms. PRL, 135(6), 063403. (www)

  @article{ , abstract = {The Kibble-Zurek (KZ) mechanism renders a theoretical framework for elucidating the formation of topological defects across continuous phase transitions. Nevertheless, it is not immediately clear whether the KZ mechanism applies to topological phase transitions. The direct experimental study for such a topic is hindered by quenching a certain parameter over orders of magnitude in topological materials. Instead, we investigate the KZ behavior across topological transitions of a Chern band in two-dimensional (2D) optical Raman lattices with quantum gases. Defined as the defects, excitation density is reconstructed via measuring the spin wave functions, with which the power-law scaling of total excitation density is extracted and such scaling could be interpreted within the KZ framework. Our work has heralded the commencement of experimentally exploring the KZ mechanism of the topological phase transitions.}, archive = {J_PRL}, author = {Huan Yuan and Chang-Rui Yi and Jia-Yu Guo and Xiang-Can Cheng and Rui-Heng Jiao and Jinyi Zhang and Shuai Chen and Jian-Wei Pan}, doi = {10.1103/5j5s-946k}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063403}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of kibble-zurek behavior across topological transitions of a chern band in ultracold atoms}, volume = {135}, year = {2025}, }
• (2025). Cryogenic optical lattice clock with 1.7×10−20 blackbody radiation stark uncertainty. PRL, 135(6), 063402. (www)

  @article{ , abstract = {Controlling the Stark perturbation from ambient thermal radiation is key to advancing the performance of many atomic frequency standards, including state-of-the-art optical lattice clocks (OLCs). We demonstrate a cryogenic OLC that utilizes a dynamically actuated radiation shield to control the perturbation at fractional frequency, a factor of beyond the best OLC to date. Our shield furnishes the atoms with a near-ideal cryogenic blackbody radiation (BBR) environment by rejecting external thermal radiation at the part-per-million level during clock spectroscopy, overcoming a key limitation with previous cryogenic BBR control solutions in OLCs. While the lowest BBR shift uncertainty is realized with cryogenic operation, we further exploit the radiation control that the shield offers over a wide range of temperatures to directly measure and verify the leading BBR Stark dynamic correction coefficient for ytterbium. This independent measurement reduces the literature-combined uncertainty of this coefficient by 30%, thus benefiting state-of-the-art Yb OLCs operated at room temperature. We verify the static BBR coefficient for Yb at the low level.}, archive = {J_PRL}, author = {Youssef S. Hassan and Kyle Beloy and Jacob L. Siegel and Takumi Kobayashi and Eric Swiler and Tanner Grogan and Roger C. Brown and Tristan Rojo and Tobias Bothwell and Benjamin D. Hunt and Adam Halaoui and Andrew D. Ludlow}, doi = {10.1103/4tky-jmsm}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063402}, shortjournal = {Phys. Rev. Lett.}, title = {Cryogenic optical lattice clock with 1.7×10−20 blackbody radiation stark uncertainty}, volume = {135}, year = {2025}, }
• (2025). Chirally protected state manipulation by tuning one-dimensional statistics. PRL, 135(6), 063401. (www)

  @article{ , abstract = {Chiral symmetry is broken by typical interactions in lattice models, but the statistical interactions embodied in the anyon-Hubbard model are an exception. This is an example for a correlated hopping model where chiral symmetry protects a degenerate zero-energy subspace. Complementary to the traditional approach of anyon braiding in real space, we adiabatically evolve the statistical parameter and find nontrivial Berry phases and holonomies in this chiral subspace. The corresponding states possess stationary checkerboard patterns in their -particle densities that are preserved under adiabatic manipulation. We give an explicit protocol for how these chirally protected zero-energy states can be prepared, observed, validated, and controlled.}, archive = {J_PRL}, author = {F. Theel and M. Bonkhoff and P. Schmelcher and T. Posske and N. L. Harshman}, doi = {10.1103/kzf6-yx24}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {063401}, shortjournal = {Phys. Rev. Lett.}, title = {Chirally protected state manipulation by tuning one-dimensional statistics}, volume = {135}, year = {2025}, }
• (2025). EMC effect of tritium and helium-3 from the JLab MARATHON experiment. PRL, 135(6), 062502. (www)

  @article{ , abstract = {Measurements of the EMC effect in the tritium and helium-3 mirror nuclei are reported. The data were obtained by the MARATHON Jefferson Lab experiment, which performed deep inelastic electron scattering from deuterium and the three-body nuclei, using a cryogenic gas target system and the high resolution spectrometers of the Hall A Facility of the Lab. The data cover the Bjorken range from 0.20 to 0.83, corresponding to a squared four-momentum transfer range from 2.7 to , and to an invariant mass of the final hadronic state greater than . The tritium EMC effect measurement is the first of its kind. The MARATHON experimental results are compared to results from previous measurements by DESY-HERMES and JLab–Hall C experiments, as well as with few-body theoretical predictions.}, archive = {J_PRL}, author = {Jefferson Lab Hall A Tritium Collaboration and D. Abrams and H. Albataineh and B. S. Aljawrneh and S. Alsalmi and D. Androic and K. Aniol and W. Armstrong and J. Arrington and H. Atac and T. Averett and C. Ayerbe Gayoso and X. Bai and J. Bane and S. Barcus and A. Beck and V. Bellini and H. Bhatt and D. Bhetuwal and D. Biswas and D. Blyth and W. Boeglin and D. Bulumulla and J. Butler and A. Camsonne and M. Carmignotto and J. Castellanos and J.-P. Chen and I. C. Cloët and E. O. Cohen and S. Covrig and K. Craycraft and R. Cruz-Torres and B. Dongwi and B. Duran and D. Dutta and N. Fomin and E. Fuchey and C. Gal and T. N. Gautam and S. Gilad and K. Gnanvo and T. Gogami and J. Gomez and C. Gu and A. Habarakada and T. Hague and J.-O. Hansen and M. Hattawy and F. Hauenstein and D. W. Higinbotham and R. J. Holt and E. W. Hughes and C. Hyde and H. Ibrahim and S. Jian and S. Joosten and A. Karki and B. Karki and A. T. Katramatou and C. Keith and C. Keppel and M. Khachatryan and V. Khachatryan and A. Khanal and A. Kievsky and D. King and P. M. King and I. Korover and S. A. Kulagin and K. S. Kumar and T. Kutz and N. Lashley-Colthirst and S. Li and W. Li and H. Liu and S. Liuti and N. Liyanage and P. Markowitz and R. E. McClellan and D. Meekins and S. Mey-Tal Beck and Z.-E. Meziani and R. Michaels and M. Mihovilovic and V. Nelyubin and D. Nguyen and Nuruzzaman and M. Nycz and R. Obrecht and M. Olson and V. F. Owen and E. Pace and B. Pandey and V. Pandey and M. Paolone and A. Papadopoulou and S. Park and S. Paul and G. G. Petratos and R. Petti and E. Piasetzky and R. Pomatsalyuk and S. Premathilake and A. J. R. Puckett and V. Punjabi and R. D. Ransome and M. N. H. Rashad and P. E. Reimer and S. Riordan and J. Roche and G. Salmè and N. Santiesteban and B. Sawatzky and A. Schmidt and B. Schmookler and S. Scopetta and J. Segal and E. P. Segarra and A. Shahinyan and S. Širca and N. Sparveris and T. Su and R. Suleiman and H. Szumila-Vance and A. S. Tadepalli and L. Tang and W. Tireman and F. Tortorici and G. M. Urciuoli and B. Wojtsekhowski and S. Wood and Z. H. Ye and Z. Y. Ye and J. Zhang}, doi = {10.1103/31xz-s84d}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {062502}, shortjournal = {Phys. Rev. Lett.}, title = {EMC effect of tritium and helium-3 from the JLab MARATHON experiment}, volume = {135}, year = {2025}, }
• (2025). Time-dependent density functional theory description of u238(n,f), pu240,242(n,f), and np237(n,f) reactions. PRL, 135(6), 062501. (www)

  @article{ , abstract = {In nuclei with an odd nucleon number the nonvanishing spin number density is the source of a pseudomagnetic field, which favors the splitting of the nucleon Cooper pairs. Such a pseudomagnetic field is generated always in the dynamics of any nucleus, but its effects on Cooper pairs are significantly enhanced in the dynamic evolution of nuclei with an odd number of nucleons. We present for the first time a microscopic study of the induced fission of the odd neutron compound nuclei U 239 , Pu 241 , 243 , and the odd proton, odd neutron compound nucleus Np 238 , performed within the time-dependent density functional theory extended to superfluid fermion systems, without any simplifying assumptions, with controlled numerical approximations, and for a very large number of initial conditions. Because of the presence of the unpaired odd nucleon(s), the time-reversal symmetry of the fission compound nucleus is spontaneously broken, an aspect routinely neglected in the most advanced microscopic approaches of the past. The emerging fission fragment properties are quite similar to the properties of fission fragments of neighboring even-even nuclei. The time from saddle-to-scission is often significantly longer in odd-odd or odd-mass nuclei than for even-even nuclei, since systems with unpaired nucleons are easier to excite and the potential energy surfaces of these nuclei have more structure, often resembling a very complicated obstacle course, rather than a more direct evolution of the nuclear shape from the top of the outer fission barrier to the scission configuration. The Pauli blocking approximation, often invoked in the literature, expected to inhibit the fission of nuclei with unpaired nucleons, is surprisingly strongly violated during the fission dynamics.}, archive = {J_PRL}, author = {Aurel Bulgac and Ibrahim Abdurrahman and Matthew Kafker and Ionel Stetcu}, doi = {10.1103/2k8k-vpng}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {062501}, shortjournal = {Phys. Rev. Lett.}, title = {Time-dependent density functional theory description of u238(n,f), pu240,242(n,f), and np237(n,f) reactions}, volume = {135}, year = {2025}, }
• (2025). Next-to-leading-order QCD predictions for the nucleon form factors. PRL, 135(6), 061901. (www)

  @article{ , abstract = {We accomplish for the first time the next-to-leading-order QCD computations of the leading-twist contributions to the Dirac nucleon form factors by applying the hard-collinear factorization theorem rigorously. Our predictions for these baryon form factors indicate that the one-loop perturbative corrections to the hard-gluon-exchange contributions are numerically substantial for a wide range of momentum transfers. Including further the soft nonfactorizable contributions, we then perform the state-of-the-art analysis of the Dirac nucleon form factors, allowing for the most robust determinations of the nucleon distribution amplitudes from the comparison with the experimental data.}, archive = {J_PRL}, author = {Yong-Kang Huang and Bo-Xuan Shi and Yu-Ming Wang and Xue-Chen Zhao}, doi = {10.1103/xz46-8ptk}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061901}, shortjournal = {Phys. Rev. Lett.}, title = {Next-to-leading-order QCD predictions for the nucleon form factors}, volume = {135}, year = {2025}, }
• (2025). Search for a neutral gauge boson with nonuniversal fermion couplings in vector boson fusion processes in proton-proton collisions at s=13 TeV. PRL, 135(6), 061803. (www)

  @article{ , abstract = {The first search for a heavy neutral spin-1 gauge boson ( ) with nonuniversal fermion couplings produced via vector boson fusion processes and decaying to tau leptons or bosons is presented. The analysis is performed using LHC data at , collected from 2016 to 2018 with the CMS experiment and corresponding to an integrated luminosity of . The data are consistent with the standard model predictions. Upper limits are set on the product of the cross section for production of the boson and its branching fraction to or . The presence of a boson decaying to ( ) is excluded for masses up to 2.45(1.60) TeV, depending on the boson coupling to standard model weak bosons, and assuming a ( ) branching fraction of 50%.}, archive = {J_PRL}, author = {CMS Collaboration and A. Hayrapetyan and A. Tumasyan and W. Adam and J. W. Andrejkovic and L. Benato and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and W. Waltenberger and C.-E. Wulz and T. Janssen and T. Van Laer and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Bilin and B. Clerbaux and A. K. Das and I. De Bruyn and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and J. Jaramillo and A. Khalilzadeh and F. A. Khan and K. Lee and A. Malara and S. Paredes and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and Y. Hong and J. Knolle and L. Lambrecht and D. Marckx and K. Mota Amarilo and K. Skovpen and N. Van Den Bossche and J. van der Linden and L. Wezenbeek and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and G. A. Alves and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and C. Mora Herrera and P. Rebello Teles and M. Soeiro and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and T. Laux Kuhn and M. Macedo and J. Martins and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and D. Laroze and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and A. Carvalho Antunes De Oliveira and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and L. Zhang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and K. Yi and J. Zhang and Y. Li and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and F. Ramirez and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and H. Abdalla and Y. Assran and B. El-mahdy and A. Lotfy and M. A. Mahmoud and K. Ehataht and M. Kadastik and T. Lange and S. Nandan and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and H. Kirschenmann and K. Osterberg and M. Voutilainen and S. Bharthuar and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Myllymäki and M. m. Rantanen and H. Siikonen and J. Tuominiemi and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and M. Kumar and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and G. Boldrini and P. Busson and A. Cappati and C. Charlot and M. Chiusi and T. D. Cuisset and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Nguyen and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and I. Lomidze and T. Toriashvili and Z. Tsamalaidze and V. Botta and S. Consuegra Rodríguez and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and D. Noll and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and C. Seth and A. Sharma and J. L. Spah and A. Stein and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and F. Blekman and K. Borras and A. Campbell and A. Cardini and C. Cheng and F. Colombina and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and Y. Otarid and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and A. Saggio and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bein and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and D. Hundhausen and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and B. Wiederspan and M. Wolf and S. Brommer and E. Butz and T. Chwalek and A. Dierlamm and A. Droll and U. Elicabuk and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and R. Koppenhöfer and O. Lavoryk and J. M. Lawhorn and M. Link and A. Lintuluoto and S. Maier and S. Mitra and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and N. Trevisani and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and P. Kontaxakis and G. Melachroinos and Z. Painesis and I. Papavergou and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and P. Major and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and T. Sheokand and J. B. Singh and A. Singla and A. Ahmed and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Baradia and S. Barman and S. Bhattacharya and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and T. Mishra and B. Parida and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and G. B. Mohanty and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and V. K. Muraleedharan Nair Bindhu and K. Naskar and A. Nayak and S. Nayak and K. Pal and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and N. Ferrara and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and C. Tuve and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and M. Alves Gallo Pereira and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and D. Bisello and P. Bortignon and G. Bortolato and A. Bragagnolo and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and F. Gasparini and S. Giorgetti and A. Gozzelino and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and M. Magherini and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. Aimè and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and A. C. Marini and D. Matos Figueiredo and A. Messineo and S. Mishra and M. Musich and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and C. Baldenegro Barrera and P. Barria and C. Basile and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and R. Gargiulo and E. Longo and L. Martikainen and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and V. Vladimirov and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and R. White and J. Babbar and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and B. Kim and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and J. Yoo and J. Goh and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and Y. W. Kim and S. Ko and H. Kwon and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and K. Hwang and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and F. Alazemi and K. Dreimanis and A. Gaile and C. Munoz Diaz and D. Osite and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and C. A. Mondragon Herrera and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and L. Grzanka and M. Malawski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and P. Fokow and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and S. Afanasiev and V. Alexakhin and D. Budkouski and I. Golutvin and I. Gorbunov and V. Karjavine and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and V. Palichik and V. Perelygin and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and V. Smirnov and O. Teryaev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and P. Levchenko and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and Yu. Andreev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and I. Tlisova and A. Toropin and T. Aushev and K. Ivanov and V. Gavrilov and N. Lychkovskaya and A. Nikitenko and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and V. Bunichev and M. Dubinin and L. Dudko and A. Gribushin and V. Klyukhin and O. Kodolova and S. Obraztsov and M. Perfilov and S. Petrushanko and V. Savrin and G. Vorotnikov and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and Y. Skovpen and V. Kachanov and D. Konstantinov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin and P. Adzic and P. Milenovic and D. Devetak and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and J. Alcaraz Maestre and Cristina F. Bedoya and J. A. Brochero Cifuentes and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. Llorente Merino and C. Martin Perez and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and S. Sánchez Navas and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and P. Leguina and E. Palencia Cortezon and J. Prado Pico and C. Ramón Álvarez and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Bhowmik and S. Blanco Fernández and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and A. A. Bin Anuar and A. Bocci and L. Borgonovi and C. Botta and E. Brondolin and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and O. Karacheban and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and L. Malgeri and M. Mannelli and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and H. Qu and D. Rabady and B. Ribeiro Lopes and F. Riti and M. Rovere and H. Sakulin and R. Salvatico and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and K. A. Wozniak and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and A. Samalan and T. K. Aarrestad and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and B. Ristic and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and L. Ceard and K. F. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and D. Tsionou and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and U. Kiminsu and Y. Komurcu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and S. Turkcapar and E. Uslan and I. S. Zorbakir and G. Sokmen and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and G. G. Dincer and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and V. J. Smith and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and C. E. Brown and O. Buchmuller and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and A. Howard and G. Iles and C. R. Knight and P. Krueper and J. Langford and K. H. Law and J. León Holgado and L. Lyons and A.-M. Magnan and B. Maier and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and E. Collins and M. R. Darwish and J. Dittmann and K. Hatakeyama and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and A. E. Simsek and S. S. Yu and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and C. Cosby and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Barone and G. Benelli and D. Cutts and L. Gouskos and M. Hadley and U. Heintz and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and D. Li and J. Luo and S. Mondal and T. Russell and S. Sagir and X. Shen and F. Simpson and M. Stamenkovic and N. Venkatasubramanian and X. Yan and S. Abbott and B. Barton and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and S. Yoo and F. Zhang and K. Adamidis and M. Bachtis and D. Campos and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and Y. f. Lo and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and G. Hanson and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and M. Quinnan and B. V. Sathia Narayanan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and S. Wang and D. Zhang and A. Bornheim and O. Cerri and A. Latorre and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and G. Karathanasis and N. Manganelli and J. Pearkes and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and S. Bright-Thonney and X. Chen and D. J. Cranshaw and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and J. Dickinson and I. Dutta and V. D. Elvira and Y. Feng and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and R. Heller and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and C. Lee and D. Lincoln and R. Lipton and T. Liu and C. Madrid and K. Maeshima and C. Mantilla and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and C. Huh and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and M. M. Baarmand and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and A. H. Merrit and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and T. Roy and S. Rudrabhatla and N. Singh and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and E. Popova and A. Shevelev and L. Wang and J. Bendavid and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and M. I. Park and C. Paus and C. Reissel and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and B. M. Joshi and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and B. Bylsma and M. Campana and J. Dervan and Y. Haddad and Y. Han and I. Israr and A. Krishna and J. Li and M. Lu and G. Madigan and R. Mccarthy and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and D. Wood and J. Bueghly and S. Dittmer and K. A. Hahn and Y. Liu and M. Mcginnis and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. W. Ho and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and D. A. Wenzl and B. L. Winer and B. R. Yates and H. Bouchamaoui and K. Coldham and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and D. Stickland and C. Tully and L. H. Vage and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and V. Scheurer and J. F. Schulte and M. Stojanovic and J. Thieman and A. K. Virdi and F. Wang and A. Wildridge and W. Xie and Y. Yao and J. Dolen and N. Parashar and A. Pathak and D. Acosta and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and I. Krommydas and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and J. Reichert and H. Routray and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and H. Wang and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and K. Androsov and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and D. Rathjens and A. Safonov and N. Akchurin and J. Damgov and N. Gogate and V. Hegde and A. Hussain and Y. Kazhykarim and K. Lamichhane and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and H. Chung and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Neu and P. E. Karchin and A. Aravind and K. Black and T. Bose and E. Chavez and S. Dasu and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden}, doi = {10.1103/srvm-f1h3}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061803}, shortjournal = {Phys. Rev. Lett.}, title = {Search for a neutral gauge boson with nonuniversal fermion couplings in vector boson fusion processes in proton-proton collisions at s=13 TeV}, volume = {135}, year = {2025}, }
• (2025). First measurement of νe and ν¯e charged-current single charged-pion production differential cross sections on argon using the MicroBooNE detector. PRL, 135(6), 061802. (www)

  @article{ , abstract = {Understanding electron neutrino interactions is crucial for measurements of neutrino oscillations and searches for new physics in neutrino experiments. We present the first measurement of the flux-averaged charged-current single charged-pion production cross section on argon using the MicroBooNE detector and data from the NuMI neutrino beam. The total cross section is measured to be at a mean energy of 730 MeV. Differential cross sections are also reported in electron energy, electron and pion angles, and electron-pion opening angle.}, archive = {J_PRL}, author = {MicroBooNE Collaboration and P. Abratenko and D. Andrade Aldana and L. Arellano and J. Asaadi and A. Ashkenazi and S. Balasubramanian and B. Baller and A. Barnard and G. Barr and D. Barrow and J. Barrow and V. Basque and J. Bateman and O. Benevides Rodrigues and S. Berkman and A. Bhat and M. Bhattacharya and M. Bishai and A. Blake and B. Bogart and T. Bolton and M. B. Brunetti and L. Camilleri and D. Caratelli and F. Cavanna and G. Cerati and A. Chappell and Y. Chen and J. M. Conrad and M. Convery and L. Cooper-Troendle and J. I. Crespo-Anadón and R. Cross and M. Del Tutto and S. R. Dennis and P. Detje and R. Diurba and Z. Djurcic and K. Duffy and S. Dytman and B. Eberly and P. Englezos and A. Ereditato and J. J. Evans and C. Fang and W. Foreman and B. T. Fleming and D. Franco and A. P. Furmanski and F. Gao and D. Garcia-Gamez and S. Gardiner and G. Ge and S. Gollapinni and E. Gramellini and P. Green and H. Greenlee and L. Gu and W. Gu and R. Guenette and P. Guzowski and L. Hagaman and M. D. Handley and O. Hen and C. Hilgenberg and G. A. Horton-Smith and A. Hussain and B. Irwin and M. S. Ismail and C. James and X. Ji and J. H. Jo and R. A. Johnson and D. Kalra and G. Karagiorgi and W. Ketchum and M. Kirby and T. Kobilarcik and N. Lane and J.-Y. Li and Y. Li and K. Lin and B. R. Littlejohn and L. Liu and W. C. Louis and X. Luo and T. Mahmud and C. Mariani and J. Marshall and N. Martinez and D. A. Martinez Caicedo and S. Martynenko and A. Mastbaum and I. Mawby and N. McConkey and L. Mellet and J. Mendez and J. Micallef and A. Mogan and T. Mohayai and M. Mooney and A. F. Moor and C. D. Moore and L. Mora Lepin and M. M. Moudgalya and S. Mulleriababu and D. Naples and A. Navrer-Agasson and N. Nayak and M. Nebot-Guinot and C. Nguyen and J. Nowak and N. Oza and O. Palamara and N. Pallat and V. Paolone and A. Papadopoulou and V. Papavassiliou and H. B. Parkinson and S. F. Pate and N. Patel and Z. Pavlovic and E. Piasetzky and K. Pletcher and I. Pophale and X. Qian and J. L. Raaf and V. Radeka and A. Rafique and M. Reggiani-Guzzo and J. Rodriguez Rondon and M. Rosenberg and M. Ross-Lonergan and I. Safa and D. W. Schmitz and A. Schukraft and W. Seligman and M. H. Shaevitz and R. Sharankova and J. Shi and E. L. Snider and S. Söldner-Rembold and J. Spitz and M. Stancari and J. St. John and T. Strauss and A. M. Szelc and N. Taniuchi and K. Terao and C. Thorpe and D. Torbunov and D. Totani and M. Toups and A. Trettin and Y.-T. Tsai and J. Tyler and M. A. Uchida and T. Usher and B. Viren and J. Wang and M. Weber and H. Wei and A. J. White and S. Wolbers and T. Wongjirad and K. Wresilo and W. Wu and E. Yandel and T. Yang and L. E. Yates and H. W. Yu and G. P. Zeller and J. Zennamo and C. Zhang}, doi = {10.1103/sfrz-c8m9}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061802}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of νe and ν¯e charged-current single charged-pion production differential cross sections on argon using the MicroBooNE detector}, volume = {135}, year = {2025}, }
• (2025). Precision measurement of the branching fraction of d+→μ+νμ. PRL, 135(6), 061801. (www)

  @article{ , abstract = {Using of collision data collected at a center-of-mass energy of with the BESIII detector operating at the BEPCII collider, we determine the branching fraction of the leptonic decay to be . Interpreting our measurement with knowledge of the Fermi coupling constant , the masses of the and as well as the lifetime of the , we determine after taking into account necessary radiative corrections. This result is a factor of 2.3 more precise than the previous best measurement. Using the value of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element given by the global standard model fit, we obtain the decay constant . Alternatively, using the value of from a precise lattice quantum chromodynamics calculation, we extract .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and J. F. Chang and G. R. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and J. J. Lane and L. Lavezzi and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. Ma and Y. M. Ma and F. E. Maas and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and H. C. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. X. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. D. Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and Z. Z. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/gb8v-4rnh}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061801}, shortjournal = {Phys. Rev. Lett.}, title = {Precision measurement of the branching fraction of d+→μ+νμ}, volume = {135}, year = {2025}, }
• (2025). Spectral constraints on theories of colored particles and gravity. PRL, 135(6), 061604. (www)

  @article{ , abstract = {In this Letter, we consider effective field theories for light fields transforming under the fundamental or adjoint representation of a continuous group. Assuming tree-level completions, we demonstrate that, in the presence of gravity, crossing symmetry combined with twice-subtracted sum rules leads to constraints on the irreducible representations that the ultraviolet degrees of freedom must populate. A spectrum is allowed only if its low energy projection contains the graviton pole. Beautifully, the graviton pole is the anchor of our argument, not an obstruction.}, archive = {J_PRL}, author = {Aaron Hillman and Yu-tin Huang and Laurentiu Rodina and Justinas Rumbutis}, doi = {10.1103/k23f-y47w}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061604}, shortjournal = {Phys. Rev. Lett.}, title = {Spectral constraints on theories of colored particles and gravity}, volume = {135}, year = {2025}, }
• (2025). Universality of rényi entropy in conformal field theory. PRL, 135(6), 061603. (www)

  @article{ , abstract = {We use the thermal effective theory to prove that, for the vacuum state in any conformal field theory in dimensions, the th Rényi entropy behaves as in the limit when the boundary of the entanglement domain is spherical with the UV cutoff . The theory dependence is encapsulated in the cosmological constant in the thermal effective action. Using this result, we estimate the density of states for large eigenvalues of the modular Hamiltonian for the domain . In two dimensions, we can use the hot spot idea, which describes the effective action in the high-temperature limit when the temperature is position-dependent, to derive more powerful formulas valid for arbitrary positive . We discuss the difference between two and higher dimensions and clarify the applicability of the hot spot idea. We also use the thermal effective theory to derive an analog of the Cardy formula for boundary operators in higher dimensions.}, archive = {J_PRL}, author = {Yuya Kusuki and Hirosi Ooguri and Sridip Pal}, doi = {10.1103/fsg7-bs7q}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061603}, shortjournal = {Phys. Rev. Lett.}, title = {Universality of rényi entropy in conformal field theory}, volume = {135}, year = {2025}, }
• (2025). Entanglement entropy as a probe beyond the horizon. PRL, 135(6), 061602. (www)

  @article{ , abstract = {The entanglement entropy of a free field in de Sitter space is enhanced by the squeezing of its modes. We show analytically that the expansion induces a term in the entanglement entropy that depends logarithmically on the size of the overall system, which may extend beyond the horizon. In cosmology the size of the system can be identified with the size of a spatially finite universe or with the wavelength of the first mode that exited the horizon in the beginning of inflation.}, archive = {J_PRL}, author = {Konstantinos Boutivas and Dimitrios Katsinis and Georgios Pastras and Nikolaos Tetradis}, doi = {10.1103/mmd6-7zzl}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061602}, shortjournal = {Phys. Rev. Lett.}, title = {Entanglement entropy as a probe beyond the horizon}, volume = {135}, year = {2025}, }
• (2025). Holography for the ishibashi-kawai-kitazawa-tsuchiya matrix model. PRL, 135(6), 061601. (www)

  @article{ , abstract = {Holographic dualities that relate type II strings on near-horizon brane geometries to super Yang-Mills theories with sixteen supercharges in dimensions provide nonconformal generalizations of the famous AdS/CFT correspondence. For the extremal case , this suggests a holographic duality for the Ishibashi-Kawai-Kitazawa-Tsuchiya (IKKT) matrix model—super Yang-Mills theory reduced to zero dimensions. Despite intriguing and highly nontrivial results in the IKKT model, this duality has remained largely unexplored so far. In this Letter, we consider the lowest supermultiplet of gauge invariant operators of the model and identify its states with the lowest Kaluza-Klein fluctuations of (Euclidean) IIB supergravity on the instanton background. We construct its holographic bulk realization as a one-dimensional maximal supergravity with 32 supercharges and local SO(10) invariance, capturing the full nonlinear dynamics. Analyzing the bulk Killing spinor equations, we construct the most general half-supersymmetric solutions, which typically break SO(10). We present their uplifts to IIB supergravity, and furthermore to waves in twelve dimensions. These results provide the minimal setup for conducting precision tests of holography involving Einstein gravity.}, archive = {J_PRL}, author = {Franz Ciceri and Henning Samtleben}, doi = {10.1103/fb8g-b8fd}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061601}, shortjournal = {Phys. Rev. Lett.}, title = {Holography for the ishibashi-kawai-kitazawa-tsuchiya matrix model}, volume = {135}, year = {2025}, }
• (2025). Wheeler-DeWitt equation and bondi-metzner-sachs (BMS) symmetry. PRL, 135(6), 061501. (www)

  @article{ , abstract = {The Hamiltonian formulation of the BMS symmetry on spacelike hypersurfaces enables one to define its action on solutions of the Wheeler-DeWitt equation. Using the Becchi-Rouet-Stora-Tyutin (BRST) reformulation of the theory, we provide operator expressions for the matrix elements of the BMS operators between Wheeler-DeWitt states. To that end, we construct the BRST-invariant extensions of the BMS generators, which form a BRST extension of the BMS algebra.}, archive = {J_PRL}, author = {Marc Henneaux}, doi = {10.1103/29w3-3mmc}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061501}, shortjournal = {Phys. Rev. Lett.}, title = {Wheeler-DeWitt equation and bondi-metzner-sachs (BMS) symmetry}, volume = {135}, year = {2025}, }
• (2025). Search for higher harmonic signals from close white dwarf binaries in the mHz band. PRL, 135(6), 061402. (www)

  @article{ , abstract = {Space-based gravitational wave (GW) detectors, such as LISA, are expected to detect thousands of Galactic close white dwarf binaries emitting nearly monochromatic GWs. In this study, we demonstrate that LISA is reasonably likely to detect higher harmonic GW signals, particularly the ( l , | m | ) = ( 3 , 3 ) mode, from a limited sample of nearby close white dwarf binaries, even with small orbital velocities v / c of order 10 − 3 . The amplitudes of these post-Newtonian modes provide robust probes of mass asymmetry in such systems, making them valuable observational targets, especially in mass-transferring binaries. Long-term, coordinated detector operations will further improve the prospects for detecting these informative signals.}, archive = {J_PRL}, author = {Naoki Seto}, doi = {10.1103/mqjd-rwrb}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061402}, shortjournal = {Phys. Rev. Lett.}, title = {Search for higher harmonic signals from close white dwarf binaries in the mHz band}, volume = {135}, year = {2025}, }
• (2025). Nature of phase transitions and metastability in scalar-tensor theories. PRL, 135(6), 061401. (www)

  @article{ , abstract = {Compact stars above a critical stellar mass develop large scalar fields in some scalar-tensor theories. This scenario called spontaneous scalarization has been an intense topic of study since it passes weak-field gravity tests naturally while providing clear observables in the strong-field regime. The underlying mechanism for the onset of scalarization is often depicted as a second-order phase transition. Here, we show that a first-order phase transition is in fact the most common mechanism. This means metastability and transitions between locally stable compact object configurations are much more likely than previously believed, opening vast new avenues for observational prospects.}, archive = {J_PRL}, author = {K𝚤vanç İ. Ünlütürk and Semih Tuna and Oğuzhan K. Yamak and Fethi M. Ramazanoğlu}, doi = {10.1103/14xz-d7xf}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061401}, shortjournal = {Phys. Rev. Lett.}, title = {Nature of phase transitions and metastability in scalar-tensor theories}, volume = {135}, year = {2025}, }
• (2025). Deciphering the soliton-halo relation in fuzzy dark matter. PRL, 135(6), 061002. (www)

  @article{ , abstract = {Soliton cores at the center of fuzzy dark matter (FDM) halos provide a promising way to distinguish FDM from other dark matter models. However, the relation between solitons and their host halos remains contentious. Here, we rigorously examine this soliton-halo relation (SHR) using a rich set of cosmological simulations across various FDM particle masses, halo masses, and redshifts. We explicitly demonstrate thermal equilibrium between solitons and surrounding halo granules, energy equipartition within halos, and an FDM concentration-mass-nonisothermality relation. For each FDM halo, we confirm that its density profile outside the central soliton matches a collisionless N-body simulation from the same initial condition, serving as stringent numerical convergence tests. Our refined SHR agrees well with virialized halos in simulations, with a deviation of less than 30%. These findings not only reaffirm the SHR proposed by Schive et al. [Understanding the core-halo relation of quantum wave dark matter from 3D simulations, Phys. Rev. Lett. 113 , 261302 (2014) ] but also offer a more comprehensive understanding that extends its applicability.}, archive = {J_PRL}, author = {Pin-Yu Liao (廖品瑜 and Guan-Ming Su (蘇冠銘 and Hsi-Yu Schive (薛熙于 and Alexander Kunkel and Hsinhao Huang (黃新豪 and Tzihong Chiueh (闕志鴻}, doi = {10.1103/9dqj-q6mt}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061002}, shortjournal = {Phys. Rev. Lett.}, title = {Deciphering the soliton-halo relation in fuzzy dark matter}, volume = {135}, year = {2025}, }
• (2025). Complete gravitational-wave spectrum of the sun. PRL, 135(6), 061001. (www)

  @article{ , abstract = {The high-temperature plasma in the solar interior generates stochastic gravitational waves (GWs). Owing to its significance as the primary source of high-frequency GWs in the Solar System, we reexamine this phenomenon by highlighting some physical processes, including the contribution of macroscopic hydrodynamic fluctuations. Our analysis builds upon several studies of axion emission from the Sun, particularly in relation to the treatment of plasma effects. The resulting GW spectrum is comparable to many well-motivated early-Universe signals, yet orders of magnitude below the current sensitivities of axion helioscopes such as (Baby)IAXO.}, archive = {J_PRL}, author = {Camilo García-Cely and Andreas Ringwald}, doi = {10.1103/gtwg-pr41}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {061001}, shortjournal = {Phys. Rev. Lett.}, title = {Complete gravitational-wave spectrum of the sun}, volume = {135}, year = {2025}, }
• (2025). Longitudinal and nonlinear coupling for high-fidelity readout of a superconducting qubit. PRL, 135(6), 060803. (www)

  @article{ , abstract = {Despite the significant progress in superconducting quantum computation over the past years, quantum state measurement still lags nearly an order of magnitude behind quantum gate operations in speed and fidelity. The main challenge is that the strong coupling and readout signal used to probe the quantum state may also introduce additional channels which may cause qubit state transitions. Here, we design a novel architecture to implement the long-sought longitudinal interaction scheme between qubits and resonators. This architecture not only provides genuine longitudinal interaction by eliminating residual transversal couplings, but also introduces proper nonlinearity to the resonator that can further minimize decay error and measurement-induced excitation error. Combined with the multilevel readout protocol, we achieved a measurement fidelity of 99.8% in 202 ns without requiring any first-stage amplification. This highlights its potential as a highly promising architecture for superconducting qubit measurement.}, archive = {J_PRL}, author = {Can Wang and Feng-Ming Liu and He Chen and Yi-Fei Du and Chong Ying and Jian-Wen Wang and Yong-Heng Huo and Cheng-Zhi Peng and Xiaobo Zhu and Ming-Cheng Chen and Chao-Yang Lu and Jian-Wei Pan}, doi = {10.1103/98n9-13y4}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060803}, shortjournal = {Phys. Rev. Lett.}, title = {Longitudinal and nonlinear coupling for high-fidelity readout of a superconducting qubit}, volume = {135}, year = {2025}, }
• (2025). Continuous-variable designs and design-based shadow tomography from random lattices. PRL, 135(6), 060802. (www)

  @article{ , abstract = {We investigate state designs for continuous-variable quantum systems using the aid of latticelike quantum states. These are code states of Gottesman-Kitaev-Preskill (GKP) codes. We show that the set of all GKP states forms a rigged continuous-variable state 2-design for an -mode system. We use these lattice state designs to construct a continuous variable shadow tomography protocol, derive sample complexity bounds for both global and local GKP shadows under reasonable physical assumptions, and provide the physical gadgets needed to implement this protocol.}, archive = {J_PRL}, author = {Jonathan Conrad and Joseph T. Iosue and Ansgar G. Burchards and Victor V. Albert}, doi = {10.1103/dy4m-gq5c}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060802}, shortjournal = {Phys. Rev. Lett.}, title = {Continuous-variable designs and design-based shadow tomography from random lattices}, volume = {135}, year = {2025}, }
• (2025). Optimal overlapping tomography. PRL, 135(6), 060801. (www)

  @article{ , abstract = {Characterizing large-scale quantum systems is central to fundamental physics and essential for applications of quantum technologies. While a full characterization requires exponentially increasing resources, focusing on application-relevant information can often lead to significantly simplified analysis. Overlapping tomography is such a scheme, allowing one to obtain all the information contained in specific subsystems of multiparticle quantum systems in an efficient manner, but the ultimate limits of this approach remain elusive. We present protocols for overlapping tomography that are optimal with respect to the number of measurement settings. First, by providing algorithmic approaches based on graph theory we find the minimal number of Pauli settings, relating overlapping tomography to the problem of covering arrays in combinatorics. This significantly reduces the number of measurement settings, showing for instance that two-body overlapping tomography of nearest neighbors in qubit systems with planar topologies can always be performed with nine Pauli settings. Second, we prove that using general projective measurements, all -body marginals can be reconstructed with only settings, independently of the system size. Finally, we demonstrate the practical applicability of our methods in a six-photon experiment. Our results will find applications in learning noise and interaction patterns in quantum computers as well as characterizing fermionic systems in quantum chemistry.}, archive = {J_PRL}, author = {Kiara Hansenne and Rui Qu and Lisa T. Weinbrenner and Carlos de Gois and Haifei Wang and Yang Ming and Zhengning Yang and Paweł Horodecki and Weibo Gao and Otfried Gühne}, doi = {10.1103/t6qb-kdcp}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060801}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal overlapping tomography}, volume = {135}, year = {2025}, }
• (2025). AI-enabled parallel assembly of thousands of defect-free neutral atom arrays. PRL, 135(6), 060602. (www)

  @article{ , abstract = {Assembling increasingly larger-scale defect-free optical-tweezer-trapped atom arrays is essential for quantum computation and quantum simulations based on atoms. Here, we propose an AI-enabled, rapid, constant-time-overhead rearrangement protocol, and we experimentally assemble defect-free 2D and 3D atom arrays with up to 2024 atoms with a constant-time cost of 60 ms. The AI model calculates the holograms for real-time atom rearrangement. With precise controls over both position and phase, a high-speed spatial light modulator moves all the atoms simultaneously. This protocol can be readily used to generate defect-free arrays of tens of thousands of atoms with current technologies and become a useful toolbox for quantum error correction.}, archive = {J_PRL}, author = {Rui Lin and Han-Sen Zhong and You Li and Zhang-Rui Zhao and Le-Tian Zheng and Tai-Ran Hu and Hong-Ming Wu and Zhan Wu and Wei-Jie Ma and Yan Gao and Yi-Kang Zhu and Zhao-Feng Su and Wan-Li Ouyang and Yu-Chen Zhang and Jun Rui and Ming-Cheng Chen and Chao-Yang Lu and Jian-Wei Pan}, doi = {10.1103/2ym8-vs82}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060602}, shortjournal = {Phys. Rev. Lett.}, title = {AI-enabled parallel assembly of thousands of defect-free neutral atom arrays}, volume = {135}, year = {2025}, }
• (2025). Scalable improvement of the generalized toffoli gate realization using trapped-ion-based qutrits. PRL, 135(6), 060601. (www)

  @article{ , abstract = {An efficient implementation of the Toffoli gate is of conceptual importance for running various quantum algorithms, including Grover’s search and Shor’s integer factorization. However, direct implementation of the Toffoli gate either entails a prohibitive increase in the number of two-qubit gates or requires ancilla qubits, whereas both of these resources are limited in the current generation of noisy intermediate-scale quantum devices. Here, we experimentally demonstrate a scalable -qubit Toffoli gate improvement using trapped-ion-based optical-metastable-ground encoded qutrits for the cases of up to . With the use of the Mølmer-Sørensen gate as a basic entangling operation, we compare the standard qubit decomposition with the qutrit approach, where upper levels are used as ancillae. The presented decomposition requires only global control of the ancilla levels, which simplifies experimental implementation of the proposed approach. Using the example of a three-qubit Grover’s search, we also demonstrate an increase in the algorithm’s accuracy by monitoring the leakage from the qubit subspace during a qutrit-based Toffoli gate implementation.}, archive = {J_PRL}, author = {Anastasiia S. Nikolaeva and Ilia V. Zalivako and Alexander S. Borisenko and Nikita V. Semenin and Kristina P. Galstyan and Andrey E. Korolkov and Evgeniy O. Kiktenko and Ksenia Yu. Khabarova and Ilya A. Semerikov and Aleksey K. Fedorov and Nikolay N. Kolachevsky}, doi = {10.1103/p1z9-6w93}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060601}, shortjournal = {Phys. Rev. Lett.}, title = {Scalable improvement of the generalized toffoli gate realization using trapped-ion-based qutrits}, volume = {135}, year = {2025}, }
• (2025). Quantum enhancement of thermalization. PRL, 135(6), 060404. (www)

  @article{ , abstract = {Equilibrium properties of many-body systems with a large number of degrees of freedom are generally expected to be described by statistical mechanics. Such expectations are closely tied to the observation of thermalization, as manifested through equipartition in time-dependent observables, which takes place both in quantum and classical systems but may look very different in comparison. By studying the dynamics of individual lattice site populations in ultracold bosonic gases, we show that the process of relaxation toward equilibrium in a quantum system can be orders of magnitude faster than in its classical counterpart. Classical chaos quantifiers reveal that this is due to a wave packet in a quantum system being able to escape regions of inefficient classical transport by a mechanism akin to tunneling. Since the presented phenomenon takes place in a broad parameter range and persists in weakly disordered systems, we expect that it occurs in a variety of many-body systems and is amenable to direct experimental verification in state-of-the-art quantum simulation platforms.}, archive = {J_PRL}, author = {Yulong Qiao and Frank Großmann and Peter Schlagheck and Gabriel M. Lando}, doi = {10.1103/gqgy-fjn6}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060404}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum enhancement of thermalization}, volume = {135}, year = {2025}, }
• (2025). Optimal bound on long-range distillable entanglement. PRL, 135(6), 060403. (www)

  @article{ , abstract = {We prove an upper bound on long-range distillable entanglement in spatial dimensions. Namely, it must decay faster than , where is the distance between entangled regions. For states that are asymptotically rotationally invariant, the bound is strengthened to . We then find explicit examples of quantum states with decay arbitrarily close to the bound. In one dimension, we construct free fermion Hamiltonians with nearest neighbor couplings that have these states as ground states. Curiously, states in conformal field theory are far from saturation, with distillable entanglement decaying faster than any polynomial.}, archive = {J_PRL}, author = {Jonah Kudler-Flam and Vladimir Narovlansky and Nikita Sopenko}, doi = {10.1103/d9tn-jfg1}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060403}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal bound on long-range distillable entanglement}, volume = {135}, year = {2025}, }
• (2025). Stabilizer scars. PRL, 135(6), 060402. (www)

  @article{ , abstract = {Quantum many-body scars are eigenstates in nonintegrable isolated quantum systems that defy typical thermalization paradigms, violating the eigenstate thermalization hypothesis and quantum ergodicity. We identify exact analytic scar solutions in a dimensional lattice gauge theory in a quasi-1D limit as zero-magic resource stabilizer states. Our results also highlight the importance of magic resources for gauge theory thermalization, revealing a connection between computational complexity and quantum ergodicity.}, archive = {J_PRL}, author = {Jeremy Hartse and Lukasz Fidkowski and Niklas Mueller}, doi = {10.1103/n5hb-l5p5}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060402}, shortjournal = {Phys. Rev. Lett.}, title = {Stabilizer scars}, volume = {135}, year = {2025}, }
• (2025). Critical dynamics in short-range quadratic hamiltonians. PRL, 135(6), 060401. (www)

  @article{ , abstract = {We investigate critical transport and the dynamical exponent through the spreading of an initially localized particle in quadratic Hamiltonians with short-range hopping in lattice dimension . We consider critical dynamics that emerges when the Thouless time, i.e., the saturation time of the mean-squared displacement, approaches the typical Heisenberg time. We establish a relation, linking the critical dynamical exponent to and to the spectral fractal dimension . This result has notable implications: it says that superdiffusive transport in and diffusive transport in cannot be critical in the sense defined above. Our findings clarify previous results on disordered and quasiperiodic models and, through Fibonacci potential models in two and three dimensions, provide nontrivial examples of critical dynamics in systems with and .}, archive = {J_PRL}, author = {Miroslav Hopjan and Lev Vidmar}, doi = {10.1103/5vyx-k877}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060401}, shortjournal = {Phys. Rev. Lett.}, title = {Critical dynamics in short-range quadratic hamiltonians}, volume = {135}, year = {2025}, }
• (2025). Necessary and sufficient condition for randomness certification from incompatibility. PRL, 135(6), 060201. (www)

  @article{ , abstract = {Quantum randomness can be certified from probabilistic behavior demonstrating Bell nonlocality or Einstein-Podolsky-Rosen steering, leveraging outcomes from uncharacterized devices. However, in standard spot-checking protocols, such nonlocal correlations are not always sufficient for this task, necessitating the identification of required minimum quantum resources. In this Letter, we focus on the bipartite scenario and provide the necessary and sufficient condition for nonzero certified randomness under any arbitrary but fixed input, formulated in terms of measurement incompatibility. Further, we develop practical approaches to detect it. Firstly, we show that the steering-based randomness can be certified if and only if the correlations arise from a measurement compatibility structure that is not isomorphic to a hypergraph containing a star subgraph. In such a structure, the central measurement is individually compatible with the measurements at branch sites, ruling out the possibility of certified randomness in the central measurement outcomes. Subsequently, we generalize this result to the Bell scenario, proving that the violation of any chained Bell inequality involving a finite number of inputs and outputs excludes such a compatibility structure, thereby validating all chained inequalities as credible witnesses for randomness certification. Our results point out the role of an incompatibility structure in generating random numbers, offering a way to identify minimum quantum resources for the task.}, archive = {J_PRL}, author = {Yi Li and Yu Xiang and Jordi Tura and Qiongyi He}, doi = {10.1103/zp36-2xg4}, journal = {Physical Review Letters}, month = {8}, number = {6}, pages = {060201}, shortjournal = {Phys. Rev. Lett.}, title = {Necessary and sufficient condition for randomness certification from incompatibility}, volume = {135}, year = {2025}, }
• (2025). Sliding ferroelectric control of unconventional magnetism in stacked bilayers. PRL, 135(5), 056801. (www)

  @article{ , abstract = {The control of unconventional magnetism, which displays ferromagnetismlike properties with compensated magnetization, has drawn intense attention for advancing antiferromagnetic spintronics. Here, through symmetry analysis, we propose a general stacking rule, characterized by a connection operator linking two stacked bilayers, for controlling unconventional magnetism via sliding ferroelectricity. Such a rule enables the simultaneous switching of both electric polarization and nonrelativistic spin splitting or anomalous Hall effect in altermagnets, a class of collinear unconventional magnets. By comprehensively surveying the 80 layer groups, we identify all the stacking orders that allow for such two types of simultaneous switching. Furthermore, we extend the stacking rule to collinear compensated ferrimagnets, where the opposite-spin sublattices are not connected by any symmetry operator, yet the net magnetization remains zero. Combined with first-principles calculations, we demonstrate the sliding ferroelectric control of spin polarization and anomalous Hall effect in the altermagnetic and bilayers. Our Letter provides a symmetry strategy for achieving ferroelectric control of unconventional magnetism in bilayer systems and opens avenues for exploring new types of magnetoelectric coupling.}, archive = {J_PRL}, author = {Yongqian Zhu and Mingqiang Gu and Yuntian Liu and Xiaobing Chen and Yuhui Li and Shixuan Du and Qihang Liu}, doi = {10.1103/dmzg-ck2t}, journal = {Physical Review Letters}, month = {8}, number = {5}, pages = {056801}, shortjournal = {Phys. Rev. Lett.}, title = {Sliding ferroelectric control of unconventional magnetism in stacked bilayers}, volume = {135}, year = {2025}, }
• (2025). Self-modulation instability in high power ferromagnetic resonance of BiYIG nanodisks. PRL, 135(5), 056703. (www)

  @article{ , abstract = {We study the high power ferromagnetic resonance of perpendicularly magnetized BiYIG nanodisks where the uniaxial anisotropy almost compensates for the shape anisotropy. We observe a strong saturation of the averaged magnetization upon moderately increasing the amplitude of the rf field and a broadening of the ferromagnetic resonance line toward lower and higher magnetic fields. Full micromagnetic simulations reveal that a self-modulation of the dynamic magnetization is responsible for this behavior. To get more insight into this unstable dynamics, we analyze it in terms of normal modes. The number of modes involved is found to rapidly increase above the critical threshold. Still, a normal mode model taking into account only a few of them and their mutual nonlinear couplings allows us to reproduce the observed phenomenon. The normal mode analysis and micromagnetic simulations also predict a Suhl-like instability at a larger excitation power, when it is slowly increased from low values, and bistability. Using two-tone spectroscopy, we directly measure the self-modulation spectrum and provide experimental evidence of bistable dynamics. These findings open some perspectives on using high dimensional dynamics in magnetic nanostructures for unconventional information processing.}, archive = {J_PRL}, author = {I. Ngouagnia Yemeli and S. Perna and D. Gouéré and A. Kolli and S. Sangiao and J. M. De Teresa and M. Muñoz and A. Anane and M. d’Aquino and H. Merbouche and C. Serpico and G. de Loubens}, doi = {10.1103/fh7m-4p37}, journal = {Physical Review Letters}, month = {8}, number = {5}, pages = {056703}, shortjournal = {Phys. Rev. Lett.}, title = {Self-modulation instability in high power ferromagnetic resonance of BiYIG nanodisks}, volume = {135}, year = {2025}, }
• (2025). Lippmann-schwinger approach for accurate photoelectron wave functions and angle-resolved photoemission spectra from first principles. PRL, 135(5), 056403. (www)

  @article{ , abstract = {We present a conceptually simple and technically straightforward method for calculating photoelectron wave functions that is easily integrable with standard wave-function-based density-functional-theory packages. Our method is based on the Lippmann-Schwinger equation, naturally incorporating the boundary condition that the final photoelectron state must satisfy. The calculated results are in good agreement with the measured photon-energy and polarization dependence of the angle-resolved photoemission spectroscopy (ARPES) of graphene, the photon-energy-dependent evolution of the so-called dark corridor arising from the pseudospin, and , the circular dichroism reflecting the hidden orbital polarization. Our Letter opens doors to do-it-yourself simulations of ARPES with standard density-functional-theory packages, of crucial importance in the era of “quantum materials,” whose key experimental tool is ARPES.}, archive = {J_PRL}, author = {Ji Hoon Ryoo and Cheol-Hwan Park}, doi = {10.1103/gwmm-6l57}, journal = {Physical Review Letters}, month = {8}, number = {5}, pages = {056403}, shortjournal = {Phys. Rev. Lett.}, title = {Lippmann-schwinger approach for accurate photoelectron wave functions and angle-resolved photoemission spectra from first principles}, volume = {135}, year = {2025}, }
• (2025). Electron-nucleus cross sections from transfer learning. PRL, 135(5), 052502. (www)

  @article{ , abstract = {Transfer learning allows a deep neural network (DNN) trained on one type of data to be adapted for new problems with limited information. We propose to use the transfer learning technique in physics. The DNN learns the details of one process, and after fine-tuning, it makes predictions for related processes. We consider the DNNs, trained on inclusive electron-carbon scattering data, and show that after fine-tuning, they accurately predict cross sections for electron interactions with nuclear targets ranging from helium-3 to iron.}, archive = {J_PRL}, author = {Krzysztof M. Graczyk and Beata E. Kowal and Artur M. Ankowski and Rwik Dharmapal Banerjee and Jose Luis Bonilla and Hemant Prasad and Jan T. Sobczyk}, doi = {10.1103/zxv6-22tz}, journal = {Physical Review Letters}, month = {8}, number = {5}, pages = {052502}, shortjournal = {Phys. Rev. Lett.}, title = {Electron-nucleus cross sections from transfer learning}, volume = {135}, year = {2025}, }
• (2025). Distributed quantum sensing with multimode N00N states. PRL, 135(5), 050802. (www)

  @article{ , abstract = {Distributed quantum sensing, which estimates a global parameter across distant nodes, has attracted significant interest for applications such as quantum imaging, sensor networks, and global-scale clock synchronization. states are regarded as one of the optimal quantum resources for quantum metrology, enabling the Heisenberg scaling. Recently, the concept of states has been extended to multimode states for quantum-enhanced multiple-parameter estimation. However, the application of multimode states in distributed quantum sensing remains unexplored. Here, we propose a distributed quantum sensing scheme that achieves the Heisenberg scaling using multimode states. We theoretically show that multimode states can reach the Heisenberg scaling by examining both the Cramér-Rao bound and the quantum Cramér-Rao bound. For experimental demonstration, we employ a four-mode 2002 state to estimate the average of two spatially distributed phases, achieving a 2.74 dB sensitivity enhancement over the standard quantum limit. We believe that utilizing multimode states for distributed quantum sensing offers a promising approach for developing entanglement-enhanced sensor networks.}, archive = {J_PRL}, author = {Dong-Hyun Kim and Seongjin Hong and Yong-Su Kim and Kyunghwan Oh and Su-Yong Lee and Changhyoup Lee and Hyang-Tag Lim}, doi = {10.1103/4vdx-7224}, journal = {Physical Review Letters}, month = {8}, number = {5}, pages = {050802}, shortjournal = {Phys. Rev. Lett.}, title = {Distributed quantum sensing with multimode N00N states}, volume = {135}, year = {2025}, }
• (2025). Spin liquid and superconductivity emerging from steady states and measurements. PRL, 135(5), 050403. (www)

  @article{ , abstract = {We demonstrate that, starting with a simple fermion wave function, the steady mixed state of the evolution of a class of Lindbladians, and the ensemble created by strong local measurement of fermion density without postselection can be mapped to the “Gutzwiller projected” wave functions in the doubled Hilbert space—the representation of the density matrix through the Choi-Jamiołkowski isomorphism. A Gutzwiller projection is a broadly used approach of constructing spin liquid states. For example, if one starts with a gapless free Dirac fermion pure quantum state, the constructed mixed state corresponds to an algebraic spin liquid in the doubled Hilbert space. We also predict that for some initial fermion wave function, the mixed state created following the procedure described above is expected to have a spontaneous “strong-to-weak” U(1) symmetry breaking, which corresponds to the emergence of superconductivity in the doubled Hilbert space. We also design the experimental protocol to construct the desired physics of mixed states.}, archive = {J_PRL}, author = {Kaixiang Su and Abhijat Sarma and Marcus Bintz and Thomas Kiely and Yimu Bao and Matthew P. A. Fisher and Cenke Xu}, doi = {10.1103/pjs3-14cc}, journal = {Physical Review Letters}, month = {8}, number = {5}, pages = {050403}, shortjournal = {Phys. Rev. Lett.}, title = {Spin liquid and superconductivity emerging from steady states and measurements}, volume = {135}, year = {2025}, }
• (2025). Erratum: Landau-zener-stückelberg-majorana interferometry of a single hole [Phys. rev. lett. 120, 207701 (2018)]. PRL, 135(5), 059901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 059901 (2025)}, archive = {J_PRL}, author = {Alex Bogan and Sergei Studenikin and Marek Korkusinski and Louis Gaudreau and Piotr Zawadzki and Andy S. Sachrajda and Lisa Tracy and John Reno and Terry Hargett}, doi = {10.1103/3s6k-wnvj}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {059901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Landau-zener-stückelberg-majorana interferometry of a single hole [Phys. rev. lett. 120, 207701 (2018)]}, volume = {135}, year = {2025}, }
• (2025). Adaptive node positioning in biological transport networks. PRL, 135(5), 058401. (www)

  @article{ , abstract = {Biological transport networks are highly optimized structures that ensure power-efficient distribution of fluids across various domains, including animal vasculature and plant venation. Theoretically, these networks can be described as space-embedded graphs, and rich structures that align well with observations emerge from optimizing their hydrodynamic energy dissipation. Studies on these models typically use regular grids and focus solely on edge width optimization. Here, we present a generalization of the hydrodynamic graph model that permits additional optimization of node positioning. We achieve this by defining sink regions, accounting for the energy dissipation of delivery within these areas, and optimizing by means of differentiable physics. In the context of leaf venation patterns, our method results in organic networks that adapt to irregularities of boundaries and node misalignment, as well as overall improved efficiency. We study the dependency of the emergent network structures on the capillary delivery conductivity and identify a transition in which the network collapses above a critical threshold. Our findings provide insights into the early formation of biological systems and the efficient construction of transport networks.}, archive = {J_PRL}, author = {Albert Alonso and Lars Erik J. Skjegstad and Julius B. Kirkegaard}, doi = {10.1103/6b4j-tq1n}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {058401}, shortjournal = {Phys. Rev. Lett.}, title = {Adaptive node positioning in biological transport networks}, volume = {135}, year = {2025}, }
• (2025). Resolving dual processes in complex oscillatory yielding. PRL, 135(5), 058201. (www)

  @article{ , abstract = {The complex two-step yielding observed in some soft materials under oscillatory shearing is shown to result from two independent phenomena. The first step at small deformations corresponds to elastic softening, while the larger deformation feature corresponds to yielding. This interpretation is supported by experimental recovery rheology data and the construction of a rheo-physical model. Our findings elucidate the mechanisms governing complex yielding and underscore the insight afforded by recovery experiments, which decouple the underlying physics between recoverable and unrecoverable processes.}, archive = {J_PRL}, author = {James J. Griebler and Anita S. Dobo and Elizabeth E. Miczuga and Simon A. Rogers}, doi = {10.1103/1qdd-6yby}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {058201}, shortjournal = {Phys. Rev. Lett.}, title = {Resolving dual processes in complex oscillatory yielding}, volume = {135}, year = {2025}, }
• (2025). Dissipation enables robust extensive scaling of multipartite correlations. PRL, 135(5), 057401. (www)

  @article{ , abstract = {We investigate the multipartite mutual information between discrete-state stochastic units interacting in a network that is invariant under unit permutations. We show that, when the system relaxes to fixed point attractors, multipartite correlations in the stationary state either do not scale extensively with or the extensive scaling is not robust to arbitrarily small perturbations of the system dynamics. In particular, robust extensive scaling cannot occur in thermodynamic equilibrium. In contrast, mutual information scales extensively when the system relaxes to time-dependent attractors (e.g., limit cycles), which can occur only far from equilibrium. This demonstrates the essential role of dissipation in the generation and maintenance of multipartite correlations. We illustrate our theory with the nonequilibrium Potts model.}, archive = {J_PRL}, author = {Krzysztof Ptaszyński and Massimiliano Esposito}, doi = {10.1103/j21x-hrsq}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {057401}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipation enables robust extensive scaling of multipartite correlations}, volume = {135}, year = {2025}, }
• (2025). Dissipation bounds the coherence of stochastic limit cycles. PRL, 135(5), 057101. (www)

  @article{ , abstract = {Overdamped stochastic systems maintained far from equilibrium can display sustained oscillations with fluctuations that decrease with the system size. The correlation time of such noisy limit cycles expressed in units of the cycle period is upper-bounded by the entropy produced per oscillation. We prove this constraint for first-order nonlinear systems in arbitrary dimensions perturbed by weak, uncorrelated Gaussian noise. We then extend the result to important examples of more general stochastic dynamics, including electronic and chemical clocks, illustrating the practical relevance of the dissipation-coherence bound for electronic computing and thermodynamic inference.}, archive = {J_PRL}, author = {Davide Santolin and Gianmaria Falasco}, doi = {10.1103/vfdp-sdfm}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {057101}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipation bounds the coherence of stochastic limit cycles}, volume = {135}, year = {2025}, }
• (2025). Terahertz-induced second-harmonic generation in quantum paraelectrics: Hot-phonon effect. PRL, 135(5), 056901. (www)

  @article{ , abstract = {Recent THz-pump second-harmonic-generation (SHG) probe measurements of quantum paraelectrics observed a significant long-lived nonoscillatory SHG component following an ultrafast resonant excitation of the soft mode, which was interpreted as a signature of THz-induced transient ferroelectric order. We propose that the THz-induced modulation of the SHG signal can be attributed solely to the dynamic variation of the dielectric environment associated with the lattice background, which reflects the coherent response of soft mode under THz pumping. We develop a temperature-dependent dynamic model incorporating the hot-phonon effect to simulate the soft-mode behaviors under ultrafast THz excitation. Its application to paraelectric KTaO 3 produces quantitatively most of the features exhibited in our time-resolved SHG measurements and those in existing literature, including a long-lived nonoscillatory SHG response, SHG oscillations at twice the soft-mode frequency, SHG dampings, and temperature and field-strength dependencies. We conclude that the observed THz-induced nonoscillatory SHG response in quantum paraelectrics is a consequence of the nonequilibrium hot-phonon effect, offering an alternative to its existing interpretation as a signature of transient ferroelectric order.}, archive = {J_PRL}, author = {F. Yang and X. J. Li and D. Talbayev and L. Q. Chen}, doi = {10.1103/74d5-4hsw}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056901}, shortjournal = {Phys. Rev. Lett.}, title = {Terahertz-induced second-harmonic generation in quantum paraelectrics: Hot-phonon effect}, volume = {135}, year = {2025}, }
• (2025). Approximately symmetric neural networks for quantum spin liquids. PRL, 135(5), 056702. (www)

  @article{ , abstract = {We propose and analyze a family of approximately symmetric neural networks for quantum spin liquid problems. These tailored architectures are parameter efficient, scalable, and significantly outperform existing symmetry-unaware neural network architectures. Utilizing the mixed-field toric code and PXP Rydberg Hamiltonian models, we demonstrate that our approach is competitive with state-of-the-art tensor network and quantum Monte Carlo methods. Moreover, at the largest system sizes ( for toric code, for Rydberg PXP), our method allows us to explore Hamiltonians with sign problems beyond the reach of both quantum Monte Carlo and finite-size matrix-product states. The network comprises an exactly symmetric block following a nonsymmetric block, which we argue learns a transformation of the ground state analogous to quasiadiabatic continuation. Our Letter paves the way toward investigating quantum spin liquid problems within interpretable neural network architectures.}, archive = {J_PRL}, author = {Dominik S. Kufel and Jack Kemp and DinhDuy Vu and Simon M. Linsel and Chris R. Laumann and Norman Y. Yao}, doi = {10.1103/pgnx-11ph}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056702}, shortjournal = {Phys. Rev. Lett.}, title = {Approximately symmetric neural networks for quantum spin liquids}, volume = {135}, year = {2025}, }
• (2025). Manipulation of topology by electric field in breathing kagome lattice. PRL, 135(5), 056701. (www)

  @article{ , abstract = {Magnetic kagome lattices have attracted much attention because the interplay of band topology with magnetism and electronic correlations give rise to various exotic quantum states. A common structural distortion in the kagome lattice is the breathing mode, which can significantly influence the magnetism and band characteristics. However, the control of breathing mode and the associated topological phenomena remain rarely explored. Here, we demonstrate that the coupling of breathing modes with ferroelectricity, magnetism, and band topology in the monolayer system enables electric field manipulation of topological spin structure and electronic states. The breathing mode mainly occurs in materials containing early transition metal elements and can be reversed or even suppressed via ferroelectric switching in low-barrier materials. Importantly, electric field-induced switching of the breathing mode can alter the chirality of the topological spin structure, or trigger a transition from a topological trivial insulator to a Chern insulator. This work paves the way for exploring novel physical phenomena driven by breathing mode in kagome materials.}, archive = {J_PRL}, author = {Yu Xie and Ke Ji and Jun He and Xiaofan Shen and Dinghui Wang and Junting Zhang}, doi = {10.1103/29ht-pwyt}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056701}, shortjournal = {Phys. Rev. Lett.}, title = {Manipulation of topology by electric field in breathing kagome lattice}, volume = {135}, year = {2025}, }
• (2025). Observation of antihelical edge states in acoustic metamaterials. PRL, 135(5), 056601. (www)

  @article{ , abstract = {As a hallmark of the quantum Hall effect, chiral edge modes (CEMs) counterpropagate along the two parallel edges of a ribbon structure. However, recent studies demonstrate counterintuitive anti-CEMs that copropagate along the parallel edges. Analogous to the established extension of the CEMs to helical edge modes (HEMs) in the quantum spin Hall effect, it is natural to extend the anti-CEMs to anti-HEMs, which comprise a pair of time-reversal-related anti-CEMs. In this Letter, we report the first observation of the anti-HEMs based on a bilayer model that features staggered positive and negative interlayer hoppings. Experimentally, we implement this antihelical model on an acoustic platform and provide compelling evidence for the anti-HEMs by selectively exciting different spin subspaces, along with identifying the energy-biased Dirac points in bulk spectra. Our findings may offer new insights into topological phases of matter and potentially pave the way for designing novel devices with unique edge transport properties.}, archive = {J_PRL}, author = {Tianzhi Xia and Qicheng Zhang and Chunyin Qiu}, doi = {10.1103/zc1g-p1nc}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of antihelical edge states in acoustic metamaterials}, volume = {135}, year = {2025}, }
• (2025). Impact of tiny fermi pockets with extremely high mobility on the hall anomaly in the kagome metal CsV3Sb5. PRL, 135(5), 056502. (www)

  @article{ , abstract = {The kagome metal exhibits an unusual charge-density-wave (CDW) order, where the emergence of loop current order that breaks time-reversal symmetry (TRS) has been proposed. A key feature of this CDW phase is a nonmonotonic Hall effect at low fields, often attributed to TRS breaking. However, its origin remains unclear. Here, we conduct comprehensive magnetotransport measurements on and, through mobility spectrum analysis, identify the formation of tiny Fermi pockets with extremely high mobility below the CDW transition. Furthermore, electron irradiation experiments reveal that the nonmonotonic Hall effect is significantly suppressed in samples with reduced mobility, despite no substantial change in the electronic structure. These results indicate that the nonmonotonic Hall effect originates from these tiny Fermi pockets with high mobility carriers rather than anomalous Hall mechanisms, providing new insights into understanding the Hall anomaly in this kagome system.}, archive = {J_PRL}, author = {S. Liu and M. Roppongi and M. Kimata and K. Ishihara and R. Grasset and M. Konczykowski and B. R. Ortiz and S. D. Wilson and K. Yoshimi and T. Shibauchi and K. Hashimoto}, doi = {10.1103/d4dw-2v6k}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056502}, shortjournal = {Phys. Rev. Lett.}, title = {Impact of tiny fermi pockets with extremely high mobility on the hall anomaly in the kagome metal CsV3Sb5}, volume = {135}, year = {2025}, }
• (2025). Non-abelian phases from the condensation of abelian anyons. PRL, 135(5), 056501. (www)

  @article{ , abstract = {The observed fractional quantum Hall (FQH) plateaus follow a recurring hierarchical structure that allows an understanding of complex states based on simpler ones. Condensing the elementary quasiparticles of an Abelian FQH state results in a new Abelian phase at a different filling factor, and this process can be iterated ad infinitum . We show that condensing clusters of the same quasiparticles into an Abelian state can instead realize non-Abelian FQH states. In particular, condensing quasiparticle pairs in the Laughlin state yields the anti-Pfaffian phase at half filling. We moreover show that the successive condensation of Laughlin quasiparticles produces quantum Hall states whose fillings coincide with the most prominent plateaus in the first excited Landau level of GaAs. More generally, such condensation can realize any non-Abelian FQH state that admits a parton representation. This surprising result is supported by an exact analysis of explicit wave functions, field theory arguments, conformal-field theory constructions of trial states, and numerical simulations.}, archive = {J_PRL}, author = {Misha Yutushui and Maria Hermanns and David F. Mross}, doi = {10.1103/3yvl-4hws}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056501}, shortjournal = {Phys. Rev. Lett.}, title = {Non-abelian phases from the condensation of abelian anyons}, volume = {135}, year = {2025}, }
• (2025). Efficient first-principles framework for overdamped phonon dynamics and anharmonic electron-phonon coupling in superionic materials. PRL, 135(5), 056402. (www)

  @article{ , abstract = {Relying on the anharmonic special displacement method, we introduce an ab initio quasistatic polymorphous framework to describe local disorder, anharmonicity, and electron-phonon coupling in superionic conductors. Using cubic , we show that positional polymorphism yields the breakdown of the phonon quasiparticle picture, leading to extremely overdamped anharmonic vibrations while preserving transverse acoustic phonons, consistent with experiments. We also demonstrate highly broadened electronic spectral functions with band gap openings of 1.0 eV due to polymorphism, and that anharmonic electron-phonon coupling leads to a band gap narrowing with increasing temperature. Our approach, relying on generating a handful of configurations, opens the way for efficient calculations in superionic crystals to elucidate their compelling high figure of merit.}, archive = {J_PRL}, author = {Yuxuan Wang and Marios Zacharias and Xiao Zhang and Nick Pant and Jacky Even and Pierre F. P. Poudeu and Emmanouil Kioupakis}, doi = {10.1103/kgw3-cxx8}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056402}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient first-principles framework for overdamped phonon dynamics and anharmonic electron-phonon coupling in superionic materials}, volume = {135}, year = {2025}, }
• (2025). Quasiparticle gap renormalization driven by internal and external screening in a WS2 device. PRL, 135(5), 056401. (www)

  @article{ , abstract = {The electronic band gap of a two-dimensional semiconductor within a device architecture is sensitive to variations in screening properties of adjacent materials in the device and to gate-controlled doping. Here, we employ microfocused angle-resolved photoemission spectroscopy to separate band gap renormalization effects stemming from environmental screening and electron doping during in situ gating of a single-layer device. The is supported on hexagonal boron nitride and contains a section that is exposed to vacuum and another section that is encapsulated by a graphene contact. We directly observe the doping-induced semiconductor-metal transition and band gap renormalization in the two sections of . Surprisingly, a larger band gap renormalization is observed in the vacuum-exposed section than in the graphene-encapsulated—and thus ostensibly better screened—section of the . Using calculations, we determine that intrinsic screening due to stronger doping in vacuum-exposed exceeds the external environmental screening in graphene-encapsulated .}, archive = {J_PRL}, author = {Chakradhar Sahoo and Yann in ’t Veld and Alfred J. H. Jones and Zhihao Jiang and Greta Lupi and Paulina E. Majchrzak and Kimberly Hsieh and Kenji Watanabe and Takashi Taniguchi and Philip Hofmann and Jill A. Miwa and Yong P. Chen and Malte Rösner and Søren Ulstrup}, doi = {10.1103/yllv-5zx7}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056401}, shortjournal = {Phys. Rev. Lett.}, title = {Quasiparticle gap renormalization driven by internal and external screening in a WS2 device}, volume = {135}, year = {2025}, }
• (2025). Flux-controlled two-site kitaev chain. PRL, 135(5), 056301. (www)

  @article{ , abstract = {In semiconducting-superconducting hybrid devices, Andreev bound states (ABSs) can mediate the coupling between quantum dots, allowing for the realization of artificial Kitaev chains. In order to engineer Majorana bound states (MBSs) in these systems, one must control the energy of the ABSs. In this Letter, we show how extended ABSs in a flux-tunable Josephson junction can be used to control the coupling between distant quantum dots separated by . In particular, we demonstrate that the combination of electrostatic control and phase control over the ABSs increases the parameter space in which MBSs are observed. Finally, by employing an additional spectroscopic probe in the hybrid region between the quantum dots, we gain information about the spatial distribution of the Majorana wave function in a two-site Kitaev chain.}, archive = {J_PRL}, author = {Ivan Kulesh and Sebastiaan L. D. ten Haaf and Qingzhen Wang and Vincent P. M. Sietses and Yining Zhang and Sebastiaan R. Roelofs and Christian G. Prosko and Di Xiao and Candice Thomas and Michael J. Manfra and Srijit Goswami}, doi = {10.1103/r9pv-2prs}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056301}, shortjournal = {Phys. Rev. Lett.}, title = {Flux-controlled two-site kitaev chain}, volume = {135}, year = {2025}, }
• (2025). Reversible phase transition enables rapid electrical switching in multilayer MoTe2 under cyclic strain. PRL, 135(5), 056101. (www)

  @article{ , abstract = {, a promising material for flexible electronics and straintronics, exhibits rapid strain-induced conductivity changes. However, the underlying mechanisms remain poorly understood. Here, through deep-learning molecular dynamics and density-functional theory calculations, we identify a reversible phase transition between the semiconductive phase and the semimetallic phase as the key mechanism driving this phenomenon. This transition, which is highly sensitive to the direction of applied strain, provides valuable insights for optimizing -based high-frequency nanoelectronic devices and reducing fabrication-related failures.}, archive = {J_PRL}, author = {Bolin Yang and Zhilong Peng and Cun Zhang and Yin Yao and Shaohua Chen and Huajian Gao}, doi = {10.1103/4zbf-rkbl}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056101}, shortjournal = {Phys. Rev. Lett.}, title = {Reversible phase transition enables rapid electrical switching in multilayer MoTe2 under cyclic strain}, volume = {135}, year = {2025}, }
• (2025). Spatially-resolved dynamics of the amplitude schmid-higgs mode in disordered superconductors. PRL, 135(5), 056001. (www)

  @article{ , abstract = {We investigate the spatially-resolved dynamics of the collective amplitude Schmid-Higgs (SH) mode in disordered -wave superconductors and fermionic superfluids. By analyzing the analytic structure of the zero-temperature SH susceptibility in the complex frequency plane, we find that, when the coherence length greatly exceeds the mean free path, (i) the SH response at fixed wave vectors exhibits late-time oscillations decaying as with frequency , where is the superconducting gap; (ii) subdiffusive oscillations with a dynamical exponent emerge at late times and large distances; and (iii) spatial oscillations at a fixed frequency decay exponentially, with a period that diverges as the frequency approaches from above. When the coherence length is comparable to the mean free path, additional exponentially-decaying oscillations at fixed wave vectors appear with a frequency above . Furthermore, we show that the SH mode induces an extra peak in the third-harmonic generation current at finite wave vectors. The frequency of this peak is shifted from the conventional resonance at , thereby providing an unambiguous signature of order parameter amplitude dynamics.}, archive = {J_PRL}, author = {P. A. Nosov and E. S. Andriyakhina and I. S. Burmistrov}, doi = {10.1103/x12p-q7bj}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {056001}, shortjournal = {Phys. Rev. Lett.}, title = {Spatially-resolved dynamics of the amplitude schmid-higgs mode in disordered superconductors}, volume = {135}, year = {2025}, }
• (2025). Magnetic double helix. PRL, 135(5), 055201. (www)

  @article{ , abstract = {Magnetic flux ropes, fundamental magnetohydrodynamic structures, often form braided helical configurations with net axial current, as observed in astrophysical and laboratory plasmas. However, an equilibrium model for such structures has remained elusive. We present a first-principles derivation of the braided flux ropes equilibrium by capturing the force balance of current-carrying plasma strands. This equilibrium reproduces the observed structure of the double helix nebula and provides a powerful tool for studying magnetic self-organization, plasma confinement, and astrophysical dynamics.}, archive = {J_PRL}, author = {Yang Zhang and Paul M. Bellan}, doi = {10.1103/sz9k-6l22}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {055201}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic double helix}, volume = {135}, year = {2025}, }
• (2025). Greater than 1000-fold gain in a free-electron laser driven by a laser-plasma accelerator with high reliability. PRL, 135(5), 055001. (www)

  @article{ , abstract = {Compact free-electron lasers (FELs) based on plasma-based accelerators have been envisioned for many years. While recent milestone experiments have demonstrated feasibility, further progress is needed to establish laser-plasma-accelerator-driven FELs as reliable light sources. Demonstrating both full FEL saturation and reliable operation commensurate with conventional FEL facilities is critical. We report progress on both of these fronts. FEL gain exceeding 1000 at a wavelength of 420 nm in the self-amplified spontaneous emission regime has been measured. Lower and upper bounds for the characteristic exponential gain length were measured at 16.7–22.5 cm. Additionally, reliability of the laser-plasma-accelerator-driven FEL, defined here as the percentage of shots displaying FEL gain, reached an unprecedented level of greater than 90% over the course of an hour while operating at 1 Hz repetition rate.}, archive = {J_PRL}, author = {S. K. Barber and F. Kohrell and C. E. Doss and K. Jensen and C. Berger and F. Isono and Z. Eisentraut and S. Schröder and A. J. Gonsalves and K. Nakamura and G. R. Plateau and R. A. van Mourik and M. Gracia-Linares and L. Labun and B. M. Hegelich and S. V. Milton and C. G. R. Geddes and J. Osterhoff and C. B. Schroeder and E. H. Esarey and J. van Tilborg}, doi = {10.1103/vh62-gz1p}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {055001}, shortjournal = {Phys. Rev. Lett.}, title = {Greater than 1000-fold gain in a free-electron laser driven by a laser-plasma accelerator with high reliability}, volume = {135}, year = {2025}, }
• (2025). Shape asymmetry and flexibility in active cross-stream migration in nonuniform shear. PRL, 135(5), 054001. (www)

  @article{ , abstract = {We show that activity and broken fore-aft shape symmetry enable microswimmers to cross streamlines in nonuniform shear, a key yet overlooked factor in active cross-stream migration. Using a model of flagellated microswimmers in microchannel flow, we find that hydrodynamic coupling and flagellar flexibility significantly impact migration. A simplified theory identifies key factors driving the underlying rich nonlinear dynamics. Our findings apply to dynamics and control of both living and artificial microswimmers, while the hydrodynamic framework extends to diverse shear flow scenarios.}, archive = {J_PRL}, author = {Derek C. Gomes and Tapan C. Adhyapak}, doi = {10.1103/6k4f-25hv}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {054001}, shortjournal = {Phys. Rev. Lett.}, title = {Shape asymmetry and flexibility in active cross-stream migration in nonuniform shear}, volume = {135}, year = {2025}, }
• (2025). Polarization inversion with Parity–Time-Reversal–Duality symmetric scatterers. PRL, 135(5), 053802. (www)

  @article{ , abstract = {We demonstrate, both theoretically and experimentally, that arbitrary scatterers preserving parity–time-reversal–duality ( ) symmetry inherently produce a backscattered wave whose electric field is the mirror-symmetric counterpart of the incident electric field, up to an amplitude factor, with respect to the system’s characteristic mirror plane. Specifically, we establish that a general elliptically polarized wave, when reflected from such structures, exhibits a polarization state related to the polarization ellipse of the incident wave by a parity transformation. Notably, a circularly polarized wave reflects with spin angular momentum opposite to that of the incident field, in stark contrast to reflection from conventional conducting objects. These findings enable several applications such as reflective polarizers and spin-selective devices.}, archive = {J_PRL}, author = {Roee Geva and Mário G. Silveirinha and Raphael Kastner}, doi = {10.1103/7928-bf5j}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {053802}, shortjournal = {Phys. Rev. Lett.}, title = {Polarization inversion with Parity–Time-Reversal–Duality symmetric scatterers}, volume = {135}, year = {2025}, }
• (2025). Transport measurements of majorization order for wave coherence. PRL, 135(5), 053801. (www)

  @article{ , abstract = {We investigate the majorization order for comparing wave coherence and reveal its fundamental consequences in transport measurements, including power distribution, absorption, transmission, and reflection. We prove that all these measurements preserve the majorization order under unitary control, enabling direct experimental characterization of the majorization order. Specifically, waves with lower coherence in the majorization order exhibit more restricted ranges of achievable measurement values. Our results deepen the understanding of coherence in transport phenomena.}, archive = {J_PRL}, author = {Cheng Guo and David A. B. Miller and Shanhui Fan}, doi = {10.1103/snx3-bbx1}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {053801}, shortjournal = {Phys. Rev. Lett.}, title = {Transport measurements of majorization order for wave coherence}, volume = {135}, year = {2025}, }
• (2025). Collective nuclear excitation and pulse propagation in single-mode X-ray waveguides. PRL, 135(5), 053601. (www)

  @article{ , abstract = {Waveguides offer a means to controllably couple atomic ensembles to the electromagnetic field therein. Here, we demonstrate x-ray propagation in planar thin-film waveguides coupled to Mössbauer nuclei under collective resonant excitation by short pulses of synchrotron radiation. We record x-ray photons that have been emitted into resonant modes of the waveguide. Depending on the geometry and mode of excitation, two fundamentally different signatures of the collective emission are observed, for which we present a unifying theoretical model. Our results form a new platform for waveguide quantum electrodynamics in the hard x-ray regime with the potential to provide a coherent narrow band source of x-rays on the nanometer scale.}, archive = {J_PRL}, author = {Leon M. Lohse and Petar Andrejić and Sven Velten and Malte Vassholz and Charlotte Neuhaus and Ankita Negi and Anjali Panchwanee and Ilya Sergeev and Adriana Pálffy and Tim Salditt and Ralf Röhlsberger}, doi = {10.1103/r2hf-9qn9}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {053601}, shortjournal = {Phys. Rev. Lett.}, title = {Collective nuclear excitation and pulse propagation in single-mode X-ray waveguides}, volume = {135}, year = {2025}, }
• (2025). Stabilizing open photon condensates by ghost-attractor dynamics. PRL, 135(5), 053402. (www)

  @article{ , abstract = {We study the temporal, driven-dissipative dynamics of open photon Bose-Einstein condensates (BEC) in a dye-filled microcavity, taking the condensate amplitude and the noncondensed fluctuations into account on the same footing by means of a cumulant expansion within the Lindblad formalism. The fluctuations fundamentally alter the dynamics in that the BEC always dephases to zero for a sufficiently long time. However, a ghost attractor , although outside of the physically accessible configuration space, attracts the dynamics and leads to a plateaulike stabilization of the BEC for an exponentially long time, consistent with experiments. We also show that the photon BEC and the lasing state are separated by a true phase transition, since they are characterized by different fixed points. The ghost-attractor nonequilibrium stabilization mechanism is an alternative to prethermalization and may possibly be realized on other dynamical platforms as well.}, archive = {J_PRL}, author = {Aya Abouelela and Michael Turaev and Roman Kramer and Moritz Janning and Michael Kajan and Sayak Ray and Johann Kroha}, doi = {10.1103/hcsq-dwcg}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {053402}, shortjournal = {Phys. Rev. Lett.}, title = {Stabilizing open photon condensates by ghost-attractor dynamics}, volume = {135}, year = {2025}, }
• (2025). Universal efimov scaling in the rabi-coupled few-body spectrum. PRL, 135(5), 053401. (www)

  @article{ , abstract = {We investigate the behavior of the Efimov effect—a universal quantum few-body phenomenon—in the presence of an external driving field. Specifically, we consider up to three bosonic atoms, such as , interacting with a light atom, such as , where the latter has two internal spin states that are Rabi coupled. Assuming that only the spin- light atom interacts with the bosons, we find that the Rabi drive transposes the entire Efimov spectrum such that the Efimov trimers and tetramers are centered around the Rabi-shifted two-body scattering resonance. Crucially, we show that the Rabi drive preserves the trimers’ discrete scaling symmetry, while universally shifting the Efimov three-body parameter, leading to a log-periodic modulation in the spectrum as the Rabi drive is varied. Our results suggest that Efimov physics can be conveniently explored using an applied driving field, opening up the prospect of an externally tunable three-body parameter.}, archive = {J_PRL}, author = {Anthony N. Zulli and Brendan C. Mulkerin and Meera M. Parish and Jesper Levinsen}, doi = {10.1103/yr6z-mtyq}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {053401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal efimov scaling in the rabi-coupled few-body spectrum}, volume = {135}, year = {2025}, }
• (2025). Neutralization of multiply charged ground-state ions by collective electron transfer from an environment. PRL, 135(5), 053201. (www)

  @article{ , abstract = {Highly charged cations are omnipresent species after the interaction of high-energy or high-intensity light with matter. When embedded in environments, the mechanism and outcome of the redistribution of the cation’s charge are crucial for the further fate of the whole system. Generally, ground-state cations can decay by charge transfer, proceeding radiatively, through nuclear dynamics, or by electron-transfer-mediated decay (ETMD). ETMD causes electron emission from a remote neighbor and appears ubiquitous in loosely bound systems. It remained unclear how multiply charged ions decay if conventional ETMD channels are closed. Here, we show that a yet undiscovered variant of ETMD is possible, where multiple electrons are collectively transferred. Explicitly, we observe ETMD in which two electrons from two distinct neighbors (partially) neutralize a multiply charged ion, and an electron from a fourth site is emitted. According to the established nomenclature, we suggest naming the process ETMD(4).}, archive = {J_PRL}, author = {Lutz Marder and Catmarna Küstner-Wetekam and Nils Kiefer and Johannes Viehmann and Niklas Golchert and Emilia Heikura and Florian Trinter and Denis Cubaynes and Jérôme Palaudoux and Francis Penent and Arno Ehresmann and Lorenz S. Cederbaum and Přemysl Kolorenč and Andreas Hans}, doi = {10.1103/9yd1-9gkx}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {053201}, shortjournal = {Phys. Rev. Lett.}, title = {Neutralization of multiply charged ground-state ions by collective electron transfer from an environment}, volume = {135}, year = {2025}, }
• (2025). Deviations from the porter-thomas distribution due to nonstatistical γ decay below the nd150 neutron separation threshold. PRL, 135(5), 052501. (www)

  @article{ , abstract = {We introduce a new method for the study of fluctuations of partial transition widths based on nuclear resonance fluorescence experiments with quasimonochromatic linearly polarized photon beams below particle separation thresholds. It is based on the average branching of decays of states of an even-even nucleus to the state in comparison to the ground state. Between 5 and 7 MeV, a constant average branching ratio for decays from states of 0.490(16) is observed for the nuclide . Assuming -distributed partial transition widths, this average branching ratio is related to a degree of freedom of , rejecting the validity of the Porter-Thomas distribution, requiring . The observed deviation can be explained by nonstatistical effects in the -decay behavior with contributions in the range of 9.4(10)% up to 94(10)%.}, archive = {J_PRL}, author = {O. Papst and J. Isaak and V. Werner and D. Savran and N. Pietralla and G. Battaglia and T. Beck and M. Beuschlein and S. W. Finch and U. Friman-Gayer and K. E. Ide and R. V. F. Janssens and M. D. Jones and J. Kleemann and B. Löher and M. Scheck and M. Spieker and W. Tornow and R. Zidarova and A. Zilges}, doi = {10.1103/n6zw-zhz2}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {052501}, shortjournal = {Phys. Rev. Lett.}, title = {Deviations from the porter-thomas distribution due to nonstatistical γ decay below the nd150 neutron separation threshold}, volume = {135}, year = {2025}, }
• (2025). Observation of the very rare Σ+→pμ+μ− decay. PRL, 135(5), 051801. (www)

  @article{ , abstract = {The first observation of the decay is reported with high significance using proton-proton collision data, corresponding to an integrated luminosity of , collected with the LHCb detector at a center-of-mass energy of 13 TeV. A yield of decays is obtained, where the uncertainty is statistical only. A branching fraction of is measured, where the uncertainty includes statistical and systematic sources. No evidence of resonant structures is found in the dimuon invariant-mass distribution. All results are compatible with standard model expectations. This represents the rarest decay of a baryon ever observed.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and J. Bartz and S. Bashir and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and O. Bezshyyko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and E. Bottalico and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and J. D. Brandenburg and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and L. Buonincontri and M. Burgos Marcos and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and S. Cesare and A. J. Chadwick and I. Chahrour and H. Chang and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and C. Coronel and I. Corredoira and A. Correia and G. Corti and J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and S. Faghih and L. N. Falcao and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and A. Gavrikov and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and C. Giugliano and M. A. Giza and F. C. Glaser and V. V. Gligorov and C. Göbel and L. Golinka-Bezshyyko and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and E. Govorkova and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and G. Hallett and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and A. Korchin and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and V. Kushnir and B. Kutsenko and I. Kyryllin and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and J. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and D. Liu and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and G. Loachamin Ordonez and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and D. Magdalinski and D. Maisuzenko and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and L. Moeser and R. A. Mohammed and R. D. Moise and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and V. Mytrochenko and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and E. Nekrasova and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and T. Pajero and A. Palano and M. Palutan and X. Pan and S. Panebianco and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and R. N. Pilato and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and M. Ribalda Galvez and R. Ribatti and G. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and B. Sevilla Sanjuan and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and M. Singha and N. Skidmore and T. Skwarnicki and M. W. Slater and E. Smith and K. Smith and M. Smith and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and M. Stefaniak and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and Y. T. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and U. Thoma and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and T. Tork and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and A. Upadhyay and B. Urbach and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and J. van Eldik and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and B. Vivacqua and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and A. Wang and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and T. X. Xing and A. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and R. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Z. Zhang and Y. Zhao and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and Y. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/r3v2-kmmp}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {051801}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of the very rare Σ+→pμ+μ− decay}, volume = {135}, year = {2025}, }
• (2025). Origin of quasinormal modes in semi-open systems. PRL, 135(5), 051401. (www)

  @article{ , abstract = {Astrophysical black holes are open systems which, when perturbed, radiate quasinormal modes (QNMs) to infinity. By contrast, laboratory analogs are necessarily finite sized, presenting a potential obstacle to exciting QNMs in experiments. We explore how the QNM spectrum of a toy-model black hole changes when enclosed by a partially reflecting wall with adjustable reflectivity. Our results reveal a continuous connection between the QNM spectra of open and finite-sized systems. Additionally, we demonstrate that QNMs in this setup are easily excited by incoherent background noise. This Letter opens new avenues for studying QNMs of black holes and compact objects in laboratory settings, where finite-size effects and noise are unavoidable.}, archive = {J_PRL}, author = {Leonardo Solidoro and Sam Patrick and Silke Weinfurtner and Ruth Gregory}, doi = {10.1103/7kjp-vrml}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {051401}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of quasinormal modes in semi-open systems}, volume = {135}, year = {2025}, }
• (2025). Direct constraints on strongly interacting dark matter from the james webb space telescope. PRL, 135(5), 051002. (www)

  @article{ , abstract = {Direct-detection searches for dark matter are insensitive to dark matter particles that have large interactions with ordinary matter, which are stopped in the atmosphere or the Earth’s crust before reaching terrestrial detectors. We use “dark” calibration images taken with the HgCdTe detectors in the near-infrared spectrograph (NIRSpec) on the James Webb Space Telescope (JWST) to derive novel constraints on sub-GeV dark matter candidates that scatter off electrons. We supplement the JWST analysis pipeline with additional masks to remove pixels with high-energy background events. For a 0.4% subcomponent of dark matter that interacts with an ultralight dark photon, we disfavor all previously allowed parameter space at high cross sections, and constrain some parameter regions for subcomponent fractions as low as .}, archive = {J_PRL}, author = {Peizhi Du and Rouven Essig and Bernard J. Rauscher and Hailin Xu}, doi = {10.1103/s2q8-rzb3}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {051002}, shortjournal = {Phys. Rev. Lett.}, title = {Direct constraints on strongly interacting dark matter from the james webb space telescope}, volume = {135}, year = {2025}, }
• (2025). Towards a robust model-independent test of the DAMA/LIBRA dark matter signal: ANAIS-112 results with six years of data. PRL, 135(5), 051001. (www)

  @article{ , abstract = {The nature of dark matter, which constitutes 27% of the Universe’s matter-energy content, remains one of the most challenging open questions in physics. Over the past two decades, the experiment has reported an annual modulation in the detection rate of of NaI(Tl) detectors operated at the Gran Sasso Laboratory, which the collaboration interprets as evidence of the galactic dark matter detection. However, this claim has not been independently confirmed and is refuted under certain dark matter particle and halo model scenarios. Therefore, it is crucial to perform an experiment with the same target material. The ANAIS experiment uses 112.5 kg of NaI(Tl) detectors at the Canfranc underground laboratory and it has been collecting data since August 2017 to model-independently test the result. This Letter presents the results of the annual modulation analysis corresponding to six years of ANAIS-112 data. Our results, the most sensitive to date with the same target material, NaI(Tl), are incompatible with the modulation signal at a confidence level. Such a discrepancy strongly challenges the dark matter interpretation and highlights the need to address systematic uncertainties affecting the comparison, particularly those related to the response of detectors to nuclear recoils, which may require further characterization of the DAMA crystals.}, archive = {J_PRL}, author = {Julio Amaré and Jaime Apilluelo and Susana Cebrián and David Cintas and Iván Coarasa and Eduardo García and María Martínez and Ysrael Ortigoza and Alfonso Ortiz de Solórzano and Tamara Pardo and Jorge Puimedón and María Luisa Sarsa and Carmen Seoane}, doi = {10.1103/ntnl-zrn9}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {051001}, shortjournal = {Phys. Rev. Lett.}, title = {Towards a robust model-independent test of the DAMA/LIBRA dark matter signal: ANAIS-112 results with six years of data}, volume = {135}, year = {2025}, }
• (2025). Observation of residual entanglement in entanglement purification. PRL, 135(5), 050801. (www)

  @article{ , abstract = {Entanglement purification is to distill high-quality entanglement from low-quality entanglement. Entanglement purification determines the efficiency and communication rates and plays a key role in quantum repeaters and long-distance quantum communications. Existing entanglement purification protocols and proof of principle experiments usually choose two identical input pairs. They are limited to focus on the successful purification case to obtain high-quality entangled states and discard the remained items if the purification fails. Recent entanglement purification theory [ Opt. Express 28 , 2291 (2020) ] for arbitrary nonidentical input mixed states indicated that the discarded items may have residual entanglement and can be reused to increase the yield of entanglement purification, while the successful purification may not obtain a high-quality entangled state. In this Letter, using hyperentanglement, we design and experimentally demonstrate an entanglement purification protocol with nonidentical input mixed states. For the first time, we experimentally confirm the existence of residual entanglement in different error models. Furthermore, we illustrate that successful purification may decrease the fidelity of purified entangled states. We also demonstrate the approach of optimal entanglement purification. Our proof of principle results have potential applications in future high-efficiency and long-distance quantum communication.}, archive = {J_PRL}, author = {Lan Zhou and Cen-Xiao Huang and Yu-Bo Sheng and Yu Guo and Xiao-Min Hu and Yun-Feng Huang and Chuan-Feng Li and Guang-Can Guo and Bi-Heng Liu}, doi = {10.1103/kbw2-fdqn}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050801}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of residual entanglement in entanglement purification}, volume = {135}, year = {2025}, }
• (2025). Realization of high-fidelity perfect entanglers between remote superconducting quantum processors. PRL, 135(5), 050603. (www)

  @article{ , abstract = {Superconducting qubit systems, one of the leading candidates for universal quantum computing, face scalability challenges such as frequency crowding, wiring complexity, and packaging problems. Distributed quantum computing offers a viable strategy for constructing larger quantum information processing systems. Yet, direct universal quantum gates between remote qubits—critical to distributed architectures—remain unrealized. Here, we demonstrate direct high-fidelity entangling gates between two remote superconducting quantum processors separated by a 30 cm distance, utilizing standing-wave modes in their connecting coaxial cable. We achieve cross-entropy benchmarking fidelities of and for the controlled- not and controlled- z gates, respectively, outperforming state transfer and feedback-based protocols in fidelity and efficiency. This advancement significantly enhances the prospect of universal distributed quantum information processing, which is the critical step toward future large-scale quantum systems.}, archive = {J_PRL}, author = {Juan Song and Shuang Yang and Pei Liu and Hui-Li Zhang and Guang-Ming Xue and Zhen-Yu Mi and Wen-Gang Zhang and Fei Yan and Yi-Rong Jin and Hai-Feng Yu}, doi = {10.1103/npr7-b7kq}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050603}, shortjournal = {Phys. Rev. Lett.}, title = {Realization of high-fidelity perfect entanglers between remote superconducting quantum processors}, volume = {135}, year = {2025}, }
• (2025). Direct implementation of high-fidelity three-qubit gates for superconducting processor with tunable couplers. PRL, 135(5), 050602. (www)

  @article{ , abstract = {Three-qubit gates can be constructed using combinations of single-qubit and two-qubit gates, making their independent realization unnecessary. However, direct implementation of three-qubit gates reduces the depth of quantum circuits, streamlines quantum programming, and facilitates efficient circuit optimization, thereby enhancing overall performance in quantum computation. In this work, we propose and experimentally demonstrate a high-fidelity scheme for implementing a three-qubit controlled-controlled- z ( ccz ) gate in a flip-chip superconducting quantum processor with tunable couplers. This direct ccz gate is implemented by simultaneously leveraging two tunable couplers interspersed between three qubits to enable three-qubit interactions, achieving an average final state fidelity of 97.94% and a process fidelity of 93.54%. This high fidelity cannot be achieved through a simple combination of single- and two-qubit gate sequences from processors with similar performance levels. Our experiments also verify that multilayer direct implementation of the ccz gate exhibits lower leakage compared to decomposed gate approaches. As a showcase, we utilize the ccz gate as an oracle to implement the Grover search algorithm on three qubits, demonstrating high performance with the target probability amplitude significantly enhanced after two iterations. These results highlight the advantage of our approach, and facilitate the implementation of complex quantum circuits.}, archive = {J_PRL}, author = {Hao-Tian Liu and Bing-Jie Chen and Jia-Chi Zhang and Yong-Xi Xiao and Tian-Ming Li and Kaixuan Huang and Ziting Wang and Hao Li and Kui Zhao and Yueshan Xu and Cheng-Lin Deng and Gui-Han Liang and Zheng-He Liu and Si-Yun Zhou and Cai-Ping Fang and Xiaohui Song and Zhongcheng Xiang and Dongning Zheng and Yun-Hao Shi and Kai Xu and Heng Fan}, doi = {10.1103/lvb9-pfr3}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050602}, shortjournal = {Phys. Rev. Lett.}, title = {Direct implementation of high-fidelity three-qubit gates for superconducting processor with tunable couplers}, volume = {135}, year = {2025}, }
• (2025). Efficient preparation of entangled states in cavity QED with grover’s algorithm. PRL, 135(5), 050601. (www)

  @article{ , abstract = {We propose to employ the amplification mechanism of Grover’s search algorithm to efficiently prepare entangled states of an ensemble of qubits. The conditional change of sign employed in the algorithm can be implemented by the phase shift of photons scattered on an optical cavity hosting an atomic ensemble. We show that collective Dicke states, Greenberger-Horne-Zeilinger states, and Schrödinger cat superpositions of atoms may be prepared deterministically by few ( ) photon scattering events without individual addressing of the atoms.}, archive = {J_PRL}, author = {Omar Nagib and M. Saffman and K. Mølmer}, doi = {10.1103/3fzf-wsr2}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050601}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient preparation of entangled states in cavity QED with grover’s algorithm}, volume = {135}, year = {2025}, }
• (2025). Unveiling a hidden percolation transition in monitored clifford circuits: Inroads from ZX calculus. PRL, 135(5), 050402. (www)

  @article{ , abstract = {We revisit the measurement-induced phase transition (MPT) in Clifford circuits, which are both classically simulable and exhibit critical behavior widely believed to be distinct from classical percolation theory, using ZX calculus. We analyze the MPT in a dynamical model composed of controlled not ( cnot ) gates, SWAP gates, identity gates, and Bell-pair measurements, respectively, arranged randomly in a brickwork pattern. Our circuits exhibit a transition that is seemingly distinct from classical percolation based on standard arguments, that is in line with the prevailing understanding in the field. In contrast, by employing ZX-calculus based simplification techniques, we unveil a hidden percolation transition within the circuit structure. We demonstrate that the classical percolation transition in the ZX-simplified network coincides with the MPT observed through mutual information. Our findings suggest that the MPT in Clifford circuits is, in fact, controlled by a classical percolation transition in disguise.}, archive = {J_PRL}, author = {Einat Buznach Ahituv and Jonathan Ruhman and Debanjan Chowdhury}, doi = {10.1103/mgy3-kr71}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050402}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling a hidden percolation transition in monitored clifford circuits: Inroads from ZX calculus}, volume = {135}, year = {2025}, }
• (2025). Magic resources of the heisenberg picture. PRL, 135(5), 050401. (www)

  @article{ , abstract = {We study a nonstabilizerness resource theory for operators, which is dual to that describing states. We identify that the stabilizer Rényi entropy analog in operator space is a good magic monotone satisfying the usual conditions while inheriting efficient computability properties and providing a tight lower bound to the minimum number of non-Clifford gates in a circuit. Operationally, this measure quantifies how well an operator can be approximated by one with only a few Pauli strings—analogous to how entanglement entropy relates to tensor-network truncation. A notable advantage of operator stabilizer entropies is their inherent locality, as captured by a Lieb-Robinson bound. This feature makes them particularly suited for studying local dynamical magic resource generation in many-body systems. We compute this quantity analytically in two distinct regimes. First, we show that under random evolution, operator magic typically reaches near-maximal value for all Rényi indices, and we evaluate the Page correction. Second, harnessing both dual unitarity and ZX graphical calculus, we solve the operator stabilizer entropy for interacting integrable XXZ circuit, finding that it quickly saturates to a constant value. Overall, this measure sheds light on the structural properties of many-body nonstabilizerness generation and can inspire Clifford-assisted tensor network methods.}, archive = {J_PRL}, author = {Neil Dowling and Pavel Kos and Xhek Turkeshi}, doi = {10.1103/p7xt-s9nz}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050401}, shortjournal = {Phys. Rev. Lett.}, title = {Magic resources of the heisenberg picture}, volume = {135}, year = {2025}, }
• (2025). Observation of anomalous information scrambling in a rydberg atom array. PRL, 135(5), 050201. (www)

  @article{ , abstract = {Quantum information scrambling, which describes the propagation and effective loss of local information, is crucial for understanding the dynamics of quantum many-body systems. We report the observation of anomalous information scrambling in an atomic tweezer array with dominant van der Waals interaction. We characterize information spreading by an out-of-time-order correlator and observe persistent oscillations inside a suppressed linear light cone for the initial Néel state. Such an anomalous dynamic, which differs from both generic thermal and many-body localized scenarios, originates from weak ergodicity breaking in quantum many-body scarred systems.}, archive = {J_PRL}, author = {Xinhui Liang and Zongpei Yue and Yu-Xin Chao and Zhen-Xing Hua and Yige Lin and Meng Khoon Tey and Li You}, doi = {10.1103/w1cp-l5vq}, journal = {Physical Review Letters}, month = {7}, number = {5}, pages = {050201}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of anomalous information scrambling in a rydberg atom array}, volume = {135}, year = {2025}, }
• (2025). Evolutionary benefits of fitness-dependent mutation rates. PRL, 135(4), 048402. (www)

  @article{ , abstract = {Motivated by recent observations that mutation rates can be correlated with individual fitness, we analyze an evolutionary hill-climbing model with fitness-dependent mutation rates. Our results show that a mutation rate that decreases with increasing relative fitness can greatly accelerate the accumulation of beneficial mutations. Moreover, we show that a lower mutation rate for fitter individuals can prevent “mutational meltdown” of small populations by decreasing the probability of fixation of deleterious mutations. These findings suggest potential strategies for accelerating the adaptation of populations to environmental changes.}, archive = {J_PRL}, author = {Andrew G. T. Pyo and Qiwei Yu and Julia Merkenschlager and Ned S. Wingreen}, doi = {10.1103/szpk-sx1c}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048402}, shortjournal = {Phys. Rev. Lett.}, title = {Evolutionary benefits of fitness-dependent mutation rates}, volume = {135}, year = {2025}, }
• (2025). Effective markovian dynamics method for solving non-markovian dynamics of stochastic gene expression. PRL, 135(4), 048401. (www)

  @article{ , abstract = {Experiments have shown that over 10% of proteins are degraded nonexponentially. Gene expression models for nonexponentially degraded proteins are notoriously difficult to solve since the underlying stochastic dynamics is non-Markovian. Here we develop an effective Markovian dynamics (EMD) method which converts a large class of non-Markovian models into effective Markovian ones so that they have the same mRNA and protein distributions at any fixed time. Using the EMD approach, we analytically solve some classical gene expression models with nonexponential or delayed protein decay, whose exact distributions are previously unknown and fail to be obtained using conventional queueing theory. Our theory successfully explains why nonexponentially degraded proteins on average have smaller mRNA-protein correlation than exponentially degraded proteins, and it predicts that bimodality is significantly enhanced in the presence of delayed protein degradation.}, archive = {J_PRL}, author = {Youming Li and Chen Jia}, doi = {10.1103/tksw-5gb6}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048401}, shortjournal = {Phys. Rev. Lett.}, title = {Effective markovian dynamics method for solving non-markovian dynamics of stochastic gene expression}, volume = {135}, year = {2025}, }
• (2025). Dynamics of acoustically energized active nematic droplets. PRL, 135(4), 048301. (www)

  @article{ , abstract = {In a liquid crystal, the nematic phase can coexist with the isotropic phase as a dispersion of microscopic droplets. At equilibrium, these droplets adopt a spindlelike shape, known as tactoids. We report the complex dynamic behavior of nematic tactoids externally energized by an acoustic field. When activated, these tactoids exhibit a wide range of phenomena, including stretching, bending, splitting, merging, spontaneous rotation, and locomotion. We further reveal that certain pulses of acoustic energy are able to trigger a topological transformation from a tactoid to a long-lived torus-shaped droplet with elevated elastic energy. Our findings provide insights into the behavior of acoustically energized active liquid crystals in the biphasic state and suggest an approach for the manipulation of nematic droplets.}, archive = {J_PRL}, author = {Tadej Emersic and Juan J. de Pablo and Alexey Snezhko and Andrey Sokolov}, doi = {10.1103/6l21-ycdp}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048301}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamics of acoustically energized active nematic droplets}, volume = {135}, year = {2025}, }
• (2025). Friction measurements with picoliter droplets using scanning probe microscopy. PRL, 135(4), 048203. (www)

  @article{ , abstract = {Topographical and chemical defects on solid surfaces tend to pin three-phase contact lines of moving liquid drops. Our quantitative understanding of the pinning process is, however, still poor. Here we use an atomic force microscope to slide droplets of water-glycerol mixtures over hydrophobic surfaces and measure friction forces. By using picoliter droplets, the sensitivity for detecting processes at the contact line is enhanced. We have found that only a region around the contact line contributes to friction. By imaging isolated nanospherical defects, we could quantify the force and energy dissipation when the front and rear of the droplet passes the defect and compare it to theory.}, archive = {J_PRL}, author = {Diego Cortés and Michael Kappl and Hans-Jürgen Butt and Pranav Sudersan and Tomas P. Corrales}, doi = {10.1103/s6ln-s593}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048203}, shortjournal = {Phys. Rev. Lett.}, title = {Friction measurements with picoliter droplets using scanning probe microscopy}, volume = {135}, year = {2025}, }
• (2025). Dislocation glides in granular media. PRL, 135(4), 048202. (www)

  @article{ , abstract = {Atomic crystals with dislocations deform plastically at low stresses via dislocation glide. Whether dislocation glide occurs in macroscopic frictional granular media remains unknown. We simulate structural and rheological responses of a granular crystal with an edge dislocation. We discover that dislocation glide occurs at low interparticle friction coefficients, whereas at high friction, the crystal order breaks down. When the dislocation glide occurs, the yield stress is markedly lower than in dislocation-free crystals and varies linearly with the interparticle friction coefficient. The linear dependence arises from both the elastic barrier associated with the Peierls stress and the interparticle friction slip criteria.}, archive = {J_PRL}, author = {Fumiaki Nakai and Takashi Uneyama and Yuto Sasaki and Kiwamu Yoshii and Hiroaki Katsuragi}, doi = {10.1103/7g7s-c157}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048202}, shortjournal = {Phys. Rev. Lett.}, title = {Dislocation glides in granular media}, volume = {135}, year = {2025}, }
• (2025). Revealing actual viscoelastic relaxation times in capillary breakup. PRL, 135(4), 048201. (www)

  @article{ , abstract = {We use experiments and theory to elucidate the size effect in capillary breakup rheometry, where prestretching in the viscocapillary stage causes the apparent relaxation time to be consistently smaller than the actual value. We propose a method accounting for both the experimental size and the finite extensibility of polymers to extract the actual relaxation time. A phase diagram characterizes the expected measurement variability and delineates scaling law conditions. The results refine capillary breakup rheometry for viscoelastic fluids and advance the understanding of breakup dynamics across scales.}, archive = {J_PRL}, author = {Nan Hu and Jonghyun Hwang and Tachin Ruangkriengsin and Howard A. Stone}, doi = {10.1103/2jz7-4w4k}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048201}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing actual viscoelastic relaxation times in capillary breakup}, volume = {135}, year = {2025}, }
• (2025). Topology-controlled microphase separation and interconversion of twist and writhe domains in supercoiled annealed polyelectrolytes. PRL, 135(4), 048101. (www)

  @article{ , abstract = {In closed circular ribbonlike polymers such as deoxyribonucleic acid, twist and writhe are known to be largely determined by the polymer’s bending and torsional rigidities, and they must sum to a topological constant. Using molecular simulations and an analytically solvable Landau theory, we study the interplay between ribbon topology and chemically annealed charges in a model polyelectrolyte. We show that the repulsions between like-charged acidic sites trigger phase separation and coexistence of supercoiling domains, in turn unveiling a complex phase diagram and providing a route to control the properties of deoxyribonucleic acid-based materials.}, archive = {J_PRL}, author = {Roman Staňo and Christos N. Likos and Davide Michieletto and Jan Smrek}, doi = {10.1103/7fh5-frst}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {048101}, shortjournal = {Phys. Rev. Lett.}, title = {Topology-controlled microphase separation and interconversion of twist and writhe domains in supercoiled annealed polyelectrolytes}, volume = {135}, year = {2025}, }
• (2025). Linear scaling causal discovery from high-dimensional time series by dynamical community detection. PRL, 135(4), 047401. (www)

  @article{ , abstract = {Understanding which parts of a dynamical system cause each other is extremely relevant in fundamental and applied sciences. However, inferring causal links from observational data, namely, without direct manipulations of the system, is still computationally challenging, especially if the data are high dimensional. In this Letter we introduce a framework for constructing causal graphs from high-dimensional time series, whose computational cost scales linearly with the number of variables. The approach is based on the automatic identification of dynamical communities , groups of variables which mutually influence each other and can therefore be described as a single node in a causal graph. These communities are efficiently identified by optimizing the information imbalance, a statistical quantity that assigns a weight to each putative causal variable based on its information content relative to a target variable. The communities are then ordered starting from the fully autonomous ones, whose evolution is independent from all the others, to those that are progressively dependent on other communities, building in this manner a community causal graph. We demonstrate the computational efficiency and the accuracy of our approach on discrete-time and continuous-time dynamical systems including up to 80 variables.}, archive = {J_PRL}, author = {Matteo Allione and Vittorio Del Tatto and Alessandro Laio}, doi = {10.1103/kd73-93cg}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {047401}, shortjournal = {Phys. Rev. Lett.}, title = {Linear scaling causal discovery from high-dimensional time series by dynamical community detection}, volume = {135}, year = {2025}, }
• (2025). Kardar-parisi-zhang scaling in time-crystalline matter. PRL, 135(4), 047101. (www)

  @article{ , abstract = {We discuss the universal behavior linked to the Goldstone mode associated with the spontaneous breaking of time-translation symmetry in many-body systems, in which the order parameter traces out a limit cycle. We show that this universal behavior is closely tied to Kardar-Parisi-Zhang physics, which can strongly affect the scaling properties in all dimensions. Our Letter predicts and rationalizes the emergence of Kardar-Parisi-Zhang in numerous systems such as nonreciprocal phases in active matter, active magnets, driven-dissipative quantum systems, and synchronization of oscillators.}, archive = {J_PRL}, author = {Romain Daviet and Carl Philipp Zelle and Armin Asadollahi and Sebastian Diehl}, doi = {10.1103/pbtn-wsgv}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {047101}, shortjournal = {Phys. Rev. Lett.}, title = {Kardar-parisi-zhang scaling in time-crystalline matter}, volume = {135}, year = {2025}, }
• (2025). Indirect band nature of atomically thin hexagonal boron nitride identified by resonant excitation in the deep ultraviolet regime. PRL, 135(4), 046903. (www)

  @article{ , abstract = {Atomically thin hexagonal boron nitride (h-BN), especially monolayer, has emerged as a pivotal quantum material due to its intriguing optical and light-matter-interaction properties. Nevertheless, fundamental ambiguities persist regarding its intrinsic band structure and deep-UV optical responses. Here, a multispectroscopic approach—combining near-resonance deep-UV photoluminescence, Raman spectroscopy, and reflectance contrast measurements—is employed to systematically resolve the layer-dependent optoelectronic evolution of h-BN. It is revealed that the absence of band-edge luminescence in 1–3 layers h-BN is indicative of their indirect band gap nature, thereby rectifying longstanding misinterpretations of monolayer BN as a direct band gap semiconductor. Strikingly, band-edge luminescence signals and indirect band gap absorption start to appear in 4-layer, and the luminescence intensity increases with the number of layers, suggesting that interlayer interactions and periodicity along the z axis enhance phonon-assisted indirect band gap transition, even in the 4-layer case, and furthermore indicating the formation process of flat bands at K / M valleys as the periodicity along z direction increases. Moreover, the prominent resonance Raman signals in atomically thin h-BN reveals exceptionally strong electron-phonon coupling, a critical parameter for quantum optoelectronic applications. Our findings provide definitive experimental benchmarks for the long-debated monolayer BN’s band structure.}, archive = {J_PRL}, author = {Lei Fu and Yuqing Hu and Ning Tang and Junxi Duan and Xionghui Jia and Huaiyuan Yang and Zhuoxian Li and Xiangyan Han and Guoping Li and Jianming Lu and Lun Dai and Weikun Ge and Yugui Yao and Bo Shen}, doi = {10.1103/rt4w-v9r8}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046903}, shortjournal = {Phys. Rev. Lett.}, title = {Indirect band nature of atomically thin hexagonal boron nitride identified by resonant excitation in the deep ultraviolet regime}, volume = {135}, year = {2025}, }
• (2025). Deterministic double-zero media and robust wave manipulation using a phononic weyl semimetal. PRL, 135(4), 046902. (www)

  @article{ , abstract = {Double-zero media exhibit unparalleled impedance-independent wave manipulation properties. However, their reliance on accidental degeneracy makes them fragile to disturbances in structural geometry and material parameters. Here, we propose a topological approach to address this limitation. By constructing a Weyl semimetal with uniaxial screw symmetry, which exhibits a charge-2 Weyl point at the Brillouin zone center, we propose a deterministic directional double-zero medium characterized by linear dispersion along one direction and quadratic dispersion along the perpendicular directions, leading to impedance-independent total transmission and divergent impedance mismatch along different directions. By experimentally constructing this Weyl semimetal, we have observed the existence of a charge-2 Weyl point and its unique wave manipulation capabilities as directional double-zero media, including frequency-tunable wave collimation and a configurable transition between positive and negative refraction. These findings open new pathways for realizing topology-protected metamaterials with unprecedented capabilities for bulk-wave manipulation.}, archive = {J_PRL}, author = {Changqing Xu and Jinjie Shi and Xiaozhou Liu and Ze-Guo Chen and Ying Wu and Yun Lai}, doi = {10.1103/vzp2-6gns}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046902}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic double-zero media and robust wave manipulation using a phononic weyl semimetal}, volume = {135}, year = {2025}, }
• (2025). All-optical magnetic imaging protocol to achieve angstrom-scale resolution with spin defects in van der waals materials. PRL, 135(4), 046901. (www)

  @article{ , abstract = {Magnetic imaging with ultrahigh spatial resolution is crucial to exploring the magnetic textures of emerging quantum materials. We propose a novel magnetic imaging protocol that achieves angstrom-scale resolution by combining spin defects in van der Waals materials and terahertz (THz) scattering scanning near-field optical microscopy. Spin defects in the atomic monolayer enable the probe-to-sample distance diving into angstrom range where the exchange interactions between the probe and sample spins become predominant. This exchange interaction leads to energy splitting of the probe spin in the order of meV, corresponding to THz frequencies. With THz optics and the spin-dependent fluorescence of the probe spin, the interaction energy can be resolved entirely through optical methods. Our proposed all-optical magnetic imaging protocol holds significant promise for investigating magnetic textures in condensed matter physics due to its excellent compatibility and high spatial resolution.}, archive = {J_PRL}, author = {Ning Wang and Jianming Cai and Chao Lei}, doi = {10.1103/9386-v25k}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046901}, shortjournal = {Phys. Rev. Lett.}, title = {All-optical magnetic imaging protocol to achieve angstrom-scale resolution with spin defects in van der waals materials}, volume = {135}, year = {2025}, }
• (2025). Tuning perpendicular magnetic anisotropy compatible with hybrid improper ferroelectricity via a geometrical route. PRL, 135(4), 046801. (www)

  @article{ , abstract = {Achieving effective manipulation of perpendicular magnetic anisotropy within the coupling of ferroelectricity remains an intricate challenge, yet it is crucial in the electric-field control of the excitation and propagation of magnonic spin-polarization currents. Perpendicularly magnetized structures are normally inhibited to varying degrees in a polarization switching path due to the intrinsic chemical incompatibility of electronic mechanisms for single-phase multiferroics. Here, we demonstrate a geometrically coupling strategy of oxygen octahedral distortions to regulate hybrid improper ferroelectricity and perpendicular magnetic anisotropy coupled in double-perovskite superlattice films. The geometrical ferroic mechanisms lead to a coexistence of strong ferromagnetism and room-temperature ferroelectricity, particularly with a perpendicularly magnetized structure. Based on the perturbation theory and Arrott-Noakes equation, it is revealed that such magnetic anisotropy originates from spin-orbit coupling and is regulated by the crystal-field splitting from Jahn-Teller distortion in a stable mean-field exchange model, compatible with polarization changes. Our Letter provides a geometrical route to design and regulate the coupling ferroic orders of perpendicular magnetic anisotropy and ferroelectricity.}, archive = {J_PRL}, author = {Yaoxiang Jiang and Donglai Xue and Jianguo Niu and Xiaohui Shi and Yanhui Liu and Cong Wang and Weibo Gao and Shifeng Zhao}, doi = {10.1103/q237-k8yg}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046801}, shortjournal = {Phys. Rev. Lett.}, title = {Tuning perpendicular magnetic anisotropy compatible with hybrid improper ferroelectricity via a geometrical route}, volume = {135}, year = {2025}, }
• (2025). Magnetic ni-N-ni centers in N-substituted NiO. PRL, 135(4), 046706. (www)

  @article{ , abstract = {To explore how anion substitution modifies the existing magnetism in strongly correlated oxides, we investigate local electronic states and magnetic ordering in nickel oxide (NiO) induced by substituting oxygen (O) with nitrogen (N). Each N introduces an additional N 2 p hole and modifies the magnetic moment of a neighboring nickel (Ni) cation site, as the exchange interaction between this hole and the Ni e g electrons exceeds the Ni-O-Ni superexchange interaction. This leads to the formation of Ni-N-Ni centers consisting of five spins, without perturbing the antiferromagnetic NiO lattice. These centers are studied using density functional theory and confirmed through high-resolution spectroscopy on N-substituted NiO thin films grown by molecular beam epitaxy. This type of magnetic design may enable future advances in quantum technologies based on strongly correlated materials, such as quantum sensors and spin-based qubits.}, archive = {J_PRL}, author = {Simon Godin and Ilya S. Elfimov and Fengmiao Li and Bruce A. Davidson and Ronny Sutarto and Jonathan D. Denlinger and Liu Hao Tjeng and George A. Sawatzky and Ke Zou}, doi = {10.1103/mp1d-jg6c}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046706}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic ni-N-ni centers in N-substituted NiO}, volume = {135}, year = {2025}, }
• (2025). Predicting and understanding diffusion lengths and lifetimes in solids via a many-body ab initio method: The role of coupled dynamics. PRL, 135(4), 046705. (www)

  @article{ , abstract = {We present an ab initio method of diffusion, relaxation, and dephasing processes of arbitrary observables and corresponding diffusion lengths and lifetimes in solids. The method is based on a linearized density-matrix master equation, with quantum treatment of electron scattering processes. It enables clear ab initio descriptions of long lifetimes and diffusion lengths using approximate formulas at different levels, such as Dyakonov-Perel and drift-diffusion relations for spin decay and those beyond with coupled dynamics. Our results of graphene– h -BN show that the coupling between dynamical processes can significantly affect spin diffusion and relaxation. Our method provides a transparent and powerful tool for predicting and understanding diffusion and relaxation.}, archive = {J_PRL}, author = {Junqing Xu}, doi = {10.1103/yy2w-pkww}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046705}, shortjournal = {Phys. Rev. Lett.}, title = {Predicting and understanding diffusion lengths and lifetimes in solids via a many-body ab initio method: The role of coupled dynamics}, volume = {135}, year = {2025}, }
• (2025). Spin dynamics in the dirac u(1) spin liquid YbZn2GaO5. PRL, 135(4), 046704. (www)

  @article{ , abstract = {YbZn 2 GaO 5 is a promising candidate for realizing a quantum spin liquid (QSL) state, particularly owing to its lack of significant site disorder. Pulsed-field magnetometry at 0.5 K shows magnetization saturating near 15 T, with a corrected saturation moment of 2.1 ( 1 ) μ B after subtracting the van Vleck contribution. Our zero-field μ SR measurements down to milliKelvin temperatures provide evidence for a dynamic ground state and the absence of magnetic order. To probe fluctuations in the local magnetic field at the muon site, we performed longitudinal field μ SR experiments. These results provide evidence for spin dynamics with a field dependence that is consistent with a U1A01 Dirac quantum spin liquid as a plausible description of the ground state.}, archive = {J_PRL}, author = {Hank C. H. Wu and Francis L. Pratt and Benjamin M. Huddart and Dipranjan Chatterjee and Paul A. Goddard and John Singleton and D. Prabhakaran and Stephen J. Blundell}, doi = {10.1103/l93v-f576}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046704}, shortjournal = {Phys. Rev. Lett.}, title = {Spin dynamics in the dirac u(1) spin liquid YbZn2GaO5}, volume = {135}, year = {2025}, }
• (2025). Field-induced magnon decays in dipolar quantum magnets. PRL, 135(4), 046703. (www)

  @article{ , abstract = {We investigate the spontaneous disintegration of magnons in two-dimensional ferromagnets and antiferromagnets dominated by long-range dipolar interactions. Analyzing kinematic constraints, we show that the unusual dispersion of dipolar ferromagnets in a uniform magnetic field precludes magnon decay at all fields, in sharp contrast to short-range exchange-driven magnets. However, in a staggered magnetic field, magnons can decay in both dipolar ferromagnets and antiferromagnets. Remarkably, such decays do not require a minimum threshold field, and happen over a nearly fixed fraction of the Brillouin zone in the XY limit, highlighting the significant role played by dipolar interactions. In addition, topological transitions in the decay surfaces lead to singularities in the magnon spectrum. Regularizing such singular behavior via a self-consistent approach, we make predictions for dynamical spin correlations accessible to near-term quantum simulators and sensors.}, archive = {J_PRL}, author = {Andrew D. Kim and Ahmed Khalifa and Shubhayu Chatterjee}, doi = {10.1103/2tx1-v7ml}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046703}, shortjournal = {Phys. Rev. Lett.}, title = {Field-induced magnon decays in dipolar quantum magnets}, volume = {135}, year = {2025}, }
• (2025). Microscopic origin of reduced magnetic order in a frustrated metal. PRL, 135(4), 046702. (www)

  @article{ , abstract = {Although magnetic frustration in metals provides a promising avenue for novel quantum phenomena, their microscopic interpretation is often challenging. Here, we use the face-centered cubic intermetallic as model material to show that Hamiltonians neglecting the charge degree of freedom are appropriate for frustrated metals possessing low density of states at the Fermi surface. Through neutron scattering techniques we determine matching magnetic exchange interactions in the paramagnetic and field-polarized states using an effective spin-1 Heisenberg Hamiltonian, for which we identify antiferromagnetic nearest and next-nearest-neighbor interactions and that are close to the critical ratio . The study further provides evidence that spin-wave theory fails to predict the low-energy spin dynamics in the antiferromagnetic zero-field state, which is dominated by overdamped magnetic excitations. We conclude that the low-energy fluctuations arise from quantum fluctuations, accounting for the missing moment of the strongly renormalized magnetic long-range order.}, archive = {J_PRL}, author = {X. Boraley and O. Stockert and J. Lass and R. Sibille and Ø. S. Fjellvåg and S. H. Moody and A. M. Läuchli and V. Fritsch and D. G. Mazzone}, doi = {10.1103/38ds-xjl3}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046702}, shortjournal = {Phys. Rev. Lett.}, title = {Microscopic origin of reduced magnetic order in a frustrated metal}, volume = {135}, year = {2025}, }
• (2025). Odd-parity magnetism driven by antiferromagnetic exchange. PRL, 135(4), 046701. (www)

  @article{ , abstract = {Realizing odd-parity, time-reversal-preserving, nonrelativistic spin splitting is a central goal for spintronics applications. We propose a group-theory-based microscopic framework to induce odd-parity spin splitting from coplanar antiferromagnetic (AFM) states without spin-orbit coupling (SOC). We develop phenomenological models for 421 conventional period-doubling AFM systems in nonsymmorphic space groups and construct minimal microscopic models for 119 of these. We find that these AFM states can attain three possible competing ground states. These ground states all break symmetries in addition to those broken by the usual AFM order. Specifically, they give rise to either odd-parity spin-splitting, nematic order, or scalar odd-parity order related to multiferroicity. Our microscopic theories reveal that the odd-parity spin-splitting energy scale is generically large and further reveal that the scalar odd-parity order gives a nonzero Berry curvature dipole without SOC. We identify 67 materials in the Magndata database for which our theory applies. We provide density-functional theory (DFT) calculations on Fe-based materials that reveal an h -wave spin splitting consistent with our symmetry arguments and apply our microscopic model to determine the nonrelativistic Edelstein response for CeNiAsO.}, archive = {J_PRL}, author = {Yue Yu and Magnus B. Lyngby and Tatsuya Shishidou and Mercè Roig and Andreas Kreisel and Michael Weinert and Brian M. Andersen and Daniel F. Agterberg}, doi = {10.1103/zk69-k6b2}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046701}, shortjournal = {Phys. Rev. Lett.}, title = {Odd-parity magnetism driven by antiferromagnetic exchange}, volume = {135}, year = {2025}, }
• (2025). Possible spin-triplet excitonic insulator in the ultraquantum limit of HfTe5. PRL, 135(4), 046601. (www)

  @article{ , abstract = {More than 50 years ago, excitonic insulators formed by the pairing of electrons and holes due to Coulomb interactions were first predicted [A. N. Kozlov and L. A. Maksimov, Sov. J. Exp. Theor. Phys. 21 , 790 (1965); L. V. Keldysh and Y. V. Kopaev, Sov. Phys. Solid State 6 , 2219 (1965); D. Jérome, T. M. Rice, and W. Kohn, Phys. Rev. 158 , 462 (1967) ]. Since then, excitonic insulators have been observed in various classes of materials, including quantum Hall bilayers, graphite, transition metal chalcogenides, and more recently in moiré superlattices. In these excitonic insulators, an electron and a hole with the same spin bind together, and the resulting exciton is a spin singlet. Here, we report the experimental observation of a spin-triplet excitonic insulator in the ultra-quantum limit of a three-dimensional topological material . We observe that the spin-polarized zeroth Landau bands dispersing along the field direction cross each other beyond a characteristic magnetic field in , forming the one-dimensional Weyl mode. Transport measurements reveal the emergence of a gap of about when the field surpasses a critical threshold. By performing the material-specific modeling, we identify this gap as a consequence of a spin-triplet exciton formation, where electrons and holes with opposite spin form bound states, and the translational symmetry is preserved. The system reaches charge neutrality following the gap opening, as evidenced by the zero Hall conductivity over a wide magnetic field range (10–72 T). Our finding of the spin-triplet excitonic insulator paves the way for studying novel spin transport including spin superfluidity, spin Josephson currents, and Coulomb drag of spin currents in analogy to the transport properties associated with the layer pseudospin in quantum Hall bilayers.}, archive = {J_PRL}, author = {Jinyu Liu and Varsha Subramanyan and Robert Welser and Timothy McSorley and Triet Ho and David Graf and Michael T. Pettes and Avadh Saxena and Laurel E. Winter and Shi-Zeng Lin and Luis A. Jauregui}, doi = {10.1103/bj2n-4k2w}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046601}, shortjournal = {Phys. Rev. Lett.}, title = {Possible spin-triplet excitonic insulator in the ultraquantum limit of HfTe5}, volume = {135}, year = {2025}, }
• (2025). Microscopic theory of pair density waves in spin-orbit coupled kondo lattice. PRL, 135(4), 046504. (www)

  @article{ , abstract = {We demonstrate that the discommensuration between the Fermi surfaces of a conduction sea and an underlying spin liquid provides a natural mechanism for the spontaneous formation of pair density waves. Using a recent formulation of the Kondo lattice model that incorporates a Yao Lee spin liquid proposed by the authors, we demonstrate that doping away from half filling induces finite-momentum electron-Majorana pair condensation, resulting in amplitude-modulated pair density waves (PDWs). Our approach provides a precise, analytically tractable pathway for understanding the spontaneous formation of PDWs in higher dimensions and offers a natural mechanism for PDW formation in the absence of Zeeman splitting.}, archive = {J_PRL}, author = {Aaditya Panigrahi and Alexei Tsvelik and Piers Coleman}, doi = {10.1103/pdqz-zb8k}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046504}, shortjournal = {Phys. Rev. Lett.}, title = {Microscopic theory of pair density waves in spin-orbit coupled kondo lattice}, volume = {135}, year = {2025}, }
• (2025). Approximate symmetries, insulators, and superconductivity in the continuum-model description of twisted WSe2. PRL, 135(4), 046503. (www)

  @article{ , abstract = {Motivated by the recent discovery of superconductivity in twisted bilayer , we analyze the correlated physics in this system in the framework of a continuum model for the moiré superlattice. Using the symmetries in a fine-tuned limit of the system, we identify the strong-coupling ground states and their fate when the perturbations caused by finite bandwidth, displacement field, and the phase of the intralayer potential are taken into account. We classify the superconducting instabilities and, employing a spin-fermion-like model, study the superconducting instabilities in proximity to these insulating particle-hole orders. This reveals that only a neighboring intervalley coherent phase (with zero or nonzero wave vector) is naturally consistent with the observed superconducting state, which we show to be crucially affected by the nontrivial band topology. Depending on details, the superconductor will be nodal or a chiral gapped state while further including electron-phonon coupling leads to a fully gapped, time-reversal symmetric pairing state.}, archive = {J_PRL}, author = {Maine Christos and Pietro M. Bonetti and Mathias S. Scheurer}, doi = {10.1103/7z4z-vlj8}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046503}, shortjournal = {Phys. Rev. Lett.}, title = {Approximate symmetries, insulators, and superconductivity in the continuum-model description of twisted WSe2}, volume = {135}, year = {2025}, }
• (2025). Low-rank quantics tensor train representations of feynman diagrams for multiorbital electron-phonon models. PRL, 135(4), 046502. (www)

  @article{ , abstract = {Feynman diagrams are an essential tool for simulating strongly correlated electron systems. However, stochastic quantum Monte Carlo sampling suffers from the sign problem, particularly when solving a multiorbital quantum impurity model. Recently, two approaches have been proposed for efficient numerical treatment of Feynman diagrams: tensor cross interpolation (TCI) to replace stochastic sampling and the quantics tensor train (QTT) representation for compressing space-time dependence. One of the remaining challenges is the nontrivial task of identifying low-rank structures in weak-coupling Feynman diagrams for multiorbital electron-phonon systems. In particular, the traditional TCI algorithm faces an ergodicity problem, which prevents it from fully exploring the multiorbital space. To address this, we incorporate a new algorithm called global search, which resolves this issue. By combining this approach with QTT, we uncover low-rank structures and achieve efficient numerical integration with exponential resolution in time and faster-than-power-law convergence of error relative to computational cost. Additionally, our approach does not require the division of discontinuous regions necessary in nonquantics TCI.}, archive = {J_PRL}, author = {Hirone Ishida and Natsuki Okada and Shintaro Hoshino and Hiroshi Shinaoka}, doi = {10.1103/tkcp-p5br}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046502}, shortjournal = {Phys. Rev. Lett.}, title = {Low-rank quantics tensor train representations of feynman diagrams for multiorbital electron-phonon models}, volume = {135}, year = {2025}, }
• (2025). Enhanced superconducting gap in the outer CuO2 plane of the trilayer cuprate (Hg, Re)Ba2Ca2Cu3O8+δ. PRL, 135(4), 046501. (www)

  @article{ , abstract = {We report the first observation of a momentum-resolved superconducting gap in the Hg-based trilayer cuprate, which holds the highest record of superconducting transition temperature ( ) at ambient pressure. By angle-resolved photoemission spectroscopy utilizing a microfocused beam, clear quasiparticle dispersions originating from the inner and outer planes (IP and OP, respectively) were separately identified. The magnitude of the superconducting gap for the IP was comparable to that of the Bi-based trilayer cuprate with a lower . In contrast, the superconducting gap for the OP was significantly larger than that of the Bi-based one. While strong pairing in the IP has been highlighted as the key element of trilayer cuprates, the present results suggest that the enhanced pairing energy in the OP is essential for the highest at ambient pressure realized in the Hg-based trilayer cuprate.}, archive = {J_PRL}, author = {M. Horio and M. Miyamoto and Y. Mino and S. Ishida and B. Thiagarajan and C. M. Polley and C. H. Lee and T. Nishio and H. Eisaki and I. Matsuda}, doi = {10.1103/p4c3-t34b}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046501}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced superconducting gap in the outer CuO2 plane of the trilayer cuprate (Hg, Re)Ba2Ca2Cu3O8+δ}, volume = {135}, year = {2025}, }
• (2025). Correlated ligand electrons in the transition-metal oxide SrRuO3. PRL, 135(4), 046402. (www)

  @article{ , abstract = {In transition-metal compounds, the transition-metal d electrons play an important role in their physical properties; however, the effects of the electron correlation between the ligand p electrons have not been clear yet. In this Letter, the Ru 4 d and O 2 p partial density of states (PDOS) in transition-metal oxide SrRuO 3 involving Weyl fermions are investigated by resonant photoemission spectroscopy. The observations demonstrate that the O 2 p PDOS is distorted from that predicted by first-principles calculations than the Ru 4 d PDOS. The results indicate that the electron correlation in the ligand orbitals will be important to understand the electronic structure of the p − d hybridized state in strongly correlated electron systems, even with topological states.}, archive = {J_PRL}, author = {Yuichi Seki and Yuki K. Wakabayashi and Takahito Takeda and Kohdai Inagaki and Shin-ichi Fujimori and Yukiharu Takeda and Atsushi Fujimori and Yoshitaka Taniyasu and Hideki Yamamoto and Yoshiharu Krockenberger and Masaaki Tanaka and Masaki Kobayashi}, doi = {10.1103/n9qh-6739}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046402}, shortjournal = {Phys. Rev. Lett.}, title = {Correlated ligand electrons in the transition-metal oxide SrRuO3}, volume = {135}, year = {2025}, }
• (2025). Strongly enhanced mass anisotropy in monolayer phosphorene and field tunability. PRL, 135(4), 046401. (www)

  @article{ , abstract = {Phosphorene has attracted extensive research interest due to its anisotropic properties with rich tunabilities such as strongly layer-dependent and field-tunable band gaps. Revealing how the electronic structure evolves down to monolayer is critical for understanding its anisotropic properties and field tunability. Here, we report the hitherto unexplored electronic structure of monolayer phosphorene, as well as field tunability in few-layer phosphorene. A strongly enhanced mass anisotropy is observed in monolayer phosphorene, which clearly distinguishes it from bilayer and thicker flakes. Moreover, by introducing an external electric field upon doping, modifications of the mass anisotropy and energy spacing between subbands in few-layer phosphorene are further revealed. Our work reveals the unique electronic structure of monolayer phosphorene, highlighting the critical roles of interlayer coupling as well as external electric field in tailoring the band parameters in phosphorene.}, archive = {J_PRL}, author = {Wanying Chen and Yiwen Yin and Fei Wang and Hongyun Zhang and Yixuan Ma and Kejie Bao and Haoyuan Zhong and Qian Li and Tianyun Lin and Changhua Bao and Hugen Yan and Junyi Zhu and Shuyun Zhou}, doi = {10.1103/3z9x-xpsq}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046401}, shortjournal = {Phys. Rev. Lett.}, title = {Strongly enhanced mass anisotropy in monolayer phosphorene and field tunability}, volume = {135}, year = {2025}, }
• (2025). Pressure-driven moiré potential enhancement and tertiary gap opening in graphene/h-BN heterostructure. PRL, 135(4), 046303. (www)

  @article{ , abstract = {Moiré superlattices enable engineering of correlated quantum states through tunable periodic potentials, where twist angle controls periodicity but dynamic potential strength modulation remains challenging. Here, we develop a high-pressure quantum transport technique for van der Waals heterostructures, achieving the ultimate pressure limit ( ∼ 9 GPa ) in encapsulated moiré devices. In aligned graphene/h-BN, we demonstrate that pressure induces a substantial enhancement of the moiré potential strength, evidenced by the suppression of the first valence bandwidth and the near-doubling of the primary band gap. Moreover, we report the first observation of a tertiary gap emerging above 6.4 GPa, verifying theoretical predictions. Our results establish hydrostatic pressure as a universal parameter to reshape moiré band structures. By enabling quantum transport studies at previously inaccessible pressure regimes, this Letter expands the accessible parameter space for exploring correlated phases in moiré systems.}, archive = {J_PRL}, author = {Yupeng Wang and Jiaqi An and Chunhui Ye and Xiangqi Wang and Di Mai and Hongze Zhao and Yang Zhang and Chiyu Peng and Kenji Watanabe and Takashi Taniguchi and Xiaoyu Sun and Rucheng Dai and Zhongping Wang and Wei Qin and Zhenhua Qiao and Zengming Zhang}, doi = {10.1103/xs5j-hp3p}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046303}, shortjournal = {Phys. Rev. Lett.}, title = {Pressure-driven moiré potential enhancement and tertiary gap opening in graphene/h-BN heterostructure}, volume = {135}, year = {2025}, }
• (2025). Thermodynamic uncertainty relations for coherent transport. PRL, 135(4), 046302. (www)

  @article{ , abstract = {We derive a universal thermodynamic uncertainty relation for fermionic coherent transport, which bounds the total rate of entropy production in terms of the mean and fluctuations of a single particle current. This bound holds for any multiterminal geometry and arbitrary chemical and thermal biases, as long as no external magnetic fields are applied. It can further be saturated in two-terminal settings with boxcar-shaped transmission functions and reduces to its classical counterpart in linear response. Upon insertion of a numerical factor, our bound also extends to systems with broken time-reversal symmetry. As an application, we derive trade-off relations between the figures of merit of coherent thermoelectric heat engines and refrigerators, which show that such devices can attain ideal efficiency only at vanishing mean power or diverging power fluctuations. To illustrate our results, we work out a model of a coherent conductor consisting of a chain of quantum dots.}, archive = {J_PRL}, author = {Kay Brandner and Keiji Saito}, doi = {10.1103/6nww-8wcp}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046302}, shortjournal = {Phys. Rev. Lett.}, title = {Thermodynamic uncertainty relations for coherent transport}, volume = {135}, year = {2025}, }
• (2025). Disorder-induced slow relaxation of phonon polarization. PRL, 135(4), 046301. (www)

  @article{ , abstract = {The role of the polarization degree of freedom in lattice dynamics in solids has been underlined recently. We theoretically discover a relaxation mechanism for both linear and circular polarizations of acoustic phonons. In the absence of scattering, the polarization exhibits oscillatory behavior. This behavior leads to a counterintuitive result: unlike linear momentum, more frequent scattering events cause slower polarization relaxation due to motional narrowing. We validate this mechanism using the quantum kinetic equation. We derive the relaxation rates of polarizations analytically for isotropic elastic bodies and numerically for a cubic crystal. Remarkably, we reveal that linear polarizations relax more slowly than circular ones. Our findings provide a pathway to prolong the lifetime of phonon angular momentum by designing disorder. This improvement has the potential to advance thermal management in disordered materials, facilitate phononic information transport, and strengthen spin-phonon coupling in spintronic devices.}, archive = {J_PRL}, author = {Yuta Suzuki and Shuichi Murakami}, doi = {10.1103/z8wj-f384}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046301}, shortjournal = {Phys. Rev. Lett.}, title = {Disorder-induced slow relaxation of phonon polarization}, volume = {135}, year = {2025}, }
• (2025). Emission of acoustic point sources near an interface. PRL, 135(4), 046204. (www)

  @article{ , abstract = {The emission of point sources is a cornerstone of wave-based physics, underpinning applications in optics and acoustics. While optical theories for point sources near interfaces are well established, a unified acoustic framework, modeled after its optical counterpart to provide cohesive insights into emission behaviors, remains underdeveloped. In this Letter, we extend the optical framework to acoustics, focusing on point sources near solid-fluid interfaces. Our theory predicts far-field patterns with richer features than their optical analogs, including multiple peaks and nonmonotonic supercritical emission dependence on source depth. For circularly polarized sources, we uncover depth-dependent transverse spin angular momentum in leaky Rayleigh waves, revealing opposite directions for distinct peaks. These findings shed new light on polarization related phenomena in acoustic near fields, bridging optics and acoustics while advancing the understanding of wave-matter interactions.}, archive = {J_PRL}, author = {Rong Zhou and Beibei Li and Liying Zhang and Yuecheng Shen and Hao Shen and Hongxing Xu and Deng Pan}, doi = {10.1103/dc6l-zt6w}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046204}, shortjournal = {Phys. Rev. Lett.}, title = {Emission of acoustic point sources near an interface}, volume = {135}, year = {2025}, }
• (2025). Magnetically induced topological evolutions of exceptional points in photonic bands. PRL, 135(4), 046203. (www)

  @article{ , abstract = {Exceptional points (EPs) have been widely studied in various non-Hermitian systems, exhibiting and underlying many unique topological properties. In photonic systems, multiple degrees of freedom of light enable the EPs with rich properties and high dimensional topology. In this Letter, we propose that the external magnetic field can serve as an additional parameter dimension to manipulate EPs with tunable evolutions and hidden topological structures in magneto-optical photonic crystal slabs. Continuous evolution of EPs can be derived by changing the external magnetic field, where paired EPs gradually approach each other as the Fermi arc shrinks, and eventually merge and annihilate. When considering the parameter space including the magnetic field dimension, these EPs form a closed ring, revealing novel topological structures. The discovered EP ring is further associated with more topological polarization properties, including the closed ring in Poincaré sphere and the transferred topological charge between the Fermi arc and the circularly polarized states in momentum space. Our Letter reveals complex topological properties in magneto-optical photonic crystal slabs, providing a framework to explore non-Hermitian topological systems with additional parameter dimensions.}, archive = {J_PRL}, author = {Xingqi Zhao and Jiajun Wang and Wenzhe Liu and Lei Shi and Jian Zi}, doi = {10.1103/wv2n-51qg}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046203}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetically induced topological evolutions of exceptional points in photonic bands}, volume = {135}, year = {2025}, }
• (2025). Intervalley coherent order in rhombohedral tetralayer graphene on MoS2. PRL, 135(4), 046202. (www)

  @article{ , abstract = {Multilayer rhombohedral graphene (RG) has recently emerged as a new, structurally simple flat-band system, which facilitates the exploration of interaction-driven correlation states with highly ordered electron arrangements. Despite a variety of many-body order behaviors observed in RG by transport measurements, the direct microscopic visualization of such correlated phases in real space is still lacking. Here, we show the discovery of a robust intervalley coherent order—a long-predicted ground state in RG—at 77 K in tetralayer RG placed on via imaging atomic-scale spatial reconstruction of wave functions for correlated states. This state is visualized in and filled flat bands, where clear spectroscopic signatures of electronic correlations are observed, manifesting as a reconstructed supercell on the graphene lattice. Surprisingly, such a pattern is absent in hexagonal-boron-nitride-supported RG under the same experimental conditions. These findings, together with our Hartree-Fock mean-field calculations, suggest a spin-orbit proximity-induced robust intervalley coherent phase of interacting electrons in tetralayer RG. Our results provide microscopic insights into the correlated phases in RG multilayers and highlight the significant potential for realizing highly accessible collective phenomena through van der Waals proximity.}, archive = {J_PRL}, author = {Wei-Yu Liao and Wen-Xiao Wang and Shihao Zhang and Yang Zhang and Ling-Hui Tong and Wenjia Zhang and Hao Cai and Yuan Tian and Yuanyuan Hu and Li Zhang and Lijie Zhang and Zhihui Qin and Long-Jing Yin}, doi = {10.1103/s27c-kmfs}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046202}, shortjournal = {Phys. Rev. Lett.}, title = {Intervalley coherent order in rhombohedral tetralayer graphene on MoS2}, volume = {135}, year = {2025}, }
• (2025). Superlubric motion of wavelike domain walls in sliding ferroelectrics. PRL, 135(4), 046201. (www)

  @article{ , abstract = {Sliding ferroelectrics constructed from stacked nonpolar monolayers enable out-of-plane polarization in two dimensions with exceptional properties. However, the widely accepted switching mechanism, involving synchronized long-distance in-plane translation of entire atomic layers, contradicts experimental findings. We demonstrate that this spinodal decompositionlike homogeneous switching process violates Neumann’s principle and is therefore highly improbable. Instead, polarization reversal relies on symmetry-breaking domain walls (DWs) and the tensorial nature of Born effective charges, highlighting the quantum nature of sliding ferroelectrics. We reveal that wide, wavelike DWs coherently propagate, a stark departure from the narrow DW mechanism recognized for decades. These wavelike DWs exhibit superlubric dynamics, achieving ultrahigh velocities of approximately at room temperature and displaying an anomalous cooling-promoted switching speed. The unexpected emergence of DW superlubricity presents new avenues for enhancing key performance metrics and offers exciting opportunities for applications in cryogenic environments.}, archive = {J_PRL}, author = {Changming Ke and Fucai Liu and Shi Liu}, doi = {10.1103/jhlq-2dd7}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046201}, shortjournal = {Phys. Rev. Lett.}, title = {Superlubric motion of wavelike domain walls in sliding ferroelectrics}, volume = {135}, year = {2025}, }
• (2025). Competing phases of HfO2 from unstable flat phonon bands of an unconventional high-symmetry structure. PRL, 135(4), 046101. (www)

  @article{ , abstract = {We carry out first-principles calculations to demonstrate that the complex energy landscape and competing phases of HfO 2 can be understood from the four unstable flat phonon bands of an unconventional high-symmetry structure of HfO 2 with the space group C m m a . We consider structures generated from the C m m a reference structure by all possible combinations of the zone center and zone boundary modes belonging to the unstable flat phonon branches. We find 12 distinct locally stable structures, of which 5 correspond to well-known phases. We also show that 8 of these 12 structures can be described as period-2 superlattices of the ferroelectric P c a 2 1 ( oIII ) , ferroelectric P m n 2 1 ( oIV ) , monoclinic P 2 1 / c ( m ) , and distorted monoclinic P 2 1 / c ( dm ) structures. We demonstrate how the unstable flat phonon bands can explain the atomically thin grain boundaries in the various types of superlattices. Finally, we point out that arbitrary-period HfO 2 superlattices derived from the 6 different types of period-2 superlattices are expected to form based on the flatness of the unstable phonon branches. The organizing principle provided by this work deepens our understanding of the underlying physics in the phase stability of HfO 2 and provides guidance for functional phase stabilization.}, archive = {J_PRL}, author = {Yubo Qi and Karin M. Rabe}, doi = {10.1103/9759-kp38}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046101}, shortjournal = {Phys. Rev. Lett.}, title = {Competing phases of HfO2 from unstable flat phonon bands of an unconventional high-symmetry structure}, volume = {135}, year = {2025}, }
• (2025). Circular-motion fulling-davies-unruh effect in coupled annular josephson junctions. PRL, 135(4), 046001. (www)

  @article{ , abstract = {We propose an experimentally feasible approach for observing the Fulling-Davies-Unruh effect in circular motions using a novel detector based on the thermally activated decay of metastable bunched fluxon-antifluxon pairs in coupled annular Josephson junctions. The uniform circular motion of fluxon pairs acting as detectors under relativistic velocities and small radii produces high acceleration, making an effective Unruh temperature on the order of 1 K observable with existing technologies. In addition, the newly designed detector delivers highly sensitive temperature measurements, offering a promising avenue for experimentally probing the nontrivial properties of the quantum vacuum. Numerical simulations confirm a clear acceleration-dependent temperature providing compelling evidence for the Fulling-Davies-Unruh effect.}, archive = {J_PRL}, author = {Haruna Katayama and Noriyuki Hatakenaka}, doi = {10.1103/mn34-7bj5}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {046001}, shortjournal = {Phys. Rev. Lett.}, title = {Circular-motion fulling-davies-unruh effect in coupled annular josephson junctions}, volume = {135}, year = {2025}, }
• (2025). Three-dimensional helical-rotating plasma structures in beam-generated partially magnetized plasmas. PRL, 135(4), 045301. (www)

  @article{ , abstract = {Azimuthal structures emerging in beam-generated partially magnetized plasmas are investigated using three-dimensional particle in cell-Monte Carlo collision simulations. Two distinct instability regimes are identified at low pressures. When the gas pressure is sufficiently high, quasineutrality is attained and 2D spiral-arm structures form as a result of the development of a lower-hybrid instability, resulting in enhanced cross-field transport. At lower pressures, quasineutrality is not achieved and a 3D helical-rotating plasma structure forms due to development of the diocotron instability. Analytical formulas are proposed for the critical threshold pressure between these regimes and for the rotation frequency of the helical structures. Preliminary experimental verification is provided.}, archive = {J_PRL}, author = {Jian Chen and Andrew T. Powis and Igor D. Kaganovich and Zhibin Wang and Yi Yu}, doi = {10.1103/77dq-hxtq}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {045301}, shortjournal = {Phys. Rev. Lett.}, title = {Three-dimensional helical-rotating plasma structures in beam-generated partially magnetized plasmas}, volume = {135}, year = {2025}, }
• (2025). Spin-polarized condensed plasmoids in radiation reaction dominated magnetic reconnection. PRL, 135(4), 045101. (www)

  @article{ , abstract = {Transient plasma evolution with spin polarization dynamics in radiation reaction dominated magnetic reconnection is investigated using particle-in-cell simulations. We identify a condensation of plasmoids accumulated into multiple tiny islands within the reconnection layer, where electrons are strongly polarized while emitting energetic -ray photons to undergo radiative spin flips. Nonlinear analyses elucidate that the condensation is caused by a spiral attractor appearing in the electron’s phase space due to radiation reaction. The spiral rotation and contraction of the attractor leads to the electrons’ polarization being almost instantaneously parallel with respect to the magnetic field, which results in a -ray emission with an anomalous linear polarization perpendicular to the electron’s moving plane. Our studies with around magnetic fields demonstrate that spin-polarized condensed plasmoids may be realized in extreme power laser facilities and intrinsically exist in extreme astrophysical reconnection scenarios, potentially explaining atypical polarization features in observed high-energy cosmic radiation.}, archive = {J_PRL}, author = {Zheng Gong and Karen Z. Hatsagortsyan and Christoph H. Keitel}, doi = {10.1103/c1pk-jmqr}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {045101}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-polarized condensed plasmoids in radiation reaction dominated magnetic reconnection}, volume = {135}, year = {2025}, }
• (2025). Physical interpretation of imaginary time delay. PRL, 135(4), 043801. (www)

  @article{ , abstract = {The scattering matrix linearly relates the vector of incoming waves to outgoing wave excitations, and contains an enormous amount of information about the scattering system and its connections to the scattering channels. Time delay is one way to extract information from , and the transmission time delay is a complex (even for Hermitian systems with unitary scattering matrices) measure of how long a wave excitation lingers before being transmitted. The real part of is a well-studied quantity, but the imaginary part of has not been systematically examined experimentally, and theoretical predictions for its behavior have not been tested. Here we experimentally test the predictions of Asano et al. [ Nat. Commun. 7 , 13488 (2016) ] for the imaginary part of transmission time delay in a nonunitary scattering system. We utilize Gaussian time-domain pulses scattering from a two-port microwave graph supporting a series of well-isolated absorptive modes to show that the carrier frequency of the pulses is changed in the scattering process by an amount in agreement with the imaginary part of the independently determined complex transmission time delay, from frequency-domain measurements of the subunitary matrix. Our results also generalize and extend those of Asano et al. , establishing a means to predict pulse propagation properties of non-Hermitian systems over a broad range of conditions.}, archive = {J_PRL}, author = {Isabella L. Giovannelli and Steven M. Anlage}, doi = {10.1103/nnk7-xy4v}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043801}, shortjournal = {Phys. Rev. Lett.}, title = {Physical interpretation of imaginary time delay}, volume = {135}, year = {2025}, }
• (2025). Excitonic enhancement of squeezed light in quantum-optical high-harmonic generation from a mott insulator. PRL, 135(4), 043603. (www)

  @article{ , abstract = {The strong-field induced generation of nonclassical states of light is not only a subject of fundamental research but also has potential usage in quantum information science and technology. The emerging field of strong-field quantum optics has developed ways of generating nonclassical states of light from the process of high-harmonic generation (HHG) at much wider frequency ranges and intensities than is typical for quantum optics. Here, we study the response from an exciton in a Mott-insulating system, using the extended Hubbard model. We find that the exciton plays a key role in the nonclassical response and generates squeezing at the exciton energy, showing a clear mapping between the quantum nature of the electronic system and the quantum nature of emitted radiation. We relate this nonclassical response to the nonvanishing time correlations of the current operator in the system. Our work defines a direction for experimental work to search for squeezed light from HHG in a spectrally confined region defined by the exciton energy.}, archive = {J_PRL}, author = {Christian Saugbjerg Lange and Thomas Hansen and Lars Bojer Madsen}, doi = {10.1103/wyk5-k8tk}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043603}, shortjournal = {Phys. Rev. Lett.}, title = {Excitonic enhancement of squeezed light in quantum-optical high-harmonic generation from a mott insulator}, volume = {135}, year = {2025}, }
• (2025). Lifetime-limited and tunable emission from single charge-stabilized nickel vacancy centers in diamond. PRL, 135(4), 043602. (www)

  @article{ , abstract = {The negatively charged nickel vacancy center ( ) in diamond is a promising spin qubit candidate with predicted inversion symmetry, large ground state spin-orbit splitting to limit phonon-induced decoherence, and emission in the near infrared. Here, we experimentally confirm the proposed geometric and electronic structure of the NiV defect via magneto-optical spectroscopy. We characterize the optical properties and find a Debye-Waller factor of 0.62. Additionally, we engineer charge state stabilized defects using electrical bias in planar all-diamond p-i-p junctions. We measure a vanishing static dipole moment and no spectral diffusion, characteristic of inversion symmetry. Under bias, we observe stable transitions with lifetime-limited linewidths as narrow as 16 MHz and convenient frequency tuning of the emission via a second-order Stark shift. Overall, this Letter provides a pathway toward coherent control of the and its use as a spin qubit and contributes to a more general understanding of charge dynamics experienced by defects in diamond.}, archive = {J_PRL}, author = {I. M. Morris and T. Lühmann and K. Klink and L. Crooks and D. Hardeman and D. J. Twitchen and S. Pezzagna and J. Meijer and S. S. Nicley and J. N. Becker}, doi = {10.1103/wzjx-z2h5}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043602}, shortjournal = {Phys. Rev. Lett.}, title = {Lifetime-limited and tunable emission from single charge-stabilized nickel vacancy centers in diamond}, volume = {135}, year = {2025}, }
• (2025). Coherent and incoherent light scattering by single-atom wave packets. PRL, 135(4), 043601. (www)

  @article{ , abstract = {We study light scattering of atomic wave packets in free space and discuss the results in terms of atom-photon entanglement and which-way information. Using ultracold atoms released from an optical lattice, we realize a Gedanken experiment which interferes single photons scattering off of Heisenberg uncertainty-limited wave packets. We unify the free-space and trapped-atom pictures by measuring the light scattered before and during wave packet expansion and show the coherence properties of the scattered light are independent of the presence of the trap. Therefore, recoilless scattering in a trap (Mössbauer effect), the different frequency of sidebands, and the excitation of an excited harmonic oscillator state are not essential to the question of which fraction of light scattering is coherent or incoherent. Our experiment demonstrates the potential of using atomic Mott insulators to create single-atom wave packets for fundamental studies.}, archive = {J_PRL}, author = {Vitaly Fedoseev and Hanzhen Lin (林翰桢 and Yu-Kun Lu and Yoo Kyung Lee and Jiahao Lyu and Wolfgang Ketterle}, doi = {10.1103/zwhd-1k2t}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043601}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent and incoherent light scattering by single-atom wave packets}, volume = {135}, year = {2025}, }
• (2025). Measurement of the differential static scalar polarizability of the sr+88 clock transition. PRL, 135(4), 043402. (www)

  @article{ , abstract = {We report on a precision measurement of the differential static scalar polarizability Δ α 0 of the S 2 1 / 2 → D 2 5 / 2 optical clock transition in the Sr + 88 ion. The polarizability was determined from the “magic” ion-trap drive frequency where the micromotion-induced second-order Doppler and quadratic Stark shifts cancel, using a single clock in an interleaved scheme by switching between minimized and large micromotion. By measuring at different Mathieu q z parameters, Δ α 0 can be obtained without prior knowledge of the angle between the rf electric field and the trap axis, which would otherwise dominate the systematic uncertainty. For validation, measurements were carried out at different micromotion levels and by displacing the ion in opposite directions. The results show excellent consistency and our value, Δ α 0 = − 4.8314 ( 20 ) × 10 − 40 J m 2 / V 2 = − 29.303 ( 12 ) au , reduces the uncertainty by a factor of 3.5 compared to a previous measurement, while showing a discrepancy of 5 σ . Our measurement reduces the polarizability-related uncertainty of the Sr + 88 clock to 2.2 × 10 − 19 for a blackbody radiation temperature of 295 K—a significant step towards total uncertainties < 1 × 10 − 18 . Using existing polarizability transfer schemes, the result can reduce the uncertainty also for other ion species.}, archive = {J_PRL}, author = {T. Lindvall and K. J. Hanhijärvi and T. Fordell and A. E. Wallin}, doi = {10.1103/52by-28mr}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043402}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of the differential static scalar polarizability of the sr+88 clock transition}, volume = {135}, year = {2025}, }
• (2025). Dual spectroscopy of quantum simulated fermi-hubbard systems. PRL, 135(4), 043401. (www)

  @article{ , abstract = {Quantum gas microscopy with atoms in optical lattices provides remarkable insights into the real space properties of many-body systems, but does not directly reveal the nature of their fundamental excitation spectrum. Here, we demonstrate that radio-frequency spectroscopy can reveal the quasiparticle nature of doped quantum many-body systems, crucial for our understanding of, e.g., high-temperature superconductors. In particular, we showcase how the existence and energy of magnetic polaron quasiparticles in doped Fermi-Hubbard systems may be probed, revealed by hallmark peaks in the spectroscopic spectrum. In combination with fundamental dualities of the Fermi-Hubbard model, we describe how these findings may be tested using several experimental platforms.}, archive = {J_PRL}, author = {K. Knakkergaard Nielsen and M. Zwierlein and G. M. Bruun}, doi = {10.1103/yfqr-y9ks}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043401}, shortjournal = {Phys. Rev. Lett.}, title = {Dual spectroscopy of quantum simulated fermi-hubbard systems}, volume = {135}, year = {2025}, }
• (2025). Hyperfine rovibrational states of h3+ in a weak external magnetic field. PRL, 135(4), 043003. (www)

  @article{ , abstract = {Rovibrational energies, wave functions, and Raman transition moments are reported for the lowest-energy states of the H 3 + molecular ion including the magnetic couplings of the proton spins and molecular rotation in the presence of a weak external magnetic field. The rovibrational-hyperfine-Zeeman Hamiltonian matrix is constructed and diagonalized using the rovibrational eigenstates and the proton spin functions. The developed methodology can be used to compute hyperfine-Zeeman effects also for higher-energy rovibrational excitations of H 3 + and other closed-shell polyatomic molecules. These developments will guide future experiments extending quantum logic spectroscopy to polyatomic systems.}, archive = {J_PRL}, author = {Gustavo Avila and Ayaki Sunaga and Stanislav Komorovsky and Edit Mátyus}, doi = {10.1103/lclp-852d}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043003}, shortjournal = {Phys. Rev. Lett.}, title = {Hyperfine rovibrational states of h3+ in a weak external magnetic field}, volume = {135}, year = {2025}, }
• (2025). Excited-state magnetic properties of carbon-like ca14+. PRL, 135(4), 043002. (www)

  @article{ , abstract = {We measured the g -factor of the excited-state P 1 3 in Ca 14 + ion to be g = 1.499032 ( 6 ) with a relative uncertainty of 4 × 10 − 6 . The magnetic field magnitude is derived from the Zeeman splitting of a Be + ion, cotrapped in the same linear Paul trap as the highly charged Ca 14 + ion. Furthermore, we experimentally determined the second-order Zeeman coefficient C 2 of the P 0 3 − P 1 3 clock transition. For the m J = 0 → m J ′ = 0 transition, we obtained C 2 = 0.39 ± 0.04 Hz mT − 2 , which is to our knowledge the smallest reported for any atomic transition to date. This confirms the predicted low sensitivity of highly charged ions to higher-order Zeeman effects, making them ideal candidates for high-precision optical clocks. Comparison of the experimental results with our state-of-the art electronic structure calculations shows good agreement and demonstrates the significance of the frequency-dependent Breit contribution, negative energy states, and QED effects on magnetic moments.}, archive = {J_PRL}, author = {Lukas J. Spieß and Shuying Chen and Alexander Wilzewski and Malte Wehrheim and Jan Gilles and Andrey Surzhykov and Erik Benkler and Melina Filzinger and Martin Steinel and Nils Huntemann and Charles Cheung and Sergey G. Porsev and Andrey I. Bondarev and Marianna S. Safronova and José R. Crespo López-Urrutia and Piet O. Schmidt}, doi = {10.1103/p88p-brnx}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043002}, shortjournal = {Phys. Rev. Lett.}, title = {Excited-state magnetic properties of carbon-like ca14+}, volume = {135}, year = {2025}, }
• (2025). Double spin resonance for traceable ultrasensitive atomic spin sensor. PRL, 135(4), 043001. (www)

  @article{ , abstract = {We report an ultrasensitive atomic spin sensor employing double spin resonance, achieving a spin signal enhancement of 2600 and a sensitivity of under nonzero magnetic field measurements. Furthermore, we establish an in situ alkali-noble-gas spin sensor by tracing the measured spin precession frequency to the nuclear spins gyromagnetic ratio constant with high accuracy. The dominant systematic uncertainty induced by Fermi-contact interactions during the trace process has been suppressed by more than 2 orders of magnitude via pulsed train sequences. This Letter paves the way for achieving both ultrahigh sensitivity and traceability, offering promising opportunities for exploring new physics beyond the standard model and advancing quantum metrology in complex environments.}, archive = {J_PRL}, author = {Xiaofei Huang and Weiyi Wang and Yanhui Hu and Yong-Chun Liu and Jiancheng Fang and Kai Wei}, doi = {10.1103/gy6f-4cs9}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {043001}, shortjournal = {Phys. Rev. Lett.}, title = {Double spin resonance for traceable ultrasensitive atomic spin sensor}, volume = {135}, year = {2025}, }
• (2025). Stellar weak rates of the rp-process waiting points: Effects of strong magnetic fields. PRL, 135(4), 042702. (www)

  @article{ , abstract = {Incorporating microscopic nuclear-structure information into the discussion of bulk properties of astronomical objects such as neutron stars has always been a challenging issue in interdisciplinary nuclear astrophysics. Using the r p -process nucleosynthesis as an example, we studied the effective stellar β + and electron capture (EC) rates as well as the corresponding neutrino energy-loss rates of eight waiting-point (WP) nuclei with realistic stellar conditions and presence of strong magnetic fields. The relevant nuclear transition strengths are provided by the projected shell model. We have found that, on average, due to the magnetic field effect, the stellar weak rates can increase by more than an order of magnitude for all combinations of density and temperature, as well as in each of the WPs studied. We relate the onset field strength, at which the weak rates begin to increase, to nuclear structure quantities, Q value or electronic chemical potential μ e . The enhanced weak rates may change considerably over the lifetime of WPs, thereby modifying the current understanding of the r p process.}, archive = {J_PRL}, author = {Qi-Ye Hu and Long-Jun Wang and Yang Sun}, doi = {10.1103/wg2d-fx7j}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {042702}, shortjournal = {Phys. Rev. Lett.}, title = {Stellar weak rates of the rp-process waiting points: Effects of strong magnetic fields}, volume = {135}, year = {2025}, }
• (2025). Tripling fluctuations and peaked sound speed in fermionic matter. PRL, 135(4), 042701. (www)

  @article{ , abstract = {A crossover involving three-fermion clusters is relevant to the hadron-quark crossover, which, if occurring in a neutron star, could naturally reproduce the dense-matter equation of state recently deduced from simultaneous observations of neutron-star masses and radii. To understand the crossover mechanism, we examine the role of tripling fluctuations induced by the formation of three-fermion clusters. The phase-shift representation of fluctuations manifests an interplay of bound and scattering states, leading to nonmonotonic momentum distributions of baryonlike clusters and peaked sound speed at finite densities. We demonstrate them by applying our approach to a nonrelativistic system of one-dimensional three-color fermions analogous to the hadron-quark matter.}, archive = {J_PRL}, author = {Hiroyuki Tajima and Kei Iida and Toru Kojo and Haozhao Liang}, doi = {10.1103/4ywp-752m}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {042701}, shortjournal = {Phys. Rev. Lett.}, title = {Tripling fluctuations and peaked sound speed in fermionic matter}, volume = {135}, year = {2025}, }
• (2025). Fragmentation functions of charged hadrons at next-to-next-to-leading order and constraints on the proton parton distribution functions. PRL, 135(4), 041902. (www)

  @article{ , abstract = {We present the first global analysis of fragmentation functions for light charged hadrons ( , ) at full next-to-next-to-leading order in quantum chromodynamics, incorporating world data from both single-inclusive electron-positron annihilation and semi-inclusive deep-inelastic scattering. The collinear factorization has been tested with low-momentum-transfer data and has demonstrated success at high hadron momenta. Additionally, we study the impact of current global data on hadron production to the parton distribution functions (PDFs), and find they favor a reduced asymmetry in the strange (anti)quark PDFs, as compared to the asymmetry predicted by state-of-the-art PDFs derived from inclusive data.}, archive = {J_PRL}, author = {Jun Gao and XiaoMin Shen and Hongxi Xing and Yuxiang Zhao and Bin Zhou}, doi = {10.1103/mcwy-b221}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041902}, shortjournal = {Phys. Rev. Lett.}, title = {Fragmentation functions of charged hadrons at next-to-next-to-leading order and constraints on the proton parton distribution functions}, volume = {135}, year = {2025}, }
• (2025). Search for pcc¯s(4459)0 and pcc¯s(4338)0 in ϒ(1S,2S) inclusive decays at belle. PRL, 135(4), 041901. (www)

  @article{ , abstract = {Using data samples of 102 million events and 158 million events collected by the Belle detector at the KEKB asymmetric-energy collider, we search for pentaquark states decaying to . Using the first observations of inclusive decays to , we find evidence of the state with a local significance of 3.3 standard deviations, including statistical and systematic uncertainties. We measure the mass and width of the to be and , respectively. The branching fractions for production are measured to be and . The inclusive branching fractions of are measured to be and . We measure the visible cross section for the continuum production at . In all cases, the first uncertainties are statistical and the second are systematic.}, archive = {J_PRL}, author = {The Belle and Belle II Collaborations and I. Adachi and L. Aggarwal and H. Ahmed and J. K. Ahn and H. Aihara and N. Akopov and M. Alhakami and A. Aloisio and N. Althubiti and D. M. Asner and H. Atmacan and V. Aushev and M. Aversano and R. Ayad and V. Babu and H. Bae and N. K. Baghel and S. Bahinipati and P. Bambade and Sw. Banerjee and S. Bansal and M. Barrett and M. Bartl and J. Baudot and A. Baur and A. Beaubien and F. Becherer and J. Becker and J. V. Bennett and F. U. Bernlochner and V. Bertacchi and M. Bertemes and E. Bertholet and M. Bessner and S. Bettarini and V. Bhardwaj and B. Bhuyan and F. Bianchi and D. Biswas and D. Bodrov and A. Bolz and A. Boschetti and A. Bozek and M. Bračko and P. Branchini and R. A. Briere and T. E. Browder and A. Budano and S. Bussino and Q. Campagna and M. Campajola and L. Cao and G. Casarosa and C. Cecchi and J. Cerasoli and M.-C. Chang and P. Chang and R. Cheaib and P. Cheema and B. G. Cheon and K. Chilikin and K. Chirapatpimol and H.-E. Cho and K. Cho and S.-J. Cho and S.-K. Choi and S. Choudhury and J. Cochran and L. Corona and J. X. Cui and E. De La Cruz-Burelo and S. A. De La Motte and G. De Nardo and G. De Pietro and R. de Sangro and M. Destefanis and S. Dey and R. Dhamija and F. Di Capua and J. Dingfelder and Z. Doležal and I. Domínguez Jiménez and T. V. Dong and X. Dong and D. Dossett and K. Dugic and G. Dujany and P. Ecker and J. Eppelt and P. Feichtinger and T. Ferber and T. Fillinger and C. Finck and G. Finocchiaro and F. Forti and B. G. Fulsom and A. Gabrielli and E. Ganiev and M. Garcia-Hernandez and G. Gaudino and V. Gaur and A. Gellrich and G. Ghevondyan and D. Ghosh and H. Ghumaryan and G. Giakoustidis and R. Giordano and A. Giri and P. Gironella Gironell and A. Glazov and B. Gobbo and R. Godang and P. Goldenzweig and E. Graziani and D. Greenwald and Z. Gruberová and Y. Guan and K. Gudkova and I. Haide and Y. Han and C. Harris and K. Hayasaka and H. Hayashii and S. Hazra and C. Hearty and M. T. Hedges and A. Heidelbach and I. Heredia de la Cruz and M. Hernández Villanueva and T. Higuchi and M. Hoek and M. Hohmann and R. Hoppe and P. Horak and C.-L. Hsu and T. Humair and T. Iijima and K. Inami and N. Ipsita and A. Ishikawa and R. Itoh and M. Iwasaki and P. Jackson and D. Jacobi and W. W. Jacobs and E.-J. Jang and Q. P. Ji and S. Jia and Y. Jin and A. Johnson and K. K. Joo and H. Junkerkalefeld and M. Kaleta and J. Kandra and K. H. Kang and S. Kang and G. Karyan and T. Kawasaki and F. Keil and C. Ketter and C. Kiesling and C.-H. Kim and D. Y. Kim and J.-Y. Kim and K.-H. Kim and Y.-K. Kim and H. Kindo and K. Kinoshita and P. Kodyš and T. Koga and S. Kohani and K. Kojima and A. Korobov and S. Korpar and E. Kovalenko and P. Križan and P. Krokovny and T. Kuhr and Y. Kulii and D. Kumar and R. Kumar and K. Kumara and T. Kunigo and A. Kuzmin and Y.-J. Kwon and S. Lacaprara and K. Lalwani and T. Lam and J. S. Lange and T. S. Lau and M. Laurenza and R. Leboucher and F. R. Le Diberder and M. J. Lee and C. Lemettais and P. Leo and P. M. Lewis and C. Li and L. K. Li and Q. M. Li and W. Z. Li and Y. Li and Y. B. Li and Y. P. Liao and J. Libby and J. Lin and M. H. Liu and Q. Y. Liu and Y. Liu and Z. Q. Liu and D. Liventsev and S. Longo and C. Lyu and Y. Ma and C. Madaan and M. Maggiora and S. P. Maharana and R. Maiti and G. Mancinelli and R. Manfredi and E. Manoni and M. Mantovano and D. Marcantonio and S. Marcello and C. Marinas and C. Martellini and A. Martens and A. Martini and T. Martinov and L. Massaccesi and M. Masuda and D. Matvienko and S. K. Maurya and M. Maushart and J. A. McKenna and R. Mehta and F. Meier and D. Meleshko and M. Merola and C. Miller and M. Mirra and S. Mitra and K. Miyabayashi and H. Miyake and R. Mizuk and G. B. Mohanty and S. Mondal and S. Moneta and H.-G. Moser and R. Mussa and I. Nakamura and M. Nakao and H. Nakazawa and Y. Nakazawa and M. Naruki and Z. Natkaniec and A. Natochii and M. Nayak and G. Nazaryan and M. Neu and S. Nishida and S. Ogawa and H. Ono and Y. Onuki and F. Otani and G. Pakhlova and S. Pardi and K. Parham and H. Park and J. Park and K. Park and S.-H. Park and B. Paschen and S. Patra and T. K. Pedlar and I. Peruzzi and R. Peschke and R. Pestotnik and M. Piccolo and L. E. Piilonen and P. L. M. Podesta-Lerma and T. Podobnik and S. Pokharel and C. Praz and S. Prell and E. Prencipe and M. T. Prim and H. Purwar and P. Rados and G. Raeuber and S. Raiz and N. Rauls and K. Ravindran and M. Reif and S. Reiter and M. Remnev and L. Reuter and D. Ricalde Herrmann and I. Ripp-Baudot and G. Rizzo and M. Roehrken and J. M. Roney and A. Rostomyan and N. Rout and D. A. Sanders and S. Sandilya and L. Santelj and V. Savinov and B. Scavino and J. Schmitz and S. Schneider and G. Schnell and C. Schwanda and Y. Seino and A. Selce and K. Senyo and J. Serrano and M. E. Sevior and C. Sfienti and W. Shan and C. Sharma and X. D. Shi and T. Shillington and T. Shimasaki and J.-G. Shiu and D. Shtol and A. Sibidanov and F. Simon and J. B. Singh and J. Skorupa and M. Sobotzik and A. Soffer and A. Sokolov and E. Solovieva and S. Spataro and B. Spruck and W. Song and M. Starič and P. Stavroulakis and S. Stefkova and R. Stroili and J. Strube and Y. Sue and M. Sumihama and K. Sumisawa and W. Sutcliffe and N. Suwonjandee and H. Svidras and M. Takahashi and M. Takizawa and U. Tamponi and K. Tanida and F. Tenchini and A. Thaller and O. Tittel and R. Tiwary and E. Torassa and K. Trabelsi and I. Tsaklidis and M. Uchida and I. Ueda and K. Unger and Y. Unno and K. Uno and S. Uno and J. Ur Rehman and P. Urquijo and Y. Ushiroda and S. E. Vahsen and R. van Tonder and M. Veronesi and A. Vinokurova and V. S. Vismaya and L. Vitale and V. Vobbilisetti and R. Volpe and A. Vossen and M. Wakai and S. Wallner and M.-Z. Wang and X. L. Wang and Z. Wang and A. Warburton and M. Watanabe and S. Watanuki and C. Wessel and E. Won and X. P. Xu and B. D. Yabsley and S. Yamada and S. B. Yang and J. Yelton and J. H. Yin and K. Yoshihara and C. Z. Yuan and J. Yuan and L. Zani and F. Zeng and B. Zhang and J. S. Zhou and Q. D. Zhou and L. Zhu and V. I. Zhukova and R. Žlebčík and S. Zou}, doi = {10.1103/pf8m-6j69}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041901}, shortjournal = {Phys. Rev. Lett.}, title = {Search for pcc¯s(4459)0 and pcc¯s(4338)0 in ϒ(1S,2S) inclusive decays at belle}, volume = {135}, year = {2025}, }
• (2025). Search for lepton-flavor-violating decay modes B0→KS0τ±ℓ∓ with hadronic b tagging at belle and belle II. PRL, 135(4), 041801. (www)

  @article{ , abstract = {We present the first search for the lepton-flavor-violating decay modes ( ) using the 711 and data samples recorded by the Belle and Belle II detectors, respectively. We use a hadronic -tagging technique to fully reconstruct a meson and search for signal decays in the system recoiling against the tagged meson, considering decays to either light leptons, one charged hadron, or one charged hadron and a neutral pion. We find no evidence for decays and set 90% confidence level upper limits on the branching fractions in the range of .}, archive = {J_PRL}, author = {Belle and Belle II Collaborations and I. Adachi and K. Adamczyk and L. Aggarwal and H. Ahmed and H. Aihara and N. Akopov and M. Alhakami and A. Aloisio and N. Althubiti and N. Anh Ky and D. M. Asner and H. Atmacan and V. Aushev and M. Aversano and R. Ayad and V. Babu and H. Bae and N. K. Baghel and S. Bahinipati and P. Bambade and Sw. Banerjee and S. Bansal and M. Barrett and M. Bartl and J. Baudot and A. Baur and A. Beaubien and F. Becherer and J. Becker and J. V. Bennett and F. U. Bernlochner and V. Bertacchi and M. Bertemes and E. Bertholet and M. Bessner and S. Bettarini and V. Bhardwaj and B. Bhuyan and F. Bianchi and D. Biswas and A. Bobrov and D. Bodrov and A. Bolz and A. Boschetti and A. Bozek and M. Bračko and P. Branchini and R. A. Briere and T. E. Browder and A. Budano and S. Bussino and Q. Campagna and M. Campajola and L. Cao and G. Casarosa and C. Cecchi and J. Cerasoli and M.-C. Chang and P. Chang and R. Cheaib and P. Cheema and B. G. Cheon and K. Chilikin and K. Chirapatpimol and H.-E. Cho and K. Cho and S.-J. Cho and S.-K. Choi and S. Choudhury and J. Cochran and L. Corona and J. X. Cui and E. De La Cruz-Burelo and S. A. De La Motte and G. de Marino and G. De Nardo and G. De Pietro and R. de Sangro and M. Destefanis and S. Dey and R. Dhamija and A. Di Canto and F. Di Capua and J. Dingfelder and Z. Doležal and I. Domínguez Jiménez and T. V. Dong and X. Dong and M. Dorigo and D. Dossett and S. Dubey and K. Dugic and G. Dujany and P. Ecker and P. Feichtinger and T. Ferber and T. Fillinger and C. Finck and G. Finocchiaro and A. Fodor and F. Forti and B. G. Fulsom and A. Gabrielli and E. Ganiev and M. Garcia-Hernandez and R. Garg and G. Gaudino and V. Gaur and A. Gaz and A. Gellrich and G. Ghevondyan and D. Ghosh and H. Ghumaryan and G. Giakoustidis and R. Giordano and A. Giri and P. Gironella Gironell and A. Glazov and B. Gobbo and R. Godang and O. Gogota and P. Goldenzweig and W. Gradl and S. Granderath and E. Graziani and D. Greenwald and Z. Gruberová and Y. Guan and K. Gudkova and I. Haide and Y. Han and T. Hara and C. Harris and K. Hayasaka and H. Hayashii and S. Hazra and C. Hearty and M. T. Hedges and A. Heidelbach and I. Heredia de la Cruz and M. Hernández Villanueva and T. Higuchi and M. Hoek and M. Hohmann and R. Hoppe and P. Horak and C.-L. Hsu and T. Humair and T. Iijima and K. Inami and G. Inguglia and N. Ipsita and A. Ishikawa and R. Itoh and M. Iwasaki and D. Jacobi and W. W. Jacobs and D. E. Jaffe and E.-J. Jang and Q. P. Ji and S. Jia and Y. Jin and A. Johnson and K. K. Joo and H. Junkerkalefeld and M. Kaleta and A. B. Kaliyar and J. Kandra and K. H. Kang and S. Kang and G. Karyan and T. Kawasaki and F. Keil and C. Ketter and C. Kiesling and C.-H. Kim and D. Y. Kim and J.-Y. Kim and K.-H. Kim and Y.-K. Kim and K. Kinoshita and P. Kodyš and T. Koga and S. Kohani and K. Kojima and A. Korobov and S. Korpar and E. Kovalenko and R. Kowalewski and P. Križan and P. Krokovny and T. Kuhr and Y. Kulii and D. Kumar and R. Kumar and K. Kumara and T. Kunigo and A. Kuzmin and Y.-J. Kwon and S. Lacaprara and Y.-T. Lai and K. Lalwani and T. Lam and L. Lanceri and J. S. Lange and T. S. Lau and M. Laurenza and R. Leboucher and F. R. Le Diberder and M. J. Lee and C. Lemettais and P. Leo and P. M. Lewis and C. Li and L. K. Li and Q. M. Li and W. Z. Li and Y. Li and Y. B. Li and Y. P. Liao and J. Libby and J. Lin and S. Lin and M. H. Liu and Q. Y. Liu and Y. Liu and Z. Q. Liu and D. Liventsev and S. Longo and T. Lueck and T. Luo and C. Lyu and Y. Ma and C. Madaan and M. Maggiora and S. P. Maharana and R. Maiti and G. Mancinelli and R. Manfredi and E. Manoni and M. Mantovano and S. Marcello and C. Marinas and C. Martellini and A. Martens and A. Martini and T. Martinov and L. Massaccesi and M. Masuda and D. Matvienko and S. K. Maurya and M. Maushart and J. A. McKenna and R. Mehta and F. Meier and D. Meleshko and M. Merola and C. Miller and M. Mirra and S. Mitra and K. Miyabayashi and H. Miyake and G. B. Mohanty and S. Mondal and S. Moneta and H.-G. Moser and R. Mussa and I. Nakamura and K. R. Nakamura and M. Nakao and Y. Nakazawa and M. Naruki and Z. Natkaniec and A. Natochii and M. Nayak and G. Nazaryan and M. Neu and S. Nishida and S. Ogawa and H. Ono and Y. Onuki and F. Otani and G. Pakhlova and E. Paoloni and S. Pardi and K. Parham and H. Park and J. Park and K. Park and S.-H. Park and B. Paschen and A. Passeri and S. Patra and T. K. Pedlar and I. Peruzzi and R. Peschke and R. Pestotnik and M. Piccolo and L. E. Piilonen and P. L. M. Podesta-Lerma and T. Podobnik and S. Pokharel and C. Praz and S. Prell and E. Prencipe and M. T. Prim and I. Prudiiev and H. Purwar and P. Rados and G. Raeuber and S. Raiz and N. Rauls and K. Ravindran and J. U. Rehman and M. Reif and S. Reiter and M. Remnev and L. Reuter and D. Ricalde Herrmann and I. Ripp-Baudot and G. Rizzo and S. H. Robertson and M. Roehrken and J. M. Roney and A. Rostomyan and N. Rout and D. A. Sanders and S. Sandilya and L. Santelj and V. Savinov and B. Scavino and S. Schneider and G. Schnell and C. Schwanda and Y. Seino and A. Selce and K. Senyo and J. Serrano and M. E. Sevior and C. Sfienti and W. Shan and C. Sharma and X. D. Shi and T. Shillington and T. Shimasaki and J.-G. Shiu and D. Shtol and A. Sibidanov and F. Simon and J. B. Singh and J. Skorupa and R. J. Sobie and M. Sobotzik and A. Soffer and A. Sokolov and E. Solovieva and S. Spataro and B. Spruck and W. Song and M. Starič and P. Stavroulakis and S. Stefkova and R. Stroili and J. Strube and Y. Sue and M. Sumihama and K. Sumisawa and W. Sutcliffe and N. Suwonjandee and H. Svidras and M. Takahashi and M. Takizawa and U. Tamponi and K. Tanida and F. Tenchini and A. Thaller and O. Tittel and R. Tiwary and E. Torassa and K. Trabelsi and I. Tsaklidis and I. Ueda and T. Uglov and K. Unger and Y. Unno and K. Uno and S. Uno and P. Urquijo and Y. Ushiroda and S. E. Vahsen and R. van Tonder and K. E. Varvell and M. Veronesi and A. Vinokurova and V. S. Vismaya and L. Vitale and V. Vobbilisetti and R. Volpe and M. Wakai and S. Wallner and M.-Z. Wang and Z. Wang and A. Warburton and M. Watanabe and S. Watanuki and C. Wessel and J. Wiechczynski and E. Won and X. P. Xu and B. D. Yabsley and S. Yamada and W. Yan and J. Yelton and J. H. Yin and K. Yoshihara and C. Z. Yuan and J. Yuan and L. Zani and F. Zeng and B. Zhang and J. S. Zhou and Q. D. Zhou and L. Zhu and V. I. Zhukova and R. Žlebčík}, doi = {10.1103/yzvh-v3hm}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for lepton-flavor-violating decay modes B0→KS0τ±ℓ∓ with hadronic b tagging at belle and belle II}, volume = {135}, year = {2025}, }
• (2025). Kaluza-klein AdS virasoro-shapiro amplitude near flat space. PRL, 135(4), 041603. (www)

  @article{ , abstract = {We bootstrap the first-order correction in the curvature expansion of the Virasoro-Shapiro amplitude in AdS spacetime, for arbitrary Kaluza-Klein charges of external operators. By constructing a universal ansatz based on single-valued multiple polylogarithms as well as an formalism, and matching it with the low-lying result, we derive a unified formula in terms of world-sheet integrals. Our result predicts an infinite number of Wilson coefficients that were not available in previous literature.}, archive = {J_PRL}, author = {Bo Wang (王波 and Di Wu (吴迪 and Ellis Ye Yuan (袁野}, doi = {10.1103/v72s-rv7y}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041603}, shortjournal = {Phys. Rev. Lett.}, title = {Kaluza-klein AdS virasoro-shapiro amplitude near flat space}, volume = {135}, year = {2025}, }
• (2025). First look at quartic-in-spin binary dynamics at third post-minkowskian order. PRL, 135(4), 041602. (www)

  @article{ , abstract = {We compute the conservative and radiation-reaction contributions to classical observables in the gravitational scattering between a spinning and a spinless black hole to the fourth order in spin and third order in the gravitational constant. The conservative results are obtained from two-loop amplitudes for the scattering process of a massive scalar with a massive spin- field ( , 1, 2) minimally coupled to gravity, employing the recently introduced spin interpolation method to resolve all spin-Casimir terms. The two-loop amplitude exhibits a spin-shift symmetry in both probe limits, which we conjecture to be a sign of yet unknown integrability of Kerr orbits through the quartic order in spin and to all orders in the gravitational constant. We obtain the radial action from the finite part of the amplitude and use it to compute classical observables, including the impulse and spin kick. This is done using the recently introduced covariant Dirac brackets, which allow for the computation of classical scattering observables for general (nonaligned) spin configurations. Finally, employing the radiation-reaction amplitude proposed by Alessio and Di Vecchia, together with the Dirac brackets, we obtain radiation-reaction contributions to observables at all orders in spin and beyond the aligned-spin limit. We find agreement with known results up to the quadratic order in spin for both conservative and radiation-reaction contributions. Our results advance the state of the art in the understanding of spinning binary dynamics in general relativity and demonstrate the power and simplicity of the Dirac bracket formalism for relating scattering amplitudes to classical observables.}, archive = {J_PRL}, author = {Dogan Akpinar and Fernando Febres Cordero and Manfred Kraus and Alexander Smirnov and Mao Zeng}, doi = {10.1103/c2dh-tj4v}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041602}, shortjournal = {Phys. Rev. Lett.}, title = {First look at quartic-in-spin binary dynamics at third post-minkowskian order}, volume = {135}, year = {2025}, }
• (2025). Phase transitions in an expanding medium: Hot remnants. PRL, 135(4), 041601. (www)

  @article{ , abstract = {We analyze the dynamics of a first order confinement-deconfinement phase transition in an expanding medium using an effective boundary description fitted to the holographic Witten model. We observe and analyze hot plasma remnants, which do not cool down or nucleate bubbles despite the expansion of the system. The appearance of the hot remnants, the dynamics of their shrinking, and subsequent dissolution and further heating up is very robust and persists in such diverse scenarios as boost-invariant expansion with a flat Minkowski metric and cosmological expansion in a Friedmann-Robertson-Walker spacetime.}, archive = {J_PRL}, author = {Romuald A. Janik and Matti Järvinen and Jacob Sonnenschein}, doi = {10.1103/wphs-1kfd}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041601}, shortjournal = {Phys. Rev. Lett.}, title = {Phase transitions in an expanding medium: Hot remnants}, volume = {135}, year = {2025}, }
• (2025). First search for axion dark matter with a MADMAX prototype. PRL, 135(4), 041001. (www)

  @article{ , abstract = {This Letter presents the first search for dark matter axions with mass in the ranges to and to using a prototype setup for the MAgnetized Disk and Mirror Axion eXperiment (MADMAX). The experimental setup employs a dielectric haloscope consisting of three sapphire disks and a mirror to resonantly enhance the axion-induced microwave signal within the magnetic dipole field provided by the 1.6 T Morpurgo magnet at CERN. Over 14.5 days of data collection, no axion signal was detected. A 95% CL upper limit on the axion-photon coupling strength down to is set in the targeted mass ranges, surpassing previous constraints, assuming a local axion dark matter density of . This study marks the first axion dark matter search using a dielectric haloscope.}, archive = {J_PRL}, author = {MADMAX Collaboration and B. Ary dos Santos Garcia and D. Bergermann and A. Caldwell and V. Dabhi and C. Diaconu and J. Diehl and G. Dvali and J. Egge and E. Garutti and S. Heyminck and F. Hubaut and A. Ivanov and J. Jochum and S. Knirck and M. Kramer and D. Kreikemeyer-Lorenzo and C. Krieger and C. Lee and D. Leppla-Weber and X. Li and A. Lindner and B. Majorovits and J. P. A. Maldonado and A. Martini and A. Miyazaki and E. Öz and P. Pralavorio and G. Raffelt and J. Redondo and A. Ringwald and J. Schaffran and A. Schmidt and F. Steffen and C. Strandhagen and I. Usherov and H. Wang and G. Wieching}, doi = {10.1103/c749-419q}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {041001}, shortjournal = {Phys. Rev. Lett.}, title = {First search for axion dark matter with a MADMAX prototype}, volume = {135}, year = {2025}, }
• (2025). Enhancing dynamic range of sub-standard-quantum-limit measurements via quantum deamplification. PRL, 135(4), 040801. (www)

  @article{ , abstract = {Balancing high sensitivity with a broad dynamic range is a fundamental challenge in measurement science, as improving one often compromises the other. While traditional quantum metrology has prioritized enhancing local sensitivity, a large dynamic range is crucial for applications such as atomic clocks, where extended phase interrogation times contribute to wider phase range. In this Letter, we introduce a novel quantum deamplification mechanism that extends dynamic range at a minimal cost of sensitivity. Our approach uses two sequential spin-squeezing operations to generate and detect an entangled probe state, respectively. We demonstrate that the optimal quantum interferometer limit can be approached through two-axis countertwisting dynamics. Further expansion of dynamic range is possible by using sequential quantum deamplification interspersed with phase encoding processes. Additionally, we show that robustness against detection noise can be enhanced by a hybrid sensing scheme that combines quantum deamplification with quantum amplification. Our protocol is within the reach of state-of-the-art atomic-molecular-optical platforms, offering a scalable, noise-resilient pathway for entanglement-enhanced metrology.}, archive = {J_PRL}, author = {Qi Liu and Ming Xue and Matthew Radzihovsky and Xinwei Li and Denis V. Vasilyev and Ling-Na Wu and Vladan Vuletić}, doi = {10.1103/25ds-9724}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040801}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing dynamic range of sub-standard-quantum-limit measurements via quantum deamplification}, volume = {135}, year = {2025}, }
• (2025). Scalable parameter design for superconducting quantum circuits with graph neural networks. PRL, 135(4), 040601. (www)

  @article{ , abstract = {To demonstrate supremacy of quantum computing, increasingly large-scale superconducting quantum computing chips are being designed and fabricated. However, the complexity of simulating quantum systems poses a significant challenge to computer-aided design of quantum chips, especially for large-scale chips. Harnessing the scalability of graph neural networks (GNNs), we here propose a parameter designing algorithm for large-scale superconducting quantum circuits. The algorithm depends on the so-called “three-stair scaling” mechanism, which comprises two neural-network models: an evaluator supervisedly trained on small-scale circuits for applying to medium-scale circuits, and a designer unsupervisedly trained on medium-scale circuits for applying to large-scale ones. We demonstrate our algorithm in mitigating quantum crosstalk errors. Frequencies for both single- and two-qubit gates (corresponding to the parameters of nodes and edges) are considered simultaneously. Numerical results indicate that the well-trained designer achieves notable advantages in efficiency, effectiveness, and scalability. For example, for large-scale superconducting quantum circuits consisting of around 870 qubits, our GNNs-based algorithm achieves 51% of the errors produced by the state-of-the-art algorithm, with a time reduction from 90 min to 27 s. Overall, a better-performing and more scalable algorithm for designing parameters of superconducting quantum chips is proposed, which demonstrates the advantages of applying GNNs in superconducting quantum chips.}, archive = {J_PRL}, author = {Hao Ai and Yu-xi Liu}, doi = {10.1103/yr9d-7z8k}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040601}, shortjournal = {Phys. Rev. Lett.}, title = {Scalable parameter design for superconducting quantum circuits with graph neural networks}, volume = {135}, year = {2025}, }
• (2025). Quantum mpemba effect in random circuits. PRL, 135(4), 040403. (www)

  @article{ , abstract = {The essence of the Mpemba effect is that nonequilibrium systems may relax faster the further they are from their equilibrium configuration. In the quantum realm, this phenomenon arises in closed systems dynamics and is witnessed by features of symmetry and entanglement. Here, we study the quantum Mpemba effect in charge-preserving random circuits, combining extensive numerical simulations and analytical arguments. We show that the more asymmetric certain classes of initial states (tilted ferromagnets) are, the faster they restore symmetry and reach the grand-canonical ensemble. Conversely, other classes of states (tilted antiferromagnets) do not show the Mpemba effect. We provide a simple and general mechanism underlying the effect, based on the spreading of nonconserved operators in terms of conserved densities. Grounded only in locality, unitarity, and symmetry, our analysis clarifies the emergence of Mpemba physics in chaotic quantum systems.}, archive = {J_PRL}, author = {Xhek Turkeshi and Pasquale Calabrese and Andrea De Luca}, doi = {10.1103/5d6p-8d1b}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040403}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum mpemba effect in random circuits}, volume = {135}, year = {2025}, }
• (2025). Finite-temperature quantum topological order in three dimensions. PRL, 135(4), 040402. (www)

  @article{ , abstract = {We identify a three-dimensional system that exhibits long-range entanglement at sufficiently small but nonzero temperature—it therefore constitutes a quantum topological order at finite temperature. The model of interest is known as the fermionic toric code, a variant of the usual 3D toric code, which admits emergent fermionic pointlike excitations. The fermionic toric code, importantly, possesses an anomalous two-form symmetry, associated with the spacelike Wilson loops of the fermionic excitations. We argue that it is this symmetry that imbues low-temperature thermal states with a novel topological order and long-range entanglement. Based on the current classification of three-dimensional topological orders, we expect that the low-temperature thermal states of the fermionic toric code belong to a phase of matter that, in the context of equilibrium phases of matter, only exists at nonzero temperatures. We conjecture that further examples of topological orders at nonzero temperatures are given by discrete gauge theories with anomalous two-form symmetries. Our Letter therefore opens the door to studying quantum topological order at nonzero temperature in physically realistic dimensions.}, archive = {J_PRL}, author = {Shu-Tong Zhou and Meng Cheng and Tibor Rakovszky and Curt von Keyserlingk and Tyler D. Ellison}, doi = {10.1103/n9sq-8cxw}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040402}, shortjournal = {Phys. Rev. Lett.}, title = {Finite-temperature quantum topological order in three dimensions}, volume = {135}, year = {2025}, }
• (2025). Effective theory for strongly attractive one-dimensional fermions. PRL, 135(4), 040401. (www)

  @article{ , abstract = {We study a one-dimensional system of two-component fermions in the limit of strong attractive particle-particle interactions. First, we analyze scattering in the corresponding few-body problem, which is analytically solvable via Bethe ansatz. This allows us to engineer effective interactions between the system’s effective degrees of freedom: fermions and bosonic dimers (tightly bound pairs of fermions). We argue that, although these interactions are strong, the resulting effective problem can be mapped onto a weakly interacting one, paving the way for the use of perturbation theory. This finding simplifies studies of many-fermion systems under confinement that are beyond reach of state-of-the-art numerical methods. We illustrate this statement by considering an impurity atom in a Fermi gas.}, archive = {J_PRL}, author = {Timothy G. Backert and Fabian Brauneis and Matija Čufar and Joachim Brand and Hans-Werner Hammer and Artem G. Volosniev}, doi = {10.1103/8mnc-x42q}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040401}, shortjournal = {Phys. Rev. Lett.}, title = {Effective theory for strongly attractive one-dimensional fermions}, volume = {135}, year = {2025}, }
• (2025). Simulating quantum instruments with projective measurements and quantum postprocessing. PRL, 135(4), 040202. (www)

  @article{ , abstract = {Quantum instruments describe both the classical outcome and the updated state associated with a quantum measurement. We ask whether these processes can be simulated using only a natural subset of resources, namely projective measurements on the system and quantum processing of the postmeasurement states. We show that the simulability of instruments can be connected to an entanglement classification problem. This leads to a computationally efficient necessary condition for simulation of generic instruments and to a complete characterisation for qubits. We use this to address relevant quantum information tasks, namely (i) the noise tolerance of standard qubit unsharp measurements, (ii) nonprojective advantages in information-disturbance trade-offs, and (iii) increased sequential Bell inequality violations under projective measurements. Moreover, we consider also d -dimensional Lüders instruments that correspond to weak versions of standard basis measurements and show that for large d these can permit scalable noise advantages over projective implementations.}, archive = {J_PRL}, author = {Shishir Khandelwal and Armin Tavakoli}, doi = {10.1103/bhr5-g71p}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040202}, shortjournal = {Phys. Rev. Lett.}, title = {Simulating quantum instruments with projective measurements and quantum postprocessing}, volume = {135}, year = {2025}, }
• (2025). Entanglement structure of non-gaussian states and how to measure it. PRL, 135(4), 040201. (www)

  @article{ , abstract = {Rapidly growing capabilities of quantum simulators to probe quantum many-body phenomena require new methods to characterize increasingly complex states. We present a protocol that constrains quantum states using experimentally measured correlation functions. This method enables measurement of a quantum state’s entanglement structure, opening a new route to study entanglement-related phenomena. Our approach extends Gaussian state parameterizations by systematically incorporating higher-order correlations. We show the protocol’s usefulness in conjunction with current and forthcoming experimental capabilities, focusing on weakly interacting fermions as a proof of concept. Here, the lowest nontrivial expansion quantitatively predicts early time thermalization dynamics, including signaling the onset of quantum chaos indicated by the entanglement Hamiltonian.}, archive = {J_PRL}, author = {Henry Froland and Torsten V. Zache and Robert Ott and Niklas Mueller}, doi = {10.1103/pnp2-g1g5}, journal = {Physical Review Letters}, month = {7}, number = {4}, pages = {040201}, shortjournal = {Phys. Rev. Lett.}, title = {Entanglement structure of non-gaussian states and how to measure it}, volume = {135}, year = {2025}, }
• (2025). Nonequilibrium structure and relaxation in active microemulsions. PRL, 135(3), 038401. (www)

  @article{ , abstract = {Microphase separation is common in active biological systems as exemplified by the separation of RNA- and DNA-rich phases in the cell nucleus driven by the transcriptional activity of polymerase enzymes acting similarly to amphiphiles in a microemulsion. Here we propose an analytically tractable model of an active microemulsion to investigate how the activity affects its structure and relaxation dynamics. Continuum theory derived from a lattice model exhibits two distinct regimes of the relaxation dynamics and is linked to the broken detailed balance due to intermittent activity of the amphiphiles.}, archive = {J_PRL}, author = {Rakesh Chatterjee and Hui-Shun Kuan and Frank Jülicher and Vasily Zaburdaev}, doi = {10.1103/jfm6-8h9s}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {038401}, shortjournal = {Phys. Rev. Lett.}, title = {Nonequilibrium structure and relaxation in active microemulsions}, volume = {135}, year = {2025}, }
• (2025). T-shaped fe-based multistoichiometry stereoscopic composite catalyst with ultrahigh activity toward fenton-like water treatment, synthesized via graphene-controlled growth. PRL, 135(3), 038001. (www)

  @article{ , abstract = {We report an unusual T-shaped Fe-based multistoichiometry stereoscopic composite catalyst with multifunctional active sites, fabricated via a one-step graphene-controlled all-solid-state synthesis. This tailored catalyst can improve all three catalysis processes of adsorption, peroxide bond activation, and desorption, resulting in a novel catalytic framework where the two-dimensional (2D) nanosheets optimize adsorption, and the 2D FeOCl nanosheets vertically grown on the surface can facilitate both the generation and desorption of .}, archive = {J_PRL}, author = {Dongting Yue and Tianbiao Zeng and Yunzhang Li and Jiahong Lin and Jiewei Xiao and Xing Liu and Youjia Ma and Mengxiang Zhu and Tao Ding and Zhengyang Liu and Xiushen Ye and Zhongjie Zhu and Kan Li and Yihong Ding and Guosheng Shi}, doi = {10.1103/vdxk-lvnt}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {038001}, shortjournal = {Phys. Rev. Lett.}, title = {T-shaped fe-based multistoichiometry stereoscopic composite catalyst with ultrahigh activity toward fenton-like water treatment, synthesized via graphene-controlled growth}, volume = {135}, year = {2025}, }
• (2025). Ground states of the mean-field spin glass with 3-spin couplings. PRL, 135(3), 037402. (www)

  @article{ , abstract = {We use heuristic optimization methods in extensive computations to determine with low systematic error ground-state configurations of the mean-field -spin glass model with . Here, all possible triplets in a system of Ising spins are connected with a bond. This model has been of recent interest, since it exhibits the “overlap gap condition,” which should make it prohibitive to find ground states asymptotically with local search methods when compared, for instance, with the case better known as the Sherrington-Kirkpatrick model (SKM). Indeed, it proves more costly to find good approximations for than for the SKM, even for our heuristic. Compared to the SKM, the ground-state behavior for is quite distinct also in other ways. For the SKM, finite-size corrections for large system sizes , of both the ensemble average over ground-state energy densities and the width of their distribution, vary anomalously with noninteger exponents. In the case here, the energy density and its distribution appear to scale with and corrections, respectively. The distribution itself is consistent with a Gumbel form. Even more stark is the contrast for the bond-diluted case, where the SKM has shown previously a notable variation of the anomalous corrections exponent with the bond density, while for no such variation is found here. Hence, for the 3-spin model, all measured corrections scale the same as for the random energy model (REM), corresponding to . This would suggest that all -spin models with exhibit the same ground-state corrections as in the REM.}, archive = {J_PRL}, author = {Stefan Boettcher and Ginger E. Lau}, doi = {10.1103/j159-lpfx}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {037402}, shortjournal = {Phys. Rev. Lett.}, title = {Ground states of the mean-field spin glass with 3-spin couplings}, volume = {135}, year = {2025}, }
• (2025). Altruistic resource-sharing mechanism for synchronization: The energy-speed-accuracy trade-off. PRL, 135(3), 037401. (www)

  @article{ , abstract = {Synchronization among a group of active agents is ubiquitous in nature. Although synchronization based on direct interactions between agents described by the Kuramoto model is well understood, the other general mechanism based on indirect interactions among agents sharing limited resources are less known. Here, we propose a minimal thermodynamically consistent model for the altruistic resource-sharing (ARS) mechanism wherein resources are needed for an individual agent to advance but a more advanced agent has a lower competence to obtain resources. We show that while differential competence in ARS mechanism provides a negative feedback leading to synchronization it also breaks detailed balance and thus requires additional energy dissipation besides the cost of driving individual agents. By solving the model analytically, our study reveals a general trade-off relation between the total energy dissipation rate and the two key performance measures of the system: average speed and synchronization accuracy. For a fixed dissipation rate, there is a distinct speed-accuracy Pareto front traversed by the scarcity of resources: scarcer resources lead to slower speed but more accurate synchronization. Increasing energy dissipation eases this trade-off by pushing the speed-accuracy Pareto front outward. The connections of our work to realistic biological systems such as the KaiABC system in cyanobacterial circadian clock and other theoretical results based on thermodynamic uncertainty relation are also discussed.}, archive = {J_PRL}, author = {Dongliang Zhang (张东良 and Yuansheng Cao and Qi Ouyang and Yuhai Tu}, doi = {10.1103/snks-5fff}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {037401}, shortjournal = {Phys. Rev. Lett.}, title = {Altruistic resource-sharing mechanism for synchronization: The energy-speed-accuracy trade-off}, volume = {135}, year = {2025}, }
• (2025). Information-optimal mixing at low reynolds number. PRL, 135(3), 037101. (www)

  @article{ , abstract = {Mutual information between particle positions before and after mixing provides a universal assumption-free measure of mixing efficiency at low Reynolds number that accounts for the kinematic reversibility of the Stokes equation. For a generic planar shear flow with time-dependent shear rate, we derive a compact expression for the mutual information as a nonlinear functional of the shearing protocol and solve the associated extremization problem exactly to determine the optimal control under both linear and nonlinear constraints, specifically total shear and total dissipation per unit volume. Remarkably, optimal protocols turn out to be universal and time-reversal symmetric in both cases. Our results establish a minimum energetic cost of erasing information in a broad class of nonequilibrium drift-diffusive systems.}, archive = {J_PRL}, author = {Luca Cocconi and Yihong Shi and Andrej Vilfan}, doi = {10.1103/cl9m-cmhb}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {037101}, shortjournal = {Phys. Rev. Lett.}, title = {Information-optimal mixing at low reynolds number}, volume = {135}, year = {2025}, }
• (2025). Amplitude mode in a multigap superconductor MgB2 investigated by terahertz two-dimensional coherent spectroscopy. PRL, 135(3), 036902. (www)

  @article{ , abstract = {We have investigated the terahertz (THz) nonlinear response of the multigap superconductor , using THz two-dimensional coherent spectroscopy (THz 2DCS). With broadband THz drive fields, we identified a nonlinear response at twice the lower superconducting gap energy at the lowest temperatures. Using narrow-band THz driving pulses, we observed first (FH) and third harmonic responses. The FH intensity shows a monotonic increase with decreasing temperature when properly normalized by the driving field strength. This is distinct from the single-gap superconductor NbN, where the FH signal exhibited a resonant enhancement at temperatures when twice the gap energy was resonant with the driving photon energy, which was interpreted to originate from the superconducting amplitude mode. Our results in are consistent with a well-defined amplitude mode only at the lowest temperatures and indicate strong damping as temperature increases. This likely indicates the importance of interband coupling in and its influence on the nature of the amplitude mode and its damping.}, archive = {J_PRL}, author = {Kota Katsumi and Jiahao Liang and Ralph Romero, III and Ke Chen and Xiaoxing Xi and N. P. Armitage}, doi = {10.1103/g5rp-6vb1}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036902}, shortjournal = {Phys. Rev. Lett.}, title = {Amplitude mode in a multigap superconductor MgB2 investigated by terahertz two-dimensional coherent spectroscopy}, volume = {135}, year = {2025}, }
• (2025). Electrically tunable and enhanced nonlinearity of moiré exciton polaritons in transition metal dichalcogenide bilayers. PRL, 135(3), 036901. (www)

  @article{ , abstract = {We develop a microscopic theory for nonlinear optical response of moiré exciton polaritons in bilayers of transition metal dichalcogenides (TMDs). Our theory allows us to study the tunnel-coupled intralayer and interlayer excitonic modes for a wide range of twist angles ( ), external electric field, and light-matter coupling, providing insights into the hybridization regime inaccessible before. Specifically, we account for the umklapp scattering processes of two exciton polaritons responsible for enhanced nonlinearity, and show that it is crucial for describing interactions at strong hybridization. We reveal a regime of attractive nonlinearity for moiré polaritons, stemming from the anisotropic Coulomb interactions, which can explain some of experimental features of optical response in TMD bilayers. Furthermore, within our theory we demonstrate that the attractive nonlinearity can be tuned into repulsive by applying an external electric field. Our findings show that nonlinear moiré polaritons offer a controllable platform nonlinear polaritonic devices.}, archive = {J_PRL}, author = {Kok Wee Song and Oleksandr Kyriienko}, doi = {10.1103/gr72-szwg}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036901}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically tunable and enhanced nonlinearity of moiré exciton polaritons in transition metal dichalcogenide bilayers}, volume = {135}, year = {2025}, }
• (2025). Large kohn anomaly and phonon collapse induced by charge density wave in UPt2Si2. PRL, 135(3), 036705. (www)

  @article{ , abstract = {Using high-energy-resolution inelastic x-ray scattering, we observe anomalous softening and damping of the transverse acoustic phonon in as the system is cooled toward the charge density wave (CDW) transition temperature . The phonon exhibits a marked Kohn-type anomaly around the CDW wave vector and becomes overdamped within a finite momentum range already well above . The dispersion anomaly is consistent with potential Fermi surface nesting, which together with the extended phonon collapse indicates strong electron-phonon coupling. The transition temperature estimated from the phonon softening is markedly lower than , consistent with a primarily electronic instability rather than a phonon-driven transition. Our results establish as a prime example of a strongly correlated electron CDW system with exceptionally strong electron-phonon coupling driving phonon softening and collapse.}, archive = {J_PRL}, author = {Jooseop Lee and Greta L. Chappell and Ryan E. Baumbach and Ayman H. Said and Igor A. Zaliznyak}, doi = {10.1103/clg4-2zzb}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036705}, shortjournal = {Phys. Rev. Lett.}, title = {Large kohn anomaly and phonon collapse induced by charge density wave in UPt2Si2}, volume = {135}, year = {2025}, }
• (2025). Beyond orbitally resolved magnetic exchange in CrI3 and NiI2. PRL, 135(3), 036704. (www)

  @article{ , abstract = {The pertinent need for a microscopic understanding of magnetic exchange motivated us to go beyond the existing theories and develop a systematic method to quantify all possible mechanisms that contribute to magnetic exchange for an arbitrary pair of atoms in a given material. We apply it to the archetypal 2D magnetic monolayers and , to reveal the previously underrated , contribution as either the leading or the second largest contribution to the total magnetic exchange. We proceed to explore the microscopic mechanisms behind all the nonzero orbital contributions in both and , and generalize the findings to other magnetic monolayers dominated by and electronic configurations of the magnetic atoms.}, archive = {J_PRL}, author = {D. Šabani and C. Bacaksiz and M. V. Milošević}, doi = {10.1103/tlq2-m6zk}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036704}, shortjournal = {Phys. Rev. Lett.}, title = {Beyond orbitally resolved magnetic exchange in CrI3 and NiI2}, volume = {135}, year = {2025}, }
• (2025). Exchange engineering of a two-dimensional half-metal. PRL, 135(3), 036703. (www)

  @article{ , abstract = {We report the emergence of two-dimensional itinerant half-metallicity in a two-atomic-layer thick iron-palladium alloy. Against the common belief that spin-orbit coupling is adverse to half-metallicity, the complex interplay between exchange and spin-orbit coupling counterintuitively enables it via electronic band hybridization. The 2D ferromagnet is engineered directly via controlled alloying and is verified experimentally via spin-resolved band structure analyses. First-principles calculations corroborate its tunability by providing a systematic bottom-up approach through stepwise ground-state construction. The appearance of hybridization points at specific points, via interplay between exchange and spin-orbit interactions, is responsible for the emergence of half-metallicity.}, archive = {J_PRL}, author = {Xin Liang Tan and Arthur Ernst and Kenta Hagiwara and Ying-Jiun Chen and Claus Michael Schneider and Christian Tusche}, doi = {10.1103/mx46-85zf}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036703}, shortjournal = {Phys. Rev. Lett.}, title = {Exchange engineering of a two-dimensional half-metal}, volume = {135}, year = {2025}, }
• (2025). Anomalous hall effect in type IV 2D collinear magnets. PRL, 135(3), 036702. (www)

  @article{ , abstract = {We identify a previously unrecognized class of two-dimensional (2D) collinear magnetic phase that extends beyond the established categories of ferromagnets, antiferromagnets, and altermagnets. These type IV 2D collinear magnets exhibit spin-degenerate bands in the nonrelativistic limit, yet support time-reversal symmetry-breaking responses, such as the anomalous Hall effect (AHE), despite having zero net magnetization. Based on spin layer group analysis, we derive the symmetry criteria for this phase and perform first-principles calculations to screen viable candidate materials from 2D databases. Using monolayer as a prototype, we demonstrate that in the absence of spin-orbit coupling, the bands are spin degenerate, while its inclusion induces an AHE driven by spin-polarized and even spin-neutral currents, accompanied by a symmetry-protected, truly full-space persistent spin texture. These findings expand the classification of magnetic phases and broaden avenues for realizing unconventional spintronic functionalities in two dimensions.}, archive = {J_PRL}, author = {Ling Bai and Run-Wu Zhang and Wanxiang Feng and Yugui Yao}, doi = {10.1103/rn1l-d6cq}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036702}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous hall effect in type IV 2D collinear magnets}, volume = {135}, year = {2025}, }
• (2025). Engineering altermagnetic states in two-dimensional square tessellations. PRL, 135(3), 036701. (www)

  @article{ , abstract = {Altermagnetism, an emergent collinear magnetic phase with zero net magnetization and momentum-dependent spin splitting, promises to revolutionize spintronics by leveraging symmetry-driven effects without requiring spin-orbit coupling. Despite its potential, a comprehensive understanding of design principles and spin-splitting mechanisms remains elusive. Here, from a mathematical perspective, we exploit the intrinsic fourfold symmetry and structural versatility of 2D square tessellations to engineer altermagnetic states. By systematically screening the altermagnetic state in all 34 2D square tessellations in the Reticular Chemistry Structure Resource database, we identify the “Lieb” (a regular lattice with 4.4.4.4 tessellation), “fes” (a semiregular net with 4.8.8 tessellation), and “tts” (a semiregular net with 3.3.4.3.4 tessellation) nets as key candidates. A tight-binding Hamiltonian analysis reveals the physical origin of spin splitting across these different tessellated nets. As proof of concept, we demonstrate the pyracylene-based metal-organic framework monolayer , with the tts net, as a robust altermagnet exhibiting a symmetry-compliant ground state. Our Letter provides a symmetry-driven design framework that bridges the mathematical architecture of tessellations with computational materials discovery, enabling reasonable control of altermagnetism in 2D materials.}, archive = {J_PRL}, author = {Yixuan Che and Haifeng Lv and Xiaojun Wu and Jinlong Yang}, doi = {10.1103/v38b-5by1}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036701}, shortjournal = {Phys. Rev. Lett.}, title = {Engineering altermagnetic states in two-dimensional square tessellations}, volume = {135}, year = {2025}, }
• (2025). Variational wave-function analysis of the fractional anomalous hall crystal. PRL, 135(3), 036604. (www)

  @article{ , abstract = {We propose fractional anomalous Hall crystals (FAHCs) as possible ground states of strongly interacting electrons in parent bands with Berry curvature. FAHCs are exotic states of matter that spontaneously break continuous translation symmetry to form a fractional Chern insulator. We construct a unified family of variational wave functions that describe FAHCs and their competing states in the presence of uniform parent Berry curvature. We calculate their variational energy with Coulomb interactions semianalytically in the thermodynamic limit. Our analysis reveals that FAHCs can be energetically favorable over both Wigner crystals and integer anomalous Hall crystals for sufficiently strong interactions or flat dispersion.}, archive = {J_PRL}, author = {Tixuan Tan and Julian May-Mann and Trithep Devakul}, doi = {10.1103/dd2d-kk3w}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036604}, shortjournal = {Phys. Rev. Lett.}, title = {Variational wave-function analysis of the fractional anomalous hall crystal}, volume = {135}, year = {2025}, }
• (2025). Bidirectional asymmetric frequency conversion in nonlinear phononic crystals. PRL, 135(3), 036603. (www)

  @article{ , abstract = {Beyond conservative systems, altering the wave propagation frequency emerges as a crucial factor across diverse physical domains. This Letter presents a demonstration of bidirectional asymmetric frequency conversion—either upward or downward—depending on the excitation direction, surpassing conventional unidirectional mechanisms. We numerically and experimentally demonstrate its practical realization in a model system of cylindrical granular crystals with intrinsic local resonance coupling. This novel wave transport mechanism arises from the interplay of nonlinear contact, spatial asymmetry, and coupled local resonance. In particular, we show that local resonance coupling induces wavenumber-dependent wave dynamics, including frequency conversion. Given that this local resonance exemplifies avoided crossings (i.e., strong coupling), this Letter may inspire studies on nonlinear systems supporting material or structural resonance.}, archive = {J_PRL}, author = {Yeongtae Jang and Beomseok Oh and Eunho Kim and Junsuk Rho}, doi = {10.1103/3n97-7kmd}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036603}, shortjournal = {Phys. Rev. Lett.}, title = {Bidirectional asymmetric frequency conversion in nonlinear phononic crystals}, volume = {135}, year = {2025}, }
• (2025). Experimental observation of k-dependent bulk-edge correspondence in sonic semimetals with high winding numbers. PRL, 135(3), 036602. (www)

  @article{ , abstract = {The bulk-edge correspondence plays a crucial role in topological physics bridging the gap between the bulk topology and the topological edge states, which recently was extended to topological metamaterials having a large number of topological boundary states. In this work, we experimentally observe the -dependent bulk-edge correspondence in the framework of a manmade sonic semimetal, supporting the coexistence of multiple topological phases which are separated by boundaries formed by versatile types of Dirac points. The structure is composed of stacked one-dimensional (1D) extended Su-Schrieffer-Heeger chains through long-range couplings, in which the topological phases are characterized by -dependent winding numbers. Through an elaborately designed methodology for measuring the acoustic pressure amplitude and phase, we not only derive -dependent topological winding numbers but also clearly observe the spatial distribution characteristics of edge states across different phases. Our findings significantly broaden the understanding of these critical topological phases and open up avenues for the manipulation of classical waves.}, archive = {J_PRL}, author = {Wei Xiong and Tingde Zhang and Zhiwang Zhang and Yuanzhou Zhu and Shuochen Wang and Haixiao Zhang and Ying Cheng and Xiaojun Liu and Johan Christensen}, doi = {10.1103/wkwd-cbn2}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036602}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental observation of k-dependent bulk-edge correspondence in sonic semimetals with high winding numbers}, volume = {135}, year = {2025}, }
• (2025). Anyonic phase transitions in the 1D extended hubbard model with fractional statistics. PRL, 135(3), 036601. (www)

  @article{ , abstract = {We study one-dimensional lattice anyons with extended Hubbard interactions at unit filling using bosonization and numerical simulations. The behavior can be continuously tuned from bosonic to fermionic statistics by adjusting the topological exchange angle , which leads to a competition of different instabilities. We present the bosonization theory in the presence of dynamic gauge fields, which predicts a phase diagram of four different gapped phases with distinct dominant correlations. Advanced numerical simulations determine and analyze the exact phase transitions between Mott insulator, charge density wave, dimerized state, and Haldane insulator, all of which meet at a multicritical line in the parameter space of anyonic angle , on-site interaction , and nearest neighbor repulsion . Superfluid and pair-superfluid phases are stable in a region of small .}, archive = {J_PRL}, author = {Martin Bonkhoff and Kevin Jägering and Shijie Hu and Axel Pelster and Sebastian Eggert and Imke Schneider}, doi = {10.1103/7n1c-vq2p}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036601}, shortjournal = {Phys. Rev. Lett.}, title = {Anyonic phase transitions in the 1D extended hubbard model with fractional statistics}, volume = {135}, year = {2025}, }
• (2025). Tensor-network study of the roughening transition in a (2+1)D z2 lattice gauge theory with matter. PRL, 135(3), 036503. (www)

  @article{ , abstract = {Within the confined phase of lattice gauge theories a roughening transition arises between a weakly confined regime with floppy string excitations and a strongly confined regime with stiff string excitations. In this Letter, we use an infinite Density Matrix Renormalization Group (iDMRG) algorithm to quantitatively characterize the properties of confined strings. To this end, we stabilize the state with a string excitation by ’t Hooft loop operators. While for zero gauge-matter coupling we can use bare ’t Hooft loop operators to do so, for finite gauge-matter coupling we have to transform them to emergent ones, which we achieve with an adiabatic protocol. By analyzing the scaling of both a novel order parameter and the entanglement entropy, our approach allows us to accurately determine the roughening transition, even at finite gauge-matter coupling.}, archive = {J_PRL}, author = {Wen-Tao Xu and Michael Knap and Frank Pollmann}, doi = {10.1103/3lxj-dx76}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036503}, shortjournal = {Phys. Rev. Lett.}, title = {Tensor-network study of the roughening transition in a (2+1)D z2 lattice gauge theory with matter}, volume = {135}, year = {2025}, }
• (2025). Altermagnetic phase transition in a lieb metal. PRL, 135(3), 036502. (www)

  @article{ , abstract = {We analyze the phase transition between a symmetric metallic parent state and itinerant altermagnetic order. The underlying mechanism we reveal in our microscopic model of electrons on a Lieb lattice does not involve orbital ordering, but derives from sublattice interference.}, archive = {J_PRL}, author = {Matteo Dürrnagel and Hendrik Hohmann and Atanu Maity and Jannis Seufert and Michael Klett and Lennart Klebl and Ronny Thomale}, doi = {10.1103/2g3v-z76q}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036502}, shortjournal = {Phys. Rev. Lett.}, title = {Altermagnetic phase transition in a lieb metal}, volume = {135}, year = {2025}, }
• (2025). New classes of quantum anomalous hall crystals in multilayer graphene. PRL, 135(3), 036501. (www)

  @article{ , abstract = {The recent experimental observation of quantum anomalous Hall (QAH) effects in the rhombohedrally stacked pentalayer graphene has motivated theoretical discussions on the possibility of quantum anomalous Hall crystal (QAHC), a topological version of Wigner crystal. Conventional topological Wigner crystals typically have one electron per unit cell. In this Letter we propose new types of topological Wigner crystals labeled as QAHC- , with electrons per unit cell. In the pentalayer graphene system, we find parameter regimes where QAHC-2 and QAHC-3 have lower energy than the conventional QAHC-1 at total filling per moiré unit cell. These states all have total Chern number and are consistent with the QAH effect observed in the experiments. The larger period QAHC states have lower kinetic energy due to the unique Mexican-hat dispersion of the pentalayer graphene, which can compensate for the loss in the interaction energy. Unlike QAHC-1, QAHC-2, and QAHC-3 break the moiré translation symmetry and are sharply distinct from a moiré band insulator. We also briefly discuss the competition between integer QAH and fractional QAH states at filling . Moreover, we find that a stronger moiré potential can significantly change the phase diagram and even favors a QAHC-1 ansatz with Chern band.}, archive = {J_PRL}, author = {Boran Zhou and Ya-Hui Zhang}, doi = {10.1103/26pl-gkh7}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036501}, shortjournal = {Phys. Rev. Lett.}, title = {New classes of quantum anomalous hall crystals in multilayer graphene}, volume = {135}, year = {2025}, }
• (2025). First-principles framework for the prediction of intersystem crossing rates in spin defects: The role of electron correlation. PRL, 135(3), 036401. (www)

  @article{ , abstract = {Optically active spin defects in solids are promising platforms for quantum technologies. Here, we present a first-principles framework to investigate intersystem crossing processes, which represent crucial steps in the optical spin-polarization cycle used to address spin defects. Considering the nitrogen-vacancy center in diamond as a case study, we demonstrate that our framework effectively captures electron correlation effects in the calculation of many-body electronic states and their spin-orbit coupling and electron-phonon interactions, while systematically addressing finite-size effects. We validate our predictions by carrying out measurements of fluorescence lifetimes, finding excellent agreement between theory and experiments. The framework presented here provides a versatile and robust tool for exploring the optical cycle of varied spin defects entirely from first principles.}, archive = {J_PRL}, author = {Yu Jin and Jinsoo Park and Marquis M. McMillan and Daniel Donghyon Ohm and Corrie Barnes and Benjamin Pingault and Christopher Egerstrom and Benchen Huang and Marco Govoni and F. Joseph Heremans and David D. Awschalom and Giulia Galli}, doi = {10.1103/nw3r-zy8q}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036401}, shortjournal = {Phys. Rev. Lett.}, title = {First-principles framework for the prediction of intersystem crossing rates in spin defects: The role of electron correlation}, volume = {135}, year = {2025}, }
• (2025). Resistive anomaly near a ferromagnetic phase transition: A classical memory effect. PRL, 135(3), 036301. (www)

  @article{ , abstract = {We investigate resistive anomalies in metals near a ferromagnetic phase transition, emphasizing the role of long-range critical fluctuations. Our analysis shows that electron diffusion near the critical temperature enhances the singular behavior of resistivity via a classical memory effect, exceeding the prediction of Fisher and Langer [ Phys. Rev. Lett. 20 , 665 (1968) ]. Close to , the resistivity develops a cusp or anticusp controlled by the critical exponent of the order parameter. We also express a concomitant non-Drude behavior of the optical conductivity in terms of critical exponents. These results provide deeper insight into the origin of resistive anomalies and their connection to criticality in metallic systems.}, archive = {J_PRL}, author = {Dmitrii L. Maslov and Vladimir I. Yudson and Cristian D. Batista}, doi = {10.1103/ff28-tt6c}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036301}, shortjournal = {Phys. Rev. Lett.}, title = {Resistive anomaly near a ferromagnetic phase transition: A classical memory effect}, volume = {135}, year = {2025}, }
• (2025). Unusual thickness-dependent friction on CuInP2S6 originating from work-function regulation. PRL, 135(3), 036202. (www)

  @article{ , abstract = {Thickness dependence is a unique trait for the friction of two-dimensional materials, where thinner samples are typically found to exhibit higher friction than thicker ones. In this Letter, we show that friction on two-dimensional nanosheets transferred on silicon substrates with predominantly upward polarization can behave in a manner completely opposite to the conventional trend, showing enhanced friction with increasing thicknesses. Assisted by Kelvin Probe Force Microscopy measurements and first-principles calculations, this unusual behavior is attributed to the work-function regulated friction mechanism. Specifically, as the sample thickness increases, the work function decreases for the ferroelectric material, which results in a more pronounced electron transfer effect and thereby stronger interactions across the intimate contact interface. This work sheds light on the physical origins of friction for ferroelectric materials and suggests an effective strategy to actively regulate friction via work-function engineering.}, archive = {J_PRL}, author = {Zhe Chen and Aisheng Song and Shuai Zhang and Ling Wang and Tianbao Ma and Xi-Qiao Feng and Qunyang Li}, doi = {10.1103/6vzc-z849}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036202}, shortjournal = {Phys. Rev. Lett.}, title = {Unusual thickness-dependent friction on CuInP2S6 originating from work-function regulation}, volume = {135}, year = {2025}, }
• (2025). Twisted bilayer materials as a promising platform for solid-state qubits. PRL, 135(3), 036201. (www)

  @article{ , abstract = {Qubits are the fundamental units in quantum computing, quantum communication, and sensing. In current platforms, such as cold atoms, superconducting circuits, point defects, and semiconductor quantum dots, each qubit requires individual preparation, making identical replication a challenging task. Constructing and maintaining stable, scalable qubits remains a formidable challenge. The race to identify the best one remains inconclusive. Our Letter introduces twisted bilayer materials as a promising platform for qubits due to their tunability, natural patterns, and extensive materials library. Our large-scale first-principles calculations reveal that the moiré superlattices have identical and localized states, akin to the discrete energy levels of an alkali atom. Existing experimental techniques allow for individual initialization, manipulation, and readout. The vast array of 2D materials provides a multitude of potential candidates for qubit exploration. Because of their inherent scalability and uniformity, our proposed qubits present significant advantages over conventional solid-state qubit systems.}, archive = {J_PRL}, author = {Zhigang Song and Yidan Wang and Péter Udvarhelyi and Prineha Narang}, doi = {10.1103/v1vp-z8jl}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {036201}, shortjournal = {Phys. Rev. Lett.}, title = {Twisted bilayer materials as a promising platform for solid-state qubits}, volume = {135}, year = {2025}, }
• (2025). New plasma regime in jupiter’s auroral zones. PRL, 135(3), 035201. (www)

  @article{ , abstract = {Observations from the Juno satellite have indicated very low electron densities, as low as , at high-latitudes in Jupiter’s magnetosphere. This region is strongly magnetized, with surface magnetic fields at the one-bar level up to 20 G, or 2 mT, leading to the unusual situation that the electron plasma frequency is less than the ion gyrofrequency. In this extremely low-density plasma, the Alfven wave becomes a plasma oscillation at the electron plasma frequency at shorter perpendicular wavelengths. Analysis of this mode with a kinetic low-frequency dispersion solver indicates that at large wave number, this mode has the characteristics of the Langmuir wave. Thus, this mode can be called an Alfvén-Langmuir mode. Below the plasma frequency, the high-wave number behavior of this mode exhibits a resonance cone, with frequency determined by the angle of the wave vector with the background magnetic field. These waves can be excited by the upward electron beams observed by Juno.}, archive = {J_PRL}, author = {R. L. Lysak and A. H. Sulaiman and S. S. Elliott and W. S. Kurth and S. J. Bolton}, doi = {10.1103/fn63-qmb7}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {035201}, shortjournal = {Phys. Rev. Lett.}, title = {New plasma regime in jupiter’s auroral zones}, volume = {135}, year = {2025}, }
• (2025). First demonstration of improved fusion yield with increased compression through reduced adiabat in inertial confinement fusion experiments at the national ignition facility. PRL, 135(3), 035101. (www)

  @article{ , abstract = {Recent advancements in indirect-drive inertial confinement fusion (ICF) experiments at the National Ignition Facility (NIF) have achieved a significant milestone by demonstrating target gains greater than one, yet future applications necessitate much higher target gains. One approach to achieving improved implosion performance is to pursue increased fuel compression via a lowered implosion adiabat. Experiments have been performed testing a reduced adiabat by introducing small changes to the drive laser pulse shape and the resulting shock timing for an existing implosion design at 1.9 MJ laser drive with near-ignition performance (experiment N210808). Experiments using the updated design demonstrate, for the very first time, increased compression and fusion yield in ICF implosions on the NIF by using a lower fuel adiabat, and increased compression with a reduced adiabat in high-density carbon ablators. Compared to the previously best-performing experiment with a laser energy of 1.9 MJ, these experiments exhibit increases of up to 80% and 14% in nuclear fusion yield and fuel compression, respectively, and with repeatable performance. Further, it is the only implosion design to have achieved a target gain exceeding one with a laser energy of less than 2 MJ. These findings highlight the efficacy of reduced adiabat designs in achieving higher compression and fusion yields, offering a promising pathway for future ICF applications. This Letter not only addresses a long-standing question in ICF but also paves the way for achieving higher target gains with optimized implosion strategies.}, archive = {J_PRL}, author = {M. Hohenberger and D. S. Clark and K. D. Humbird and A. Pak and A. Do and C. V. Young and T. Döppner and A. L. Kritcher and D. T. Casey and A. Allen and S. H. Baxamusa and B. Bachmann and J. Biener and R. M. Bionta and T. Braun and T. M. Briggs and T. Chapman and C. R. Danly and T. R. Dittrich and L. Divol and M. Durocher and V. E. Fatherley and T. Fehrenbach and M. Freeman and S. W. Haan and K. D. Hahn and S. Hayes and O. A. Hurricane and S. F. Khan and C. W. Kong and B. Kozioziemski and O. L. Landen and B. J. MacGowan and S. A. MacLaren and M. Millot and A. S. Moore and A. Nikroo and R. C. Nora and J. E. Ralph and M. Ratledge and M. S. Rubery and D. J. Schlossberg and M. P. Selwood and M. Stadermann and S. Stoupin and C. Trosseille and C. R. Weber and C. Wild and C. Wilde and B. N. Woodworth and A. B. Zylstra}, doi = {10.1103/h2ss-6zpf}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {035101}, shortjournal = {Phys. Rev. Lett.}, title = {First demonstration of improved fusion yield with increased compression through reduced adiabat in inertial confinement fusion experiments at the national ignition facility}, volume = {135}, year = {2025}, }
• (2025). First lasing and stable operation of a direct-amplification enabled harmonic generation free-electron laser. PRL, 135(3), 035001. (www)

  @article{ , abstract = {Seeded free-electron lasers (FELs) capable of operating at repetition rates up to the MHz level are in high demand for advanced time-resolved spectroscopies, which require both full longitudinal coherence and high average photon flux in the extreme ultraviolet (EUV) and x-ray regimes. However, conventional external-seeding methods require ultraviolet seed lasers with peak powers on the order of 100 MW, constraining them to lower repetition rates. Here, we report the first lasing and stable operation of a direct-amplification enabled harmonic generation FEL driven by a weak seed laser with only MW-level peak power. Beginning with an ultraviolet seed laser with only pulse energy, we demonstrate its direct amplification to over within an 8-m-long modulator. We observe coherent harmonic generation up to the harmonic of the seed and achieve saturation of the harmonic in the radiator. These results represent a crucial milestone toward the realization of MHz-class, fully coherent EUV and x-ray light sources.}, archive = {J_PRL}, author = {Zheng Qi and Junhao Liu and Lanpeng Ni and Tao Liu and Zhen Wang and Kaiqing Zhang and Hanxiang Yang and Zhangfeng Gao and Nanshun Huang and Si Chen and Hang Luo and Yaozong Xiao and Cheng Yu and Yongmei Wen and Fei Gao and Yangyang Lei and Huan Zhao and Yanyan Zhu and Liping Sun and Weiyi Yin and Xingtao Wang and Taihe Lan and Xiaoqing Liu and Lie Feng and Wenyan Zhang and Ximing Zhang and Bin Li and Chao Feng and Bo Liu and Zhentang Zhao}, doi = {10.1103/sslg-jjkz}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {035001}, shortjournal = {Phys. Rev. Lett.}, title = {First lasing and stable operation of a direct-amplification enabled harmonic generation free-electron laser}, volume = {135}, year = {2025}, }
• (2025). Skyrmionic polarization texture around the phase singularity of optical vortices. PRL, 135(3), 033805. (www)

  @article{ , abstract = {We disclose the existence of a type of optical skyrmion, Gauss-Stokes (GS) skyrmions, that is naturally present in an optical vortex around its phase singularity. Contrary to previous research with optical skyrmions, we neither shape vector beams nor superpose different spatial modes and polarizations. In GS skyrmions, the phase singularity in the transversal field of a single monochromatic beam of uniform polarization (a scalar beam) is concealed by the axial field dictated by Gauss’s divergence law, giving rise to a polarization singularity of undefined polarization plane. This singularity is enclosed by a rich skyrmionic polarization texture fulfilling a topological map and covering all the states of transverse-axial polarization. In our experiment, we facilitate the observation of a GS skyrmion with the predicted features using focused fields with an enhanced axial component.}, archive = {J_PRL}, author = {Nilo Mata-Cervera and Deepak K. Sharma and Yijie Shen and Ramon Paniagua-Dominguez and Miguel A. Porras}, doi = {10.1103/ndy2-wxwx}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033805}, shortjournal = {Phys. Rev. Lett.}, title = {Skyrmionic polarization texture around the phase singularity of optical vortices}, volume = {135}, year = {2025}, }
• (2025). Radiant field theory: A transport approach to shaped wave transmission through disordered media. PRL, 135(3), 033804. (www)

  @article{ , abstract = {We present a field-theoretic framework to characterize the distribution of transmission eigenvalues for coherent wave propagation through disordered media. The central outcome is a transport equation for a matrix-valued radiance, analogous to the classical radiative transport equation but capable of capturing coherent effects encoded in the transmission matrix. Unlike the Dorokhov-Mello-Pereyra-Kumar (DMPK) theory, our approach does not rely on the isotropy hypothesis, which presumes uniform angular scattering by material slices. As a result, it remains valid beyond the diffusive regime, accurately describing the transmission eigenvalue distribution in the quasiballistic regime as well. Moreover, the framework is more versatile than the DMPK theory, enabling straightforward incorporation of experimental realities such as absorption and incomplete channel control. These factors are frequently encountered in wave experiments on complex media but have lacked an ab initio theoretical treatment until now. We validate our predictions through numerical simulations based on the microscopic wave equation, confirming the accuracy and broad applicability of the theory.}, archive = {J_PRL}, author = {David Gaspard and Arthur Goetschy}, doi = {10.1103/g3kd-sg4x}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033804}, shortjournal = {Phys. Rev. Lett.}, title = {Radiant field theory: A transport approach to shaped wave transmission through disordered media}, volume = {135}, year = {2025}, }
• (2025). Extremely narrow band in moiré photonic time crystal. PRL, 135(3), 033803. (www)

  @article{ , abstract = {The moiré superlattice has attracted growing interest in the electromagnetic and optical communities. Here, we extend this concept to time-varying photonic systems by superposing two binary modulations on the refractive index with different modulation periods, i.e., the moiré photonic time crystal (PTC). Such a moiré PTC leads to extremely narrow bands in momentum space that support temporal localized modes, exhibiting periodically self-reconstructing pulses in the time domain. We investigate the tunability of the band structure of the moiré PTC and the temporal localization behavior, which can be greatly manipulated by varying the temporal modulation parameters. Moreover, we explore the Floquet mode-locking mechanism in the moiré PTC, which points toward potential applications in mode-locked lasers with a tunable time width of the generated pulses. The modulation-induced extremely narrow band also offers intriguing opportunities in exceptional-point-enhanced sensing. Our Letter brings the concept of moiré patterns to the field of PTCs, and unveils new possibilities in wave manipulations with time-varying systems.}, archive = {J_PRL}, author = {Zhaohui Dong and Xianfeng Chen and Luqi Yuan}, doi = {10.1103/4lqd-z567}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033803}, shortjournal = {Phys. Rev. Lett.}, title = {Extremely narrow band in moiré photonic time crystal}, volume = {135}, year = {2025}, }
• (2025). Universal non-hermitian transport in disordered systems. PRL, 135(3), 033802. (www)

  @article{ , abstract = {In disordered Hermitian systems, localization of energy eigenstates prohibits wave propagation. In non-Hermitian systems, however, wave propagation is possible even when the eigenstates of a Hamiltonian are exponentially localized by disorders. We find in this regime that non-Hermitian wave propagation exhibits novel universal scaling behaviors without Hermitian counterpart. Furthermore, our theory demonstrates how the tail of imaginary-part density of states dictates wave propagation in the long-time limit. Specifically, for the three typical classes, namely the Gaussian, the uniform, and the linear imaginary-part density of states, we obtain logarithmically suppressed sub-ballistic transport, and two types of subdiffusion with exponents that depend only on spatial dimensions, respectively. Our work highlights the fundamental differences between Hermitian and non-Hermitian Anderson localization, and uncovers unique universality in non-Hermitian wave propagation.}, archive = {J_PRL}, author = {Bo Li and Chuan Chen and Zhong Wang}, doi = {10.1103/z9m1-3mwb}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033802}, shortjournal = {Phys. Rev. Lett.}, title = {Universal non-hermitian transport in disordered systems}, volume = {135}, year = {2025}, }
• (2025). Toward nonlinear optics with mössbauer nuclei using X-ray cavities. PRL, 135(3), 033801. (www)

  @article{ , abstract = {Strong excitation of nuclear resonances, particularly of Mössbauer nuclei, has been a longstanding goal and the advance of novel x-ray sources is promising new options in this regard. Here, we map out the necessary experimental conditions for the more general goal of entering the nonlinear optics regime with nuclei and compare with available technology. In particular, we present a comprehensive theory of nonlinear nuclear excitation in thin-film x-ray cavities by focused x-ray pulses. We thereby identify cavity geometries with broad resonances that allow one to boost the nuclear excitation even at moderately tight focusing and offer the possibility to mitigate radiation damage.}, archive = {J_PRL}, author = {Dominik Lentrodt and Christoph H. Keitel and Jörg Evers}, doi = {10.1103/1lcz-r8d3}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033801}, shortjournal = {Phys. Rev. Lett.}, title = {Toward nonlinear optics with mössbauer nuclei using X-ray cavities}, volume = {135}, year = {2025}, }
• (2025). Time-periodic driving of a bath-coupled open quantum gas of light. PRL, 135(3), 033603. (www)

  @article{ , abstract = {We study the frequency-resolved density response of a photon Bose–Einstein condensate coupled to a bath of dye molecules by time-periodic driving. By monitoring the photon number dynamics for different drive frequencies, we obtain the spectral response of the condensate in a phase-sensitive way. We find that as the photon number increases, the response of the coupled condensate-bath system transitions from overdamped to resonant behavior, indicating a transition from closed to open system dynamics. Our spectroscopy method paves the way for studies of collective excitations in complex driven-dissipative systems.}, archive = {J_PRL}, author = {Andris Erglis and Alexander Sazhin and Frank Vewinger and Martin Weitz and Stefan Yoshi Buhmann and Julian Schmitt}, doi = {10.1103/922g-1fng}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033603}, shortjournal = {Phys. Rev. Lett.}, title = {Time-periodic driving of a bath-coupled open quantum gas of light}, volume = {135}, year = {2025}, }
• (2025). Unraveling superradiance: Entanglement and mutual information in collective decay. PRL, 135(3), 033602. (www)

  @article{ , abstract = {We study the collective decay of an initially inverted ensemble of two-level emitters in two distinct scenarios: when coupled to a squeezed photonic reservoir and when interacting with a one-dimensional waveguide. Using a quantum-state diffusion approach to unravel the emission process, we investigate entanglement and classical correlations along individual quantum trajectories over time. This numerical analysis shows that despite an initial buildup of entanglement and a significant amount of entanglement due to either spin squeezing or dark states at late times, the essential features of the superradiant burst are well described by averages over fully factorizable states. We explain this observation in terms of an almost complete factorization of all 2-local observables, which we identify as a generic property of superradiant decay. Based on this insight, we provide a purely classical theory for the burst in squeezed superradiance, which is both intuitive and exact for a large number of emitters. Moreover, we find that our numerical approach also performs well in the presence of subradiant states, which dominate the slow residual decay of nonuniform ensembles at late times.}, archive = {J_PRL}, author = {Xin H. H. Zhang and Daniel Malz and Peter Rabl}, doi = {10.1103/qbfk-zrzc}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033602}, shortjournal = {Phys. Rev. Lett.}, title = {Unraveling superradiance: Entanglement and mutual information in collective decay}, volume = {135}, year = {2025}, }
• (2025). Quantum interfaces with multilayered superwavelength atomic arrays. PRL, 135(3), 033601. (www)

  @article{ , abstract = {We consider quantum light-matter interfaces comprised of multiple layers of two-dimensional tweezer atomic arrays, wherein the lattice spacings exceed the wavelength of light. While the coupling of light to a single layer of such a “superwavelength” lattice is considerably reduced due to scattering losses to high diffraction orders, we show that the addition of layers can suppress these losses through destructive interference between the layers. Mapping the problem to a 1D model of a quantum interface wherein the coupling efficiency is characterized by a reflectivity, we analyze the latter by developing a geometrical optics formulation, accounting for realistic finite-size arrays. We find that optimized efficiency favors small diffraction-order angles and small interlayer separations, and that the coupling inefficiency for two layers universally scales as with the atom number per layer . We validate our predictions using direct numerical calculations of the scattering reflectivity and the performance of a quantum memory protocol, demonstrating high atom-photon coupling efficiency. This opens the way for various applications in tweezer atomic-array platforms.}, archive = {J_PRL}, author = {Roni Ben-Maimon and Yakov Solomons and Nir Davidson and Ofer Firstenberg and Ephraim Shahmoon}, doi = {10.1103/yw5w-j13k}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033601}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum interfaces with multilayered superwavelength atomic arrays}, volume = {135}, year = {2025}, }
• (2025). Understanding floquet resonances in ultracold quantum gas scattering. PRL, 135(3), 033402. (www)

  @article{ , abstract = {It is demonstrated that the effective scattering length can be highly manipulated via time-periodic driving of a short-range interparticle potential. By developing a Floquet-scattering theory we show that sharp Floquet resonances occur at which the effective interaction can be tuned to very large attractive or repulsive values. The resulting -wave scattering length can be obtained in analytic form and the shape of these resonances is given by a simple formula describing how resonance position and width can be altered by the driving strength. Our approach allows the identification of the underlying physical mechanism of the scattering resonances as Floquet bound states with positive energies, which are dynamically created by the drive. This insight is valuable for a detailed analysis and uncovers a general resource for enhanced or reduced scattering in Floquet systems, as was recently confirmed experimentally.}, archive = {J_PRL}, author = {Christoph Dauer and Axel Pelster and Sebastian Eggert}, doi = {10.1103/47xs-223h}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033402}, shortjournal = {Phys. Rev. Lett.}, title = {Understanding floquet resonances in ultracold quantum gas scattering}, volume = {135}, year = {2025}, }
• (2025). Toward quantum analog simulation of many-body supersymmetry with rydberg atom arrays. PRL, 135(3), 033401. (www)

  @article{ , abstract = {A topological quantum number, the Witten index, characterizes supersymmetric models by probing for zero energy modes and the possibility of supersymmetry breaking. We propose an averaging method to infer the Witten index in quantum analog simulators. Motivated by recent work on Rydberg atoms trapped in optical tweezer arrays, we consider a related supersymmetric XXZ spin model. We show how to infer the Witten index from open-system averaging and numerically demonstrate its topological robustness in this model. Our Letter defines a route for quantum analog simulators to directly identify many-body topological physics.}, archive = {J_PRL}, author = {Hrushikesh Sable and Nathan M. Myers and Vito W. Scarola}, doi = {10.1103/746s-fv7x}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033401}, shortjournal = {Phys. Rev. Lett.}, title = {Toward quantum analog simulation of many-body supersymmetry with rydberg atom arrays}, volume = {135}, year = {2025}, }
• (2025). Electron diffraction imaging of carbon monoxide via K-shell ionization by compton scattering of 20 keV photons. PRL, 135(3), 033203. (www)

  @article{ , abstract = {We report theoretical momentum distributions of electrons ejected from the C and O shells of fixed-in-space CO molecules by Compton scattering of 20 keV photons for different magnitudes and orientations of the photon momentum transfer with respect to the molecular axis. We observe distinct diffraction patterns in our computed momentum distributions, which are governed by the interference of the direct Compton electrons and those which are scattered on the parent and neighboring nuclei. The observed phenomenon is similar to that employed in diffraction imaging using high-energy photoelectrons. It persists after integration over different magnitudes and the orientation of the photon momentum transfer in the molecular frame of reference. A corresponding coincidence experiment confirms our theoretical predictions.}, archive = {J_PRL}, author = {D. M. Haubenreißer and N. M. Novikovskiy and N. Melzer and M. Kircher and A. Pier and L. Kaiser and J. Kruse and N. Anders and J. Stindl and L. Sommerlad and O. D. McGinnis and M. Schmidt and L. Nowak and A. Kügler and I. Dwojak and J. Drnec and F. Trinter and M. S. Schöffler and L. Ph. H. Schmidt and T. Jahnke and R. Dörner and Ph. V. Demekhin}, doi = {10.1103/thh1-8twn}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033203}, shortjournal = {Phys. Rev. Lett.}, title = {Electron diffraction imaging of carbon monoxide via K-shell ionization by compton scattering of 20 keV photons}, volume = {135}, year = {2025}, }
• (2025). Dynamic interference of chirped photoelectrons. PRL, 135(3), 033202. (www)

  @article{ , abstract = {Dynamic interference is an elusive strong-field effect where photoelectrons from intense laser pulses interfere in time, forming rich kinetic energy patterns. Here, we present the first experimental demonstration of isolated dynamic interference using a novel two-color scheme: chirped laser-assisted dynamic interference. Isolation was achieved with a crossed-polarization setup combining an extreme ultraviolet harmonic field and an infrared pulse with tailored spectrotemporal properties. Beyond prior works, our approach enables precise control over interfering trajectories, yielding holographic interference patterns and advancing our understanding of strong-field phenomena.}, archive = {J_PRL}, author = {Federico Vismarra and Mattias Bertolino and Elisa Appi and Marius Plach and Lénárd Gulyás Oldal and Tímea Grósz and Gian Luca Dolso and Vénus Poulain and Daniele Mocci and Giacomo Inzani and Chinmoy Biswas and Massimo De Marco and Gabriele Zeni and Fabio Frassetto and Luca Poletto and Maurizio Reduzzi and Rocio Borrego-Varillas and Hans Jakob Wörner and Zoltán Filus and Imre Seres and Péter Jójárt and Balázs Major and Tamás Csizmadia and Mauro Nisoli and Per Eng-Johnsson and Jan Marcus Dahlström and Matteo Lucchini}, doi = {10.1103/73tl-w87y}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033202}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamic interference of chirped photoelectrons}, volume = {135}, year = {2025}, }
• (2025). High-stability single-ion clock with 5.5×10−19 systematic uncertainty. PRL, 135(3), 033201. (www)

  @article{ , abstract = {We report a single-ion optical atomic clock with a fractional frequency uncertainty of and fractional frequency stability of , based on quantum logic spectroscopy of a single ion. A cotrapped ion provides sympathetic cooling and quantum logic readout of the clock transition. A Rabi probe duration of 1 s, enabled by laser stability transfer from a remote cryogenic silicon cavity across a 3.6 km fiber link, results in a threefold reduction in instability compared to previous clocks. Systematic uncertainties are lower due to an improved ion trap electrical design, which reduces excess micromotion, and a new vacuum system, which reduces collisional shifts. We also perform a direction-sensitive measurement of the ac magnetic field due to the rf ion trap, eliminating systematic uncertainty due to field orientation.}, archive = {J_PRL}, author = {Mason C. Marshall and Daniel A. Rodriguez Castillo and Willa J. Arthur-Dworschack and Alexander Aeppli and Kyungtae Kim and Dahyeon Lee and William Warfield and Joost Hinrichs and Nicholas V. Nardelli and Tara M. Fortier and Jun Ye and David R. Leibrandt and David B. Hume}, doi = {10.1103/hb3c-dk28}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {033201}, shortjournal = {Phys. Rev. Lett.}, title = {High-stability single-ion clock with 5.5×10−19 systematic uncertainty}, volume = {135}, year = {2025}, }
• (2025). Fluctuations and correlations of quark spin in hot and dense QCD matter. PRL, 135(3), 032302. (www)

  @article{ , abstract = {In this Letter, we examine the impact of QCD phase transitions on the quark spin fluctuations and correlations. We propose the quark-antiquark correlation, which relates to the vector meson spin alignment and the correlation, and can be used as a novel probe of the critical end point (CEP) in the QCD phase diagram. Using the Nambu-Jona-Lanisio model, we qualitatively study the properties of quark-antiquark spin correlations. Our findings reveal a peak structure near the CEP of the chiral phase transition, which may serve as an experimental signature of the CEP and account for the non-monotonic behavior of meson alignment at low collision energies observed recently in experiments.}, archive = {J_PRL}, author = {Hao-Lei Chen (陈浩磊 and Wei-jie Fu (付伟杰 and Xu-Guang Huang (黄旭光 and Guo-Liang Ma (马国亮}, doi = {10.1103/g1bh-85h4}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {032302}, shortjournal = {Phys. Rev. Lett.}, title = {Fluctuations and correlations of quark spin in hot and dense QCD matter}, volume = {135}, year = {2025}, }
• (2025). Correspondence between color glass condensate and high-twist formalism. PRL, 135(3), 032301. (www)

  @article{ , abstract = {The color glass condensate (CGC) effective theory and the collinear factorization at high twist (HT) are two well-known frameworks describing perturbative QCD multiple scatterings in nuclear media. It has long been recognized that these two formalisms have their own domain of validity in different kinematic regions. Taking direct photon production in proton-nucleus collisions as an example, we clarify for the first time the relation between CGC and HT at the level of a physical observable. We show that the CGC formalism beyond shock-wave approximation, and with the Landau-Pomeranchuk-Migdal interference effect is consistent with the HT formalism in the transition region where they overlap. Such a unified picture paves the way for mapping out the phase diagram of parton density in nuclear medium from dilute to dense region.}, archive = {J_PRL}, author = {Yu Fu and Zhong-Bo Kang and Farid Salazar and Xin-Nian Wang and Hongxi Xing}, doi = {10.1103/PhysRevLett.135.032301}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {032301}, shortjournal = {Phys. Rev. Lett.}, title = {Correspondence between color glass condensate and high-twist formalism}, volume = {135}, year = {2025}, }
• (2025). Precise determination of the strong coupling constant from dijet cross sections up to the multi-TeV range. PRL, 135(3), 031903. (www)

  @article{ , abstract = {We determine the value of the strong coupling and study its running over a wide range of scales as probed by the dijet production process at hadron colliders, based on a next-to-next-to-leading-order QCD analysis of LHC dijet data. From a large subset of these data a value of is obtained for the strong coupling at the scale of the Z-boson mass , using the invariant mass of the dijet system to select the scale where is probed. The combination of different datasets enhances the reach and precision of the analysis in the multi-TeV range and allows for the first determination of up to scales of . Complementing the LHC data with dijet cross sections measured at the HERA electron–proton collider, the kinematic range is extended to test the running of the strong coupling toward smaller scales. Our results exhibit excellent agreement with predictions based on the renormalization group equation of QCD, and represent a comprehensive test of the asymptotic behavior of QCD, spanning more than three orders of magnitude in energy scale.}, archive = {J_PRL}, author = {Fazila Ahmadova and Daniel Britzger and Xuan Chen and Johannes Gäßler and Aude Gehrmann-De Ridder and Thomas Gehrmann and Nigel Glover and Claire Gwenlan and Gudrun Heinrich and Alexander Huss and Lucas Kunz and João Pires and Klaus Rabbertz and Mark Sutton}, doi = {10.1103/knrv-2r3t}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031903}, shortjournal = {Phys. Rev. Lett.}, title = {Precise determination of the strong coupling constant from dijet cross sections up to the multi-TeV range}, volume = {135}, year = {2025}, }
• (2025). Implication of the existence of JPC=0−− D¯sDK bound state on the nature of ds0*(2317), and a new configuration of exotic state. PRL, 135(3), 031902. (www)

  @article{ , abstract = {The discovery of numerous new hadrons over the past two decades has provided unprecedented opportunities to understand the nonperturbative QCD and hadron structure. The hadronic molecule picture plays an important role in explaining these new hadrons and enriching the configurations of exotic hadronic states. In this Letter, using the model-independent potential extracted from the relevant experimental data, a three-body hadronic molecule is predicted with a mass of . This state shows decoupling to conventional charmonia or the two-body molecular state. It can be regarded as a compelling three-body hadronic molecular candidate. We further demonstrate that the decays could be promising channels for searching for the predicted state in future high-luminosity LHCb runs.}, archive = {J_PRL}, author = {Tian-Wei Wu and Ming-Zhu Liu and Li-Sheng Geng}, doi = {10.1103/3gbb-ms8c}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031902}, shortjournal = {Phys. Rev. Lett.}, title = {Implication of the existence of JPC=0−− D¯sDK bound state on the nature of ds0*(2317), and a new configuration of exotic state}, volume = {135}, year = {2025}, }
• (2025). Search for quasiparticle scattering in the quark-gluon plasma with jet splittings in pp and pb-pb collisions at sNN=5.02 TeV. PRL, 135(3), 031901. (www)

  @article{ , abstract = {The ALICE Collaboration reports measurements of the large relative transverse momentum ( ) component of jet substructure in and Pb-Pb collisions at center-of-mass energy per nucleon pair . Enhancement in the yield of such large- emissions in head-on Pb-Pb collisions is predicted to arise from partonic scattering with quasiparticles of the quark-gluon plasma. The analysis utilizes charged-particle jets reconstructed by the anti- algorithm with resolution parameter in the transverse-momentum interval . The soft drop and dynamical grooming algorithms are used to identify high transverse momentum splittings in the jet shower. Comparison of measurements in Pb-Pb and collisions shows medium-induced narrowing, corresponding to yield suppression of high- splittings, in contrast to the expectation of yield enhancement due to quasiparticle scattering. The measurements are compared to theoretical model calculations incorporating jet modification due to jet-medium interactions (“jet quenching”), both with and without quasiparticle scattering effects. These measurements provide new insight into the underlying mechanisms and theoretical modeling of jet quenching.}, archive = {J_PRL}, author = {ALICE Collaboration and S. Acharya and A. Agarwal and G. Aglieri Rinella and L. Aglietta and M. Agnello and N. Agrawal and Z. Ahammed and S. Ahmad and S. U. Ahn and I. Ahuja and A. Akindinov and V. Akishina and M. Al-Turany and D. Aleksandrov and B. Alessandro and H. M. Alfanda and R. Alfaro Molina and B. Ali and A. Alici and N. Alizadehvandchali and A. Alkin and J. Alme and G. Alocco and T. Alt and A. R. Altamura and I. Altsybeev and J. R. Alvarado and C. O. R. Alvarez and M. N. Anaam and C. Andrei and N. Andreou and A. Andronic and E. Andronov and V. Anguelov and F. Antinori and P. Antonioli and N. Apadula and L. Aphecetche and H. Appelshäuser and C. Arata and S. Arcelli and R. Arnaldi and J. G. M. C. A. Arneiro and I. C. Arsene and M. Arslandok and A. Augustinus and R. Averbeck and D. Averyanov and M. D. Azmi and H. Baba and A. Badalà and J. Bae and Y. W. Baek and X. Bai and R. Bailhache and Y. Bailung and R. Bala and A. Balbino and A. Baldisseri and B. Balis and Z. Banoo and V. Barbasova and F. Barile and L. Barioglio and M. Barlou and B. Barman and G. G. Barnaföldi and L. S. Barnby and E. Barreau and V. Barret and L. Barreto and C. Bartels and K. Barth and E. Bartsch and N. Bastid and S. Basu and G. Batigne and D. Battistini and B. Batyunya and D. Bauri and J. L. Bazo Alba and I. G. Bearden and C. Beattie and P. Becht and D. Behera and I. Belikov and A. D. C. Bell Hechavarria and F. Bellini and R. Bellwied and S. Belokurova and L. G. E. Beltran and Y. A. V. Beltran and G. Bencedi and A. Bensaoula and S. Beole and Y. Berdnikov and A. Berdnikova and L. Bergmann and M. G. Besoiu and L. Betev and P. P. Bhaduri and A. Bhasin and B. Bhattacharjee and L. Bianchi and J. Bielčík and J. Bielčíková and A. P. Bigot and A. Bilandzic and G. Biro and S. Biswas and N. Bize and J. T. Blair and D. Blau and M. B. Blidaru and N. Bluhme and C. Blume and G. Boca and F. Bock and T. Bodova and J. Bok and L. Boldizsár and M. Bombara and P. M. Bond and G. Bonomi and H. Borel and A. Borissov and A. G. Borquez Carcamo and E. Botta and Y. E. M. Bouziani and L. Bratrud and P. Braun-Munzinger and M. Bregant and M. Broz and G. E. Bruno and V. D. Buchakchiev and M. D. Buckland and D. Budnikov and H. Buesching and S. Bufalino and P. Buhler and N. Burmasov and Z. Buthelezi and A. Bylinkin and S. A. Bysiak and J. C. Cabanillas Noris and M. F. T. Cabrera and M. Cai and H. Caines and A. Caliva and E. Calvo Villar and J. M. M. Camacho and P. Camerini and F. D. M. Canedo and S. L. Cantway and M. Carabas and A. A. Carballo and F. Carnesecchi and R. Caron and L. A. D. Carvalho and J. Castillo Castellanos and M. Castoldi and F. Catalano and S. Cattaruzzi and R. Cerri and I. Chakaberia and P. Chakraborty and S. Chandra and S. Chapeland and M. Chartier and S. Chattopadhay and S. Chattopadhyay and M. Chen and T. Cheng and C. Cheshkov and V. Chibante Barroso and D. D. Chinellato and E. S. Chizzali and J. Cho and S. Cho and P. Chochula and Z. A. Chochulska and D. Choudhury and P. Christakoglou and C. H. Christensen and P. Christiansen and T. Chujo and M. Ciacco and C. Cicalo and M. R. Ciupek and G. Clai and F. Colamaria and J. S. Colburn and D. Colella and A. Colelli and M. Colocci and M. Concas and G. Conesa Balbastre and Z. Conesa del Valle and G. Contin and J. G. Contreras and M. L. Coquet and P. Cortese and M. R. Cosentino and F. Costa and S. Costanza and C. Cot and P. Crochet and L. Cunqueiro and M. M. Czarnynoga and A. Dainese and G. Dange and M. C. Danisch and A. Danu and P. Das and S. Das and A. R. Dash and S. Dash and A. De Caro and G. de Cataldo and J. de Cuveland and A. De Falco and D. De Gruttola and N. De Marco and C. De Martin and S. De Pasquale and R. Deb and R. Del Grande and L. Dello Stritto and W. Deng and K. C. Devereaux and P. Dhankher and D. Di Bari and A. Di Mauro and B. Di Ruzza and B. Diab and R. A. Diaz and T. Dietel and Y. Ding and J. Ditzel and R. Divià and Ø. Djuvsland and U. Dmitrieva and A. Dobrin and B. Dönigus and J. M. Dubinski and A. Dubla and P. Dupieux and N. Dzalaiova and T. M. Eder and R. J. Ehlers and F. Eisenhut and R. Ejima and D. Elia and B. Erazmus and F. Ercolessi and B. Espagnon and G. Eulisse and D. Evans and S. Evdokimov and L. Fabbietti and M. Faggin and J. Faivre and F. Fan and W. Fan and A. Fantoni and M. Fasel and A. Feliciello and G. Feofilov and A. Fernández Téllez and L. Ferrandi and M. B. Ferrer and A. Ferrero and C. Ferrero and A. Ferretti and V. J. G. Feuillard and V. Filova and D. Finogeev and F. M. Fionda and E. Flatland and F. Flor and A. N. Flores and S. Foertsch and I. Fokin and S. Fokin and U. Follo and E. Fragiacomo and E. Frajna and U. Fuchs and N. Funicello and C. Furget and A. Furs and T. Fusayasu and J. J. Gaardhøje and M. Gagliardi and A. M. Gago and T. Gahlaut and C. D. Galvan and S. Gami and D. R. Gangadharan and P. Ganoti and C. Garabatos and J. M. Garcia and T. García Chávez and E. Garcia-Solis and C. Gargiulo and P. Gasik and H. M. Gaur and A. Gautam and M. B. Gay Ducati and M. Germain and R. A. Gernhaeuser and C. Ghosh and M. Giacalone and G. Gioachin and S. K. Giri and P. Giubellino and P. Giubilato and A. M. C. Glaenzer and P. Glässel and E. Glimos and D. J. Q. Goh and V. Gonzalez and P. Gordeev and M. Gorgon and K. Goswami and S. Gotovac and V. Grabski and L. K. Graczykowski and E. Grecka and A. Grelli and C. Grigoras and V. Grigoriev and S. Grigoryan and F. Grosa and J. F. Grosse-Oetringhaus and R. Grosso and D. Grund and N. A. Grunwald and G. G. Guardiano and R. Guernane and M. Guilbaud and K. Gulbrandsen and J. J. W. K. Gumprecht and T. Gündem and T. Gunji and W. Guo and A. Gupta and R. Gupta and K. Gwizdziel and L. Gyulai and C. Hadjidakis and F. U. Haider and S. Haidlova and M. Haldar and H. Hamagaki and Y. Han and B. G. Hanley and R. Hannigan and J. Hansen and M. R. Haque and J. W. Harris and A. Harton and M. V. Hartung and H. Hassan and D. Hatzifotiadou and P. Hauer and L. B. Havener and E. Hellbär and H. Helstrup and M. Hemmer and T. Herman and S. G. Hernandez and G. Herrera Corral and S. Herrmann and K. F. Hetland and B. Heybeck and H. Hillemanns and B. Hippolyte and I. P. M. Hobus and F. W. Hoffmann and B. Hofman and G. H. Hong and M. Horst and A. Horzyk and Y. Hou and P. Hristov and P. Huhn and L. M. Huhta and T. J. Humanic and A. Hutson and D. Hutter and M. C. Hwang and R. Ilkaev and M. Inaba and G. M. Innocenti and M. Ippolitov and A. Isakov and T. Isidori and M. S. Islam and S. Iurchenko and M. Ivanov and V. Ivanov and K. E. Iversen and M. Jablonski and B. Jacak and N. Jacazio and P. M. Jacobs and S. Jadlovska and J. Jadlovsky and S. Jaelani and C. Jahnke and M. J. Jakubowska and M. A. Janik and T. Janson and S. Ji and S. Jia and T. Jiang and A. A. P. Jimenez and F. Jonas and D. M. Jones and J. M. Jowett and J. Jung and M. Jung and A. Junique and A. Jusko and J. Kaewjai and P. Kalinak and A. Kalweit and A. Karasu Uysal and D. Karatovic and N. Karatzenis and O. Karavichev and T. Karavicheva and E. Karpechev and M. J. Karwowska and U. Kebschull and M. Keil and B. Ketzer and J. Keul and S. S. Khade and A. M. Khan and S. Khan and A. Khanzadeev and Y. Kharlov and A. Khatun and A. Khuntia and Z. Khuranova and B. Kileng and B. Kim and C. Kim and D. J. Kim and E. J. Kim and J. Kim and M. Kim and S. Kim and T. Kim and K. Kimura and A. Kirkova and S. Kirsch and I. Kisel and S. Kiselev and A. Kisiel and J. P. Kitowski and J. L. Klay and J. Klein and S. Klein and C. Klein-Bösing and M. Kleiner and T. Klemenz and A. Kluge and C. Kobdaj and R. Kohara and T. Kollegger and A. Kondratyev and N. Kondratyeva and J. Konig and S. A. Konigstorfer and P. J. Konopka and G. Kornakov and M. Korwieser and S. D. Koryciak and C. Koster and A. Kotliarov and N. Kovacic and V. Kovalenko and M. Kowalski and V. Kozhuharov and G. Kozlov and I. Králik and A. Kravčáková and L. Krcal and M. Krivda and F. Krizek and K. Krizkova Gajdosova and C. Krug and M. Krüger and D. M. Krupova and E. Kryshen and V. Kučera and C. Kuhn and P. G. Kuijer and T. Kumaoka and D. Kumar and L. Kumar and N. Kumar and S. Kumar and S. Kundu and P. Kurashvili and A. B. Kurepin and A. Kuryakin and S. Kushpil and V. Kuskov and M. Kutyla and A. Kuznetsov and M. J. Kweon and Y. Kwon and S. L. La Pointe and P. La Rocca and A. Lakrathok and M. Lamanna and A. R. Landou and R. Langoy and P. Larionov and E. Laudi and L. Lautner and R. A. N. Laveaga and R. Lavicka and R. Lea and H. Lee and I. Legrand and G. Legras and J. Lehrbach and A. M. Lejeune and T. M. Lelek and R. C. Lemmon and I. León Monzón and M. M. Lesch and E. D. Lesser and P. Lévai and M. Li and P. Li and X. Li and B. E. Liang-Gilman and J. Lien and R. Lietava and I. Likmeta and B. Lim and S. H. Lim and V. Lindenstruth and C. Lippmann and D. H. Liu and J. Liu and G. S. S. Liveraro and I. M. Lofnes and C. Loizides and S. Lokos and J. Lömker and X. Lopez and E. López Torres and C. Lotteau and P. Lu and Z. Lu and F. V. Lugo and J. R. Luhder and M. Lunardon and G. Luparello and Y. G. Ma and M. Mager and A. Maire and E. M. Majerz and M. V. Makariev and M. Malaev and G. Malfattore and N. M. Malik and S. K. Malik and L. Malinina and D. Mallick and N. Mallick and G. Mandaglio and S. K. Mandal and A. Manea and V. Manko and F. Manso and V. Manzari and Y. Mao and R. W. Marcjan and G. V. Margagliotti and A. Margotti and A. Marín and C. Markert and C. F. B. Marquez and P. Martinengo and M. I. Martínez and G. Martínez García and M. P. P. Martins and S. Masciocchi and M. Masera and A. Masoni and L. Massacrier and O. Massen and A. Mastroserio and O. Matonoha and S. Mattiazzo and A. Matyja and F. Mazzaschi and M. Mazzilli and Y. Melikyan and M. Melo and A. Menchaca-Rocha and J. E. M. Mendez and E. Meninno and A. S. Menon and M. W. Menzel and M. Meres and Y. Miake and L. Micheletti and D. Mihai and D. L. Mihaylov and K. Mikhaylov and N. Minafra and D. Miśkowiec and A. Modak and B. Mohanty and M. Mohisin Khan and M. A. Molander and S. Monira and C. Mordasini and D. A. Moreira De Godoy and I. Morozov and A. Morsch and T. Mrnjavac and V. Muccifora and S. Muhuri and J. D. Mulligan and A. Mulliri and M. G. Munhoz and R. H. Munzer and H. Murakami and S. Murray and L. Musa and J. Musinsky and J. W. Myrcha and B. Naik and A. I. Nambrath and B. K. Nandi and R. Nania and E. Nappi and A. F. Nassirpour and V. Nastase and A. Nath and S. Nath and C. Nattrass and M. N. Naydenov and A. Neagu and A. Negru and E. Nekrasova and L. Nellen and R. Nepeivoda and S. Nese and N. Nicassio and B. S. Nielsen and E. G. Nielsen and S. Nikolaev and S. Nikulin and V. Nikulin and F. Noferini and S. Noh and P. Nomokonov and J. Norman and N. Novitzky and P. Nowakowski and A. Nyanin and J. Nystrand and S. Oh and A. Ohlson and V. A. Okorokov and J. Oleniacz and A. Onnerstad and C. Oppedisano and A. Ortiz Velasquez and J. Otwinowski and M. Oya and K. Oyama and Y. Pachmayer and S. Padhan and D. Pagano and G. Paić and S. Paisano-Guzmán and A. Palasciano and I. Panasenko and S. Panebianco and C. Pantouvakis and H. Park and J. Park and J. E. Parkkila and Y. Patley and R. N. Patra and B. Paul and H. Pei and T. Peitzmann and X. Peng and M. Pennisi and S. Perciballi and D. Peresunko and G. M. Perez and Y. Pestov and M. T. Petersen and V. Petrov and M. Petrovici and S. Piano and M. Pikna and P. Pillot and O. Pinazza and L. Pinsky and C. Pinto and S. Pisano and M. Płoskoń and M. Planinic and F. Pliquett and D. K. Plociennik and M. G. Poghosyan and B. Polichtchouk and S. Politano and N. Poljak and A. Pop and S. Porteboeuf-Houssais and V. Pozdniakov and I. Y. Pozos and K. K. Pradhan and S. K. Prasad and S. Prasad and R. Preghenella and F. Prino and C. A. Pruneau and I. Pshenichnov and M. Puccio and S. Pucillo and S. Qiu and L. Quaglia and A. M. K. Radhakrishnan and S. Ragoni and A. Rai and A. Rakotozafindrabe and L. Ramello and F. Rami and M. Rasa and S. S. Räsänen and R. Rath and M. P. Rauch and I. Ravasenga and K. F. Read and C. Reckziegel and A. R. Redelbach and K. Redlich and C. A. Reetz and H. D. Regules-Medel and A. Rehman and F. Reidt and H. A. Reme-Ness and K. Reygers and A. Riabov and V. Riabov and R. Ricci and M. Richter and A. A. Riedel and W. Riegler and A. G. Riffero and M. Rignanese and C. Ripoli and C. Ristea and M. V. Rodriguez and M. Rodríguez Cahuantzi and S. A. Rodríguez Ramírez and K. Røed and R. Rogalev and E. Rogochaya and T. S. Rogoschinski and D. Rohr and D. Röhrich and S. Rojas Torres and P. S. Rokita and G. Romanenko and F. Ronchetti and E. D. Rosas and K. Roslon and A. Rossi and A. Roy and S. Roy and N. Rubini and J. A. Rudolph and D. Ruggiano and R. Rui and P. G. Russek and R. Russo and A. Rustamov and E. Ryabinkin and Y. Ryabov and A. Rybicki and J. Ryu and W. Rzesa and B. Sabiu and S. Sadovsky and J. Saetre and K. Šafařík and S. Saha and B. Sahoo and R. Sahoo and S. Sahoo and D. Sahu and P. K. Sahu and J. Saini and K. Sajdakova and S. Sakai and M. P. Salvan and S. Sambyal and D. Samitz and I. Sanna and T. B. Saramela and D. Sarkar and P. Sarma and V. Sarritzu and V. M. Sarti and M. H. P. Sas and S. Sawan and E. Scapparone and J. Schambach and H. S. Scheid and C. Schiaua and R. Schicker and F. Schlepper and A. Schmah and C. Schmidt and H. R. Schmidt and M. O. Schmidt and M. Schmidt and N. V. Schmidt and A. R. Schmier and R. Schotter and A. Schröter and J. Schukraft and K. Schweda and G. Scioli and E. Scomparin and J. E. Seger and Y. Sekiguchi and D. Sekihata and M. Selina and I. Selyuzhenkov and S. Senyukov and J. J. Seo and D. Serebryakov and L. Serkin and L. Šerkšnytė and A. Sevcenco and T. J. Shaba and A. Shabetai and R. Shahoyan and A. Shangaraev and B. Sharma and D. Sharma and H. Sharma and M. Sharma and S. Sharma and U. Sharma and A. Shatat and O. Sheibani and K. Shigaki and M. Shimomura and J. Shin and S. Shirinkin and Q. Shou and Y. Sibiriak and S. Siddhanta and T. Siemiarczuk and T. F. Silva and D. Silvermyr and T. Simantathammakul and R. Simeonov and B. Singh and K. Singh and R. Singh and S. Singh and V. K. Singh and V. Singhal and T. Sinha and B. Sitar and M. Sitta and T. B. Skaali and G. Skorodumovs and N. Smirnov and R. J. M. Snellings and E. H. Solheim and J. Song and C. Sonnabend and J. M. Sonneveld and F. Soramel and A. B. Soto-Hernandez and R. Spijkers and I. Sputowska and J. Staa and J. Stachel and I. Stan and P. J. Steffanic and T. Stellhorn and S. F. Stiefelmaier and D. Stocco and I. Storehaug and N. J. Strangmann and P. Stratmann and S. Strazzi and A. Sturniolo and C. P. Stylianidis and A. A. P. Suaide and C. Suire and M. Sukhanov and M. Suljic and R. Sultanov and V. Sumberia and S. Sumowidagdo and M. Szymkowski and L. H. Tabares and S. F. Taghavi and G. Taillepied and J. Takahashi and G. J. Tambave and S. Tang and Z. Tang and J. D. Tapia Takaki and N. Tapus and L. A. Tarasovicova and M. G. Tarzila and G. F. Tassielli and A. Tauro and A. Tavira García and G. Tejeda Muñoz and L. Terlizzi and C. Terrevoli and S. Thakur and D. Thomas and A. Tikhonov and N. Tiltmann and A. R. Timmins and M. Tkacik and T. Tkacik and A. Toia and R. Tokumoto and S. Tomassini and K. Tomohiro and N. Topilskaya and M. Toppi and V. V. Torres and A. G. Torres Ramos and A. Trifiró and T. Triloki and A. S. Triolo and S. Tripathy and T. Tripathy and S. Trogolo and V. Trubnikov and W. H. Trzaska and T. P. Trzcinski and C. Tsolanta and R. Tu and A. Tumkin and R. Turrisi and T. S. Tveter and K. Ullaland and B. Ulukutlu and S. Upadhyaya and A. Uras and M. Urioni and G. L. Usai and M. Vala and N. Valle and L. V. R. van Doremalen and M. van Leeuwen and C. A. van Veen and R. J. G. van Weelden and P. Vande Vyvre and D. Varga and Z. Varga and P. Vargas Torres and M. Vasileiou and A. Vasiliev and O. Vázquez Doce and O. Vazquez Rueda and V. Vechernin and E. Vercellin and S. Vergara Limón and R. Verma and L. Vermunt and R. Vértesi and M. Verweij and L. Vickovic and Z. Vilakazi and O. Villalobos Baillie and A. Villani and A. Vinogradov and T. Virgili and M. M. O. Virta and A. Vodopyanov and B. Volkel and M. A. Völkl and S. A. Voloshin and G. Volpe and B. von Haller and I. Vorobyev and N. Vozniuk and J. Vrláková and J. Wan and C. Wang and D. Wang and Y. Wang and Z. Wang and A. Wegrzynek and F. T. Weiglhofer and S. C. Wenzel and J. P. Wessels and J. Wiechula and J. Wikne and G. Wilk and J. Wilkinson and G. A. Willems and B. Windelband and M. Winn and J. R. Wright and W. Wu and Y. Wu and Z. Xiong and R. Xu and A. Yadav and A. K. Yadav and Y. Yamaguchi and S. Yang and S. Yano and E. R. Yeats and Z. Yin and I.-K. Yoo and J. H. Yoon and H. Yu and S. Yuan and A. Yuncu and V. Zaccolo and C. Zampolli and F. Zanone and N. Zardoshti and A. Zarochentsev and P. Závada and N. Zaviyalov and M. Zhalov and B. Zhang and C. Zhang and L. Zhang and M. Zhang and S. Zhang and X. Zhang and Y. Zhang and Z. Zhang and M. Zhao and V. Zherebchevskii and Y. Zhi and D. Zhou and Y. Zhou and J. Zhu and S. Zhu and Y. Zhu and S. C. Zugravel and N. Zurlo}, doi = {10.1103/PhysRevLett.135.031901}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031901}, shortjournal = {Phys. Rev. Lett.}, title = {Search for quasiparticle scattering in the quark-gluon plasma with jet splittings in pp and pb-pb collisions at sNN=5.02 TeV}, volume = {135}, year = {2025}, }
• (2025). Testing the dark origin of neutrino masses with oscillation experiments. PRL, 135(3), 031801. (www)

  @article{ , abstract = {The origin of neutrino masses remains unknown to date. One popular idea involves interactions between neutrinos and ultralight dark matter, described as fields or particles with masses . Due to the large phase-space number density, this type of dark matter exists in coherent states and can be effectively described by an oscillating classical field. As a result, neutrino mass-squared differences undergo field-induced interference in spacetime, potentially generating detectable effects in oscillation experiments. We demonstrate that if , the mechanism becomes sensitive to dark matter density fluctuations, which suppresses the oscillatory behavior of flavor-changing probabilities as a function of neutrino propagation distance in a model-independent way, thereby ruling out this regime. Furthermore, by analyzing data from the Kamioka Liquid Scintillator Antineutrino Detector (KamLAND), a benchmark long-baseline reactor experiment, we show that the hypothesis of a dark origin for the neutrino masses is disfavored for , compared to the case of constant mass values in vacuum. This result holds at more than the level across different datasets and parameter choices. The mass range can be further tested in current and future oscillation experiments by searching for time variations (rather than periodicity) in oscillation parameters.}, archive = {J_PRL}, author = {Andrew Cheek and Luca Visinelli and Hong-Yi Zhang}, doi = {10.1103/wyns-m4y5}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031801}, shortjournal = {Phys. Rev. Lett.}, title = {Testing the dark origin of neutrino masses with oscillation experiments}, volume = {135}, year = {2025}, }
• (2025). Kinematic flow and the emergence of time. PRL, 135(3), 031602. (www)

  @article{ , abstract = {Perhaps the most basic question we can ask about cosmological correlations is how their strength changes as we smoothly vary kinematic parameters. The answer is encoded in differential equations that govern this evolution in kinematic space. In this Letter, we introduce a new perspective on these differential equations. We show that, in the simplified setting of conformally coupled scalars in power-law Friedmann-Robertson-Walker spacetimes, the equations for arbitrary tree-level processes can be obtained from a small number of simple combinatorial rules. While this “kinematic flow” is defined purely in terms of boundary data, it reflects the physics of bulk time evolution. The unexpected regularity of the equations suggests the existence of an autonomously defined mathematical structure from which cosmological correlations and the time evolution of the associated spacetime emerge.}, archive = {J_PRL}, author = {Nima Arkani-Hamed and Daniel Baumann and Aaron Hillman and Austin Joyce and Hayden Lee and Guilherme L. Pimentel}, doi = {10.1103/dsjm-tckw}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031602}, shortjournal = {Phys. Rev. Lett.}, title = {Kinematic flow and the emergence of time}, volume = {135}, year = {2025}, }
• (2025). Complete function space for planar two-loop six-particle scattering amplitudes. PRL, 135(3), 031601. (www)

  @article{ , abstract = {We derive the full system of canonical differential equations for all planar two-loop massless six-particle master integrals and determine analytically the boundary conditions. This fully specifies the solutions, which may be written as Chen iterated integrals. We argue that this is sufficient information for evaluating any scattering amplitude in four dimensions up to the finite part. We support this claim by reducing, for the most complicated integral topologies, integrals with typical Yang-Mills numerators. We use the analytic solutions to the differential equations, together with dihedral symmetry, to provide the full solution space relevant for two-loop six-particle computations. This includes the relevant function alphabet, as well as the independent set of iterated integrals up to weight four. We also provide the answer for all master integrals in terms of iterated integrals that can be readily evaluated numerically. As a proof of concept, we provide a numerical implementation that evaluates the integrals in part of the Euclidean region and validate this against numerical evaluation of the Feynman integrals. Our result removes the bottleneck of the Feynman integral evaluation, paving the way for future analytic evaluations of six-particle scattering amplitudes.}, archive = {J_PRL}, author = {Johannes Henn and Antonela Matijašić and Julian Miczajka and Tiziano Peraro and Yingxuan Xu and Yang Zhang}, doi = {10.1103/zhzd-tj9p}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031601}, shortjournal = {Phys. Rev. Lett.}, title = {Complete function space for planar two-loop six-particle scattering amplitudes}, volume = {135}, year = {2025}, }
• (2025). Cosmic censorship in a dual collider. PRL, 135(3), 031501. (www)

  @article{ , abstract = {We investigate cosmic censorship in anti–de Sitter space in holographic models in which the ground state is described by a good singularity. These include supersymmetric truncations of string/M theory, for which a positive-energy theorem holds. At the boundary, our solutions describe a boost-invariant fluid in which the temperature decreases monotonically with time. On the gravity side, they correspond to black-brane spacetimes with a receding horizon. In classical gravity, curvature invariants at the horizon grow without bound. In the full theory this regime may or may not be reached. In some cases it is avoided by a phase transition to a regular geometry. In others it is reached but the boundary hydrodynamic evolution can be continued, provided the equation of state at parametrically small energies is known. Both cases require the inclusion of finite- or finite-coupling effects.}, archive = {J_PRL}, author = {Marc Aragonès Fontboté and David Mateos and Guillem Pérez Martín and Wilke van der Schee and Javier G. Subils}, doi = {10.1103/dsrc-4yp2}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031501}, shortjournal = {Phys. Rev. Lett.}, title = {Cosmic censorship in a dual collider}, volume = {135}, year = {2025}, }
• (2025). Unstable chords and destructive resonant excitation of black hole quasinormal modes. PRL, 135(3), 031401. (www)

  @article{ , abstract = {The quasinormal mode spectrum of black holes is unstable against small modifications of the radial potential describing massless perturbations. We study how these small modifications affect the convergence of the quasinormal mode expansion and the mode excitation by computing the mode amplitudes from first principles, without relying on any fitting procedure. We show that the decomposition of the prompt ringdown waveform is not unique: small modifications in the radial potential produce new quasinormal mode “basis sets” that can improve the convergence of the quasinormal mode expansion, even capturing the late-time tail. We also study avoided crossings and exceptional points of the Kerr and Kerr–de Sitter spectrum. We show that while the mode amplitude can be resonantly excited, modes that exhibit avoided crossing destructively interfere with each other, so that the prompt ringdown waveform remains stable.}, archive = {J_PRL}, author = {Naritaka Oshita and Emanuele Berti and Vitor Cardoso}, doi = {10.1103/ht2n-vvvh}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031401}, shortjournal = {Phys. Rev. Lett.}, title = {Unstable chords and destructive resonant excitation of black hole quasinormal modes}, volume = {135}, year = {2025}, }
• (2025). Search for extremely-high-energy neutrinos and first constraints on the ultrahigh-energy cosmic-ray proton fraction with IceCube. PRL, 135(3), 031001. (www)

  @article{ , abstract = {We present a search for the diffuse extremely-high-energy neutrino flux using 12.6 years of IceCube data. The nonobservation of neutrinos with energies well above 10 PeV constrains the all-flavor neutrino flux at to a level of , the most stringent limit to date. Using these data, we constrain the proton fraction of ultrahigh-energy cosmic rays (UHECRs) above to be (at 90% CL) if the cosmological evolution of the sources is comparable to or stronger than the star formation rate. This is the first result to disfavor the “proton-only” hypothesis for UHECR in this evolution regime using neutrino data. This result complements direct air-shower measurements by being insensitive to uncertainties associated with hadronic interaction models. We also evaluate the tension between IceCube’s nonobservation and the KM3NeT neutrino candidate (KM3-230213A), finding it to be based on a joint-livetime fit between neutrino datasets.}, archive = {J_PRL}, author = {IceCube Collaboration and R. Abbasi and M. Ackermann and J. Adams and S. K. Agarwalla and J. A. Aguilar and M. Ahlers and J. M. Alameddine and N. M. Amin and K. Andeen and C. Argüelles and Y. Ashida and S. Athanasiadou and S. N. Axani and R. Babu and X. Bai and A. Balagopal V and M. Baricevic and S. W. Barwick and S. Bash and V. Basu and R. Bay and J. J. Beatty and J. Becker Tjus and J. Beise and C. Bellenghi and S. BenZvi and D. Berley and E. Bernardini and D. Z. Besson and E. Blaufuss and L. Bloom and S. Blot and F. Bontempo and J. Y. Book Motzkin and C. Boscolo Meneguolo and S. Böser and O. Botner and J. Böttcher and J. Braun and B. Brinson and Z. Brisson-Tsavoussis and J. Brostean-Kaiser and L. Brusa and R. T. Burley and D. Butterfield and M. A. Campana and I. Caracas and K. Carloni and J. Carpio and S. Chattopadhyay and N. Chau and Z. Chen and D. Chirkin and S. Choi and B. A. Clark and A. Coleman and P. Coleman and G. H. Collin and A. Connolly and J. M. Conrad and R. Corley and D. F. Cowen and C. De Clercq and J. J. DeLaunay and D. Delgado and S. Deng and A. Desai and P. Desiati and K. D. de Vries and G. de Wasseige and T. DeYoung and A. Diaz and J. C. Díaz-Vélez and P. Dierichs and M. Dittmer and A. Domi and L. Draper and H. Dujmovic and D. Durnford and K. Dutta and M. A. DuVernois and T. Ehrhardt and L. Eidenschink and A. Eimer and P. Eller and E. Ellinger and S. El Mentawi and D. Elsässer and R. Engel and H. Erpenbeck and W. Esmail and J. Evans and P. A. Evenson and K. L. Fan and K. Fang and K. Farrag and A. R. Fazely and A. Fedynitch and N. Feigl and S. Fiedlschuster and C. Finley and L. Fischer and D. Fox and A. Franckowiak and S. Fukami and P. Fürst and J. Gallagher and E. Ganster and A. Garcia and M. Garcia and G. Garg and E. Genton and L. Gerhardt and A. Ghadimi and C. Girard-Carillo and C. Glaser and T. Glüsenkamp and J. G. Gonzalez and S. Goswami and A. Granados and D. Grant and S. J. Gray and S. Griffin and S. Griswold and K. M. Groth and D. Guevel and C. Günther and P. Gutjahr and C. Ha and C. Haack and A. Hallgren and L. Halve and F. Halzen and L. Hamacher and H. Hamdaoui and M. Ha Minh and M. Handt and K. Hanson and J. Hardin and A. A. Harnisch and P. Hatch and A. Haungs and J. Häußler and K. Helbing and J. Hellrung and J. Hermannsgabner and L. Heuermann and N. Heyer and S. Hickford and A. Hidvegi and C. Hill and G. C. Hill and R. Hmaid and K. D. Hoffman and S. Hori and K. Hoshina and M. Hostert and W. Hou and T. Huber and K. Hultqvist and M. Hünnefeld and R. Hussain and K. Hymon and A. Ishihara and W. Iwakiri and M. Jacquart and S. Jain and O. Janik and M. Jansson and M. Jeong and M. Jin and B. J. P. Jones and N. Kamp and D. Kang and W. Kang and X. Kang and A. Kappes and D. Kappesser and L. Kardum and T. Karg and M. Karl and A. Karle and A. Katil and U. Katz and M. Kauer and J. L. Kelley and M. Khanal and A. Khatee Zathul and A. Kheirandish and J. Kiryluk and S. R. Klein and Y. Kobayashi and A. Kochocki and R. Koirala and H. Kolanoski and T. Kontrimas and L. Köpke and C. Kopper and D. J. Koskinen and P. Koundal and M. Kowalski and T. Kozynets and N. Krieger and J. Krishnamoorthi and T. Krishnan and K. Kruiswijk and E. Krupczak and A. Kumar and E. Kun and N. Kurahashi and N. Lad and C. Lagunas Gualda and M. Lamoureux and M. J. Larson and F. Lauber and J. P. Lazar and K. Leonard DeHolton and A. Leszczyńska and J. Liao and M. Lincetto and Y. T. Liu and M. Liubarska and C. Love and L. Lu and F. Lucarelli and W. Luszczak and Y. Lyu and J. Madsen and E. Magnus and K. B. M. Mahn and Y. Makino and E. Manao and S. Mancina and A. Mand and W. Marie Sainte and I. C. Mariş and S. Marka and Z. Marka and M. Marsee and I. Martinez-Soler and R. Maruyama and F. Mayhew and F. McNally and J. V. Mead and K. Meagher and S. Mechbal and A. Medina and M. Meier and Y. Merckx and L. Merten and J. Mitchell and T. Montaruli and R. W. Moore and Y. Morii and R. Morse and M. Moulai and T. Mukherjee and R. Naab and M. Nakos and U. Naumann and J. Necker and A. Negi and L. Neste and M. Neumann and H. Niederhausen and M. U. Nisa and K. Noda and A. Noell and A. Novikov and A. Obertacke Pollmann and V. O’Dell and A. Olivas and R. Orsoe and J. Osborn and E. O’Sullivan and V. Palusova and H. Pandya and N. Park and G. K. Parker and V. Parrish and E. N. Paudel and L. Paul and C. Pérez de los Heros and T. Pernice and J. Peterson and A. Pizzuto and M. Plum and A. Pontén and Y. Popovych and M. Prado Rodriguez and B. Pries and R. Procter-Murphy and G. T. Przybylski and L. Pyras and C. Raab and J. Rack-Helleis and N. Rad and M. Ravn and K. Rawlins and Z. Rechav and A. Rehman and E. Resconi and S. Reusch and W. Rhode and B. Riedel and A. Rifaie and E. J. Roberts and S. Robertson and S. Rodan and M. Rongen and A. Rosted and C. Rott and T. Ruhe and L. Ruohan and D. Ryckbosch and I. Safa and J. Saffer and D. Salazar-Gallegos and P. Sampathkumar and A. Sandrock and M. Santander and S. Sarkar and J. Savelberg and P. Savina and P. Schaile and M. Schaufel and H. Schieler and S. Schindler and L. Schlickmann and B. Schlüter and F. Schlüter and N. Schmeisser and T. Schmidt and J. Schneider and F. G. Schröder and L. Schumacher and S. Schwirn and S. Sclafani and D. Seckel and L. Seen and M. Seikh and M. Seo and S. Seunarine and P. Sevle Myhr and R. Shah and S. Shefali and N. Shimizu and M. Silva and B. Skrzypek and B. Smithers and R. Snihur and J. Soedingrekso and A. Søgaard and D. Soldin and P. Soldin and G. Sommani and C. Spannfellner and G. M. Spiczak and C. Spiering and J. Stachurska and M. Stamatikos and T. Stanev and T. Stezelberger and T. Stürwald and T. Stuttard and G. W. Sullivan and I. Taboada and S. Ter-Antonyan and A. Terliuk and M. Thiesmeyer and W. G. Thompson and J. Thwaites and S. Tilav and K. Tollefson and C. Tönnis and S. Toscano and D. Tosi and A. Trettin and M. A. Unland Elorrieta and A. K. Upadhyay and K. Upshaw and A. Vaidyanathan and N. Valtonen-Mattila and J. Vandenbroucke and N. van Eijndhoven and D. Vannerom and J. van Santen and J. Vara and F. Varsi and J. Veitch-Michaelis and M. Venugopal and M. Vereecken and S. Vergara Carrasco and S. Verpoest and D. Veske and A. Vijai and C. Walck and A. Wang and C. Weaver and P. Weigel and A. Weindl and J. Weldert and A. Y. Wen and C. Wendt and J. Werthebach and M. Weyrauch and N. Whitehorn and C. H. Wiebusch and D. R. Williams and L. Witthaus and M. Wolf and G. Wrede and X. W. Xu and J. P. Yanez and E. Yildizci and S. Yoshida and R. Young and F. Yu and S. Yu and T. Yuan and A. Zegarelli and S. Zhang and Z. Zhang and P. Zhelnin and P. Zilberman and M. Zimmerman}, doi = {10.1103/PhysRevLett.135.031001}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {031001}, shortjournal = {Phys. Rev. Lett.}, title = {Search for extremely-high-energy neutrinos and first constraints on the ultrahigh-energy cosmic-ray proton fraction with IceCube}, volume = {135}, year = {2025}, }
• (2025). Enhanced quantum frequency estimation by nonlinear scrambling. PRL, 135(3), 030802. (www)

  @article{ , abstract = {Frequency estimation, a cornerstone of basic and applied sciences, has been significantly enhanced by quantum sensing strategies. Despite breakthroughs in quantum-enhanced frequency estimation, key challenges remain: static probes limit flexibility, and the interplay between resource efficiency, sensing precision, and potential enhancements from nonlinear probes remains not fully understood. In this Letter, we show that dynamically encoding an unknown frequency in a nonlinear quantum electromagnetic field can significantly improve frequency estimation. To provide a fair comparison of resources, we define the energy cost as the figure of merit for our sensing strategy. We further show that specific higher-order nonlinear processes lead to nonlinear-enhanced frequency estimation. This enhancement results from quantum scrambling, where local quantum information spreads across a larger portion of the Hilbert space. We quantify this effect using the Wigner-Yanase skew information, which measures the degree of noncommutativity in the Hamiltonian structure. Our Letter sheds light on the connection between Wigner-Yanase skew information and quantum sensing, providing a direct method to optimize nonlinear quantum probes.}, archive = {J_PRL}, author = {Victor Montenegro and Sara Dornetti and Alessandro Ferraro and Matteo G. A. Paris}, doi = {10.1103/39bt-37yl}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030802}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced quantum frequency estimation by nonlinear scrambling}, volume = {135}, year = {2025}, }
• (2025). Complete self-testing of a system of remote superconducting qubits. PRL, 135(3), 030801. (www)

  @article{ , abstract = {Self-testing protocols enable the certification of quantum systems in a device-independent manner, i.e., without knowledge of the inner workings of the quantum devices under test. Here, we demonstrate this high standard for characterization routines with superconducting circuits, a prime platform for building large-scale quantum computing systems. We first develop the missing theory allowing for the self-testing of Pauli measurements. We then self-test Bell pair generation and measurements at the same time, performing a complete self-test in a system composed of two entangled superconducting circuits operated at a separation of 30 m. In an experiment based on 17 million trials, we measure an average CHSH (Clauser-Horne-Shimony-Holt) value of 2.236. Without relying on additional assumptions on the experimental setup, we certify an average Bell state fidelity of at least 58.9% and an average measurement fidelity of at least 89.5% in a device-independent manner, both with 99% confidence. This enables applications in the field of distributed quantum computing and communication with superconducting circuits, such as delegated quantum computing.}, archive = {J_PRL}, author = {Simon Storz and Anatoly Kulikov and Josua D. Schär and Victor Barizien and Xavier Valcarce and Florence Berterottière and Nicolas Sangouard and Jean-Daniel Bancal and Andreas Wallraff}, doi = {10.1103/nv7d-k3wr}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030801}, shortjournal = {Phys. Rev. Lett.}, title = {Complete self-testing of a system of remote superconducting qubits}, volume = {135}, year = {2025}, }
• (2025). Strongly interacting fermions are nontrivial yet nonglassy. PRL, 135(3), 030602. (www)

  @article{ , abstract = {Random spin systems at low temperatures are glassy and feature computational hardness in finding low-energy states. We study the random all-to-all interacting fermionic Sachdev-Ye-Kitaev model and prove that, in contrast, the low-energy states have polynomial circuit depth, yet the annealed and quenched free energies agree to polynomially inverse low temperatures, ruling out a glassy phase transition in this sense. These results are derived by showing that fermionic and spin systems significantly differ in their “commutation index,” which quantifies the noncommutativity of Hamiltonian terms. Our results suggest that low-temperature strongly interacting fermions, unlike spins, belong in a classically nontrivial yet quantumly easy phase.}, archive = {J_PRL}, author = {Eric R. Anschuetz and Chi-Fang Chen and Bobak T. Kiani and Robbie King}, doi = {10.1103/cbqf-d24r}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030602}, shortjournal = {Phys. Rev. Lett.}, title = {Strongly interacting fermions are nontrivial yet nonglassy}, volume = {135}, year = {2025}, }
• (2025). Beating the natural grover bound for low-energy estimation and state preparation. PRL, 135(3), 030601. (www)

  @article{ , abstract = {Estimating ground state energies of many-body Hamiltonians is a central task in many areas of quantum physics. In this Letter, we give quantum algorithms which, given any -body Hamiltonian , compute an estimate for the ground state energy and prepare a quantum state achieving said energy, respectively. Specifically, for any , our algorithms return, with high probability, an estimate of the ground state energy of within additive error , or a quantum state with the corresponding energy. Here, is the total strength of all interaction terms, which in general is extensive in the system size. Our approach makes no assumptions about the geometry or spatial locality of interaction terms of the input Hamiltonian and thus handles even long-range or all-to-all interactions, such as in quantum chemistry, where lattice-based techniques break down. In this fully general setting, the run-time of our algorithms scales as for , yielding the first quantum algorithms for low-energy estimation breaking a standard square root Grover speedup for unstructured search. The core of our approach is remarkably simple, and relies on showing that an extensive fraction of the interactions can be neglected with a controlled error. What this ultimately implies is that even arbitrary -local Hamiltonians have structure in their low energy space, in the form of an exponential-dimensional low energy subspace.}, archive = {J_PRL}, author = {Harry Buhrman and Sevag Gharibian and Zeph Landau and François Le Gall and Norbert Schuch and Suguru Tamaki}, doi = {10.1103/29qw-bssx}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030601}, shortjournal = {Phys. Rev. Lett.}, title = {Beating the natural grover bound for low-energy estimation and state preparation}, volume = {135}, year = {2025}, }
• (2025). Failure of the conformal-map method for relativistic quantum billiards. PRL, 135(3), 030401. (www)

  @article{ , abstract = {In H. Xu et al. [ Phys. Rev. Lett. 110 , 064102 (2013) ], a numerical method is introduced—an extension of the conformal-map method of Robnik [ J. Phys. A 17 , 1049 (1984) ] for nonrelativistic quantum billiards—for the quantization of relativistic neutrino billiards consisting of a massless noninteracting spin- particle confined to a two-dimensional domain. We demonstrate in this Letter that this method does not provide solutions of the associated Weyl (Dirac) equation, nor does it fulfill the boundary conditions imposed on the spinor eigenfunctions to ensure confinement of the particle to the domain of the billiard. We review in detail the wave equation, boundary conditions, and quantization of neutrino billiards and derivation of relevant equations to make the proof comprehensible for the general reader. Our results are corroborated with numerical ones for nonrelativistic and relativistic quantum billiards whose shapes depend on a parameter, which allows the study of the properties of their eigenstates as the classical dynamics experiences a transition from regular to chaotic dynamics.}, archive = {J_PRL}, author = {Barbara Dietz}, doi = {10.1103/vj94-kc98}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030401}, shortjournal = {Phys. Rev. Lett.}, title = {Failure of the conformal-map method for relativistic quantum billiards}, volume = {135}, year = {2025}, }
• (2025). Quantum correlations cannot be reproduced with a finite number of measurements in any no-signaling theory. PRL, 135(3), 030201. (www)

  @article{ , abstract = {We show, for any finite , that there exist quantum correlations obtained from performing dichotomic quantum measurements in a bipartite Bell scenario, which cannot be reproduced by mixtures of measurement devices with at most ( ) incompatible measurements across different partitions in any no-signaling theory. That is, it requires for any no-signaling theory an unbounded number of measurements to reproduce the predictions of quantum theory. We prove our results by showing that there exist linear Bell inequalities that have to be obeyed by any no-signaling theory involving only ( )-wise incompatible measurements and show explicitly how these can be violated in quantum theory. Finally, we discuss the relation of our work to previous works ruling out alternatives to quantum theory with some kind of bounded degree of freedom and consider the experimental verifiability of our results.}, archive = {J_PRL}, author = {Lucas Tendick}, doi = {10.1103/7vjx-62ng}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum correlations cannot be reproduced with a finite number of measurements in any no-signaling theory}, volume = {135}, year = {2025}, }
• (2025). Essay: Using machine learning for antibiotic discovery. PRL, 135(3), 030001. (www)

  @article{ , abstract = {Antimicrobial resistance is a critical global health challenge and one of the World Health Organization’s top ten public health threats. The alarming rise of drug-resistant pathogens threatens to usher in a postantibiotic era where common infections could once again become fatal. Despite the urgency, traditional discovery methods are time-consuming, expensive, and insufficient to keep pace with rapidly evolving resistance. Recent advances in machine learning (ML) and artificial intelligence (AI) present a transformative alternative, enabling the rapid identification of potential candidate antibiotics in a fraction of the time required by conventional methods. In this Essay, we discuss how ML and AI significantly accelerate antibiotic discovery, drawing on previous works and insights in this emerging field. We also consider the promises and challenges of this emerging area and speculate on its evolution in the coming years, highlighting the potential contributions from the physics community.}, archive = {J_PRL}, author = {Cesar de la Fuente-Nunez and James J. Collins}, doi = {10.1103/y3fg-s9vg}, journal = {Physical Review Letters}, month = {7}, number = {3}, pages = {030001}, shortjournal = {Phys. Rev. Lett.}, title = {Essay: Using machine learning for antibiotic discovery}, volume = {135}, year = {2025}, }
• (2025). Twist-induced networking and fast propagation of defects in three-dimensional active nematics. PRL, 135(2), 028302. (www)

  @article{ , abstract = {Owing to the sustained energy input, active nematics can spontaneously generate topological defects, which generally undergo chaotic motions ruled by active hydrodynamics. Here, we combine theory and simulations to investigate the structure and dynamics of topological defects in three-dimensional (3D) active nematics under boundary twisting, similar to twisted bilayer graphene. We show that increasing twist angle will lead to the transition of defect patterns from wedge-twist defect loops to pure-twist defect lines. These defect lines can organize into ordered networks, which oscillate persistently and propagate as a wave. Intriguingly, the wave speed of defect networks is significantly faster than that of local active flows, in contrast to the traditional active defects. We identify that the fast propagation of 3D topological defects results from the activity-driven defect pattern transition and the vertical oscillations mediated by the nematic elasticity. These findings reveal the marked influence of boundary perturbations on active nematics and could also provide a simple strategy to program 3D defect dynamics.}, archive = {J_PRL}, author = {Zhong-Yi Li and Anna Dai and Shao-Zhen Lin and Rui Zhang and Bo Li}, doi = {10.1103/j6tt-s3xh}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {028302}, shortjournal = {Phys. Rev. Lett.}, title = {Twist-induced networking and fast propagation of defects in three-dimensional active nematics}, volume = {135}, year = {2025}, }
• (2025). Colloidal model for investigating optimal efficiency in weakly coupled ratchet motors. PRL, 135(2), 028301. (www)

  @article{ , abstract = {We investigate the transport of superparamagnetic colloidal particles along self-assembled tracks using a periodically applied magnetic field as a model for ratchetlike mechanisms. Through video microscopy and simulations, we examine how different factors influence transport efficiency. The findings reveal that processive motion can be achieved without residual attraction, with optimal transport efficiency governed by the combined effects of particle size ratios, actuation frequency, track roughness, and asymmetry in the applied potential. Additionally, we explore alternative strategies, including weak residual attraction and alternating magnetic fields, to further enhance efficiency. These findings provide valuable insights for the development of synthetic micro- and nanomotors with potential applications in drug delivery and environmental remediation.}, archive = {J_PRL}, author = {José Martín-Roca and Laura Izquierdo Solis and Fernando Martínez Pedrero and Pau Casadejust and Ignacio Pagonabarraga and Carles Calero}, doi = {10.1103/sjss-vkqv}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {028301}, shortjournal = {Phys. Rev. Lett.}, title = {Colloidal model for investigating optimal efficiency in weakly coupled ratchet motors}, volume = {135}, year = {2025}, }
• (2025). Thermodynamic origin of multistep polymer crystallization. PRL, 135(2), 028101. (www)

  @article{ , abstract = {We combine atomistic simulations and theories to predict the free energy of polymer crystallization, which highlights the roles of backbone stiffness and orientational coupling between monomers in the formation of metastable mesophases. We show that polyethylene (PE) with sufficient backbone stiffness in the conformationally disordered state can develop uniaxial order through metastable nematic and rotator phases before conformationally ordering into the crystalline state. Isotactic polypropylene (iPP), with a lower backbone stiffness, undergoes one-step crystallization directly from the isotropic phase to the crystalline phase. The predicted bulk phase transition temperatures for iPP and PE of different molecular weights agree well with experiments.}, archive = {J_PRL}, author = {Wenlin Zhang (张文麟}, doi = {10.1103/bzpn-qpj5}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {028101}, shortjournal = {Phys. Rev. Lett.}, title = {Thermodynamic origin of multistep polymer crystallization}, volume = {135}, year = {2025}, }
• (2025). Aqueous ion mobility over a broad concentration range. PRL, 135(2), 028002. (www)

  @article{ , abstract = {For concentrations between dilute and the highly concentrated limit of almost 5 M, we compare our explicit-water molecular dynamics simulations of (which dissociates into anions relevant to biochemical processes and cations relevant to battery technology) to our pulsed-field gradient NMR measurements of ion diffusion, and find compensation between electrostatic and osmotic forces. The significance is that, noticing that the Kirkwood equation holds when using its exact solution but seemingly is violated when making the traditional approximation of using total force relaxation time in place of the memory relaxation time, we explain slower translational diffusion with increasing ion concentration as a dynamical effect arising from growing memory relaxation time. Physically, 2 orders of magnitude separate the timescales of electrostatic and osmotic forces from the total force such that dynamical correlations between force components lead to concentration-independent total force variance and force relaxation time.}, archive = {J_PRL}, author = {Tian Huang and Setare Mostajabi Sarhangi and Steve Granick and Dmitry V. Matyushov}, doi = {10.1103/dvck-px3k}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {028002}, shortjournal = {Phys. Rev. Lett.}, title = {Aqueous ion mobility over a broad concentration range}, volume = {135}, year = {2025}, }
• (2025). Observing the mobile surface layer of water during vapor deposition and its impact on structure. PRL, 135(2), 028001. (www)

  @article{ , abstract = {Historically, amorphous solid water (ASW) films have been created by physical vapor deposition both naturally on interstellar particles and in the laboratory. The present study focuses on the role of the mobile surface layer, which can be observed during vapor deposition and characterized by dielectric relaxation techniques. It is shown that the mobility of the surface layer can determine whether an as-deposited film is porous (p-ASW), collapsed (c-ASW), or crystallized to cubic ice ( ). The latter case occurs when the fictive temperature of the surface reaches deep into the so-called “no man’s land”, whereas the actual temperature remains below that of the glass transition at . The dynamics of this surface layer is independent of deposition temperature in the 15 to 120 K range.}, archive = {J_PRL}, author = {Erik Thoms and Jan P. Gabriel and Ranko Richert}, doi = {10.1103/hwwg-gscf}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {028001}, shortjournal = {Phys. Rev. Lett.}, title = {Observing the mobile surface layer of water during vapor deposition and its impact on structure}, volume = {135}, year = {2025}, }
• (2025). Deep generative modeling of the canonical ensemble with differentiable thermal properties. PRL, 135(2), 027301. (www)

  @article{ , abstract = {It is a long-standing challenge to accurately and efficiently compute thermodynamic quantities of many-body systems at thermal equilibrium. The conventional methods, e.g., Markov chain Monte Carlo, require many steps to equilibrate. The recently developed deep learning methods can perform direct sampling, but only work at a single trained temperature point and risk biased sampling. Here, we propose a variational method for canonical ensembles with differentiable temperatures, which gives thermodynamic quantities as continuous functions of temperature akin to an analytical solution. The proposed method is a general framework that works with any tractable density generative model. At optimal, the model is theoretically guaranteed to be the unbiased Boltzmann distribution. We validated our method by calculating phase transitions in the Ising and XY models, demonstrating that our direct-sampling simulations are as accurate as Markov chain Monte Carlo methods but more efficient. Moreover, our differentiable free energy aligns closely with the exact one to the second-order derivative, indicating that the variational model captures the subtle thermal transitions at the phase transitions. This functional dependence on external parameters is a fundamental advancement in combining the exceptional fitting ability of deep learning with rigorous physical analysis.}, archive = {J_PRL}, author = {Shuo-Hui Li and Yao-Wen Zhang and Ding Pan}, doi = {10.1103/8wx7-kyx8}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {027301}, shortjournal = {Phys. Rev. Lett.}, title = {Deep generative modeling of the canonical ensemble with differentiable thermal properties}, volume = {135}, year = {2025}, }
• (2025). Experimental realization of special-unitary operations in classical mechanics by nonadiabatic evolutions. PRL, 135(2), 027201. (www)

  @article{ , abstract = {Artificial classical wave systems such as wave crystals and metamaterials have demonstrated promising capabilities in simulating a wide range of quantum mechanical phenomena. Yet some gaps between quantum and classical worlds are generally considered fundamental and difficult to bridge. Dynamics obeying special unitary groups, e.g., electronic spins described by SU(2), color symmetries of fundamental particles described by SU(3), are such examples. In this Letter, we present the experimental realization of universal SU(2) and SU(3) dynamic operations in classical mechanical oscillator systems with temporally modulated coupling terms. Our approach relies on the sequential execution of nonadiabatic holonomic evolutions, which are typically used in constructing quantum-logic gates. The method is swift and purely geometric and can be extended to realize more sophisticated dynamic operations. Our results open a new way for studying and simulating quantum phenomena in classical systems.}, archive = {J_PRL}, author = {Congwei Lu and Xulong Wang and Guancong Ma}, doi = {10.1103/24zr-pl3m}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {027201}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental realization of special-unitary operations in classical mechanics by nonadiabatic evolutions}, volume = {135}, year = {2025}, }
• (2025). Quantum confining excitons with an electrostatic moiré superlattice. PRL, 135(2), 026901. (www)

  @article{ , abstract = {Quantum confining excitons has been a persistent challenge in the pursuit of strong exciton interactions and quantum light generation. Unlike electrons, which can be readily controlled via electric fields, imposing strong nanoscale potentials on excitons to enable quantum confinement has proven challenging. In this Letter, we utilize piezoelectric force microscopy to image the domain structures of twisted hexagonal boron nitride ( ), revealing evidence of strong in-plane electric fields at the domain boundaries. By placing a monolayer only 1 to 2 nm away from the twisted interface, we observe energy splitting of neutral excitons and Fermi polarons by several millielectronvolts at the moiré domain boundaries. We attribute such observations to excitons confined in a nanoscale one-dimensional electrostatic potential created by the strong in-plane electric fields at the moiré domain boundaries. Intriguingly, this 1D quantum confinement results in pronounced polarization anisotropy in the excitons’ reflection and emission, persistent to temperatures as high as . These findings open new avenues for exploring and controlling strongly interacting excitons for classical and quantum optoelectronics.}, archive = {J_PRL}, author = {Liuxin Gu and Lifu Zhang and Sam Felsenfeld and Beini Gao and Rundong Ma and Suji Park and Houk Jang and Takashi Taniguchi and Kenji Watanabe and You Zhou}, doi = {10.1103/tyr4-9z16}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026901}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum confining excitons with an electrostatic moiré superlattice}, volume = {135}, year = {2025}, }
• (2025). Fluctuations and correlations of local topological order parameters in disordered two-dimensional topological insulators. PRL, 135(2), 026603. (www)

  @article{ , abstract = {Two-dimensional topological insulators are characterized by an insulating bulk and conductive edge states protected by the nontrivial topology of the bulk electronic structure. They remain robust against moderate disorder until Anderson localization occurs and destroys the topological phase. Interestingly, disorder can also induce a topological phase—known as a topological Anderson insulator—starting from an otherwise pristine trivial phase. While topological invariants are generally regarded as global quantities, we argue that space-resolved topological markers can act as local order parameters, revealing the role of fluctuations and correlations in the local topology under Anderson disorder and vacancies. With this perspective, we perform numerical simulations of disorder-driven topological phase transitions in the Haldane and Kane-Mele models, using supercells with both open and periodic boundary conditions. We find that short-scale fluctuations of topological markers vanish upon coarse graining, except at the topological phase transition, where their correlation length peaks and large-scale fluctuations remain. Notably, such a topological correlation function is characterized by critical exponents that appear universal across disorder types, yet they can resolve different topological phase transitions.}, archive = {J_PRL}, author = {Roberta Favata and Nicolas Baù and Antimo Marrazzo}, doi = {10.1103/h4d8-3lw1}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026603}, shortjournal = {Phys. Rev. Lett.}, title = {Fluctuations and correlations of local topological order parameters in disordered two-dimensional topological insulators}, volume = {135}, year = {2025}, }
• (2025). Internal entropy of non-abelian anyons from heat current through a tunneling barrier. PRL, 135(2), 026602. (www)

  @article{ , abstract = {We demonstrate that the effective internal entropy of quasiparticles within the non-Abelian fractional quantum Hall effect manifests in the heat current through a tunneling barrier. We derive the electric current and heat current resulting from voltage and heat biases of the junction, taking into account the quasiparticles’ internal entropy. We find that when the tunneling processes are dominated by quasiparticle tunneling of one type of charge, the effective internal entropy can be inferred from the measurement of the heat current and the charge current. Our methods may be used to conclusively identify non-Abelian quasiparticles, such as the anyons that emerge in the ν = 5 / 2 fractional quantum Hall state.}, archive = {J_PRL}, author = {Noam Schiller and Hiromi Ebisu and Gil Refael and Yuval Oreg}, doi = {10.1103/v3lq-ptgd}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026602}, shortjournal = {Phys. Rev. Lett.}, title = {Internal entropy of non-abelian anyons from heat current through a tunneling barrier}, volume = {135}, year = {2025}, }
• (2025). Magnetic field induced quantum metric dipole in dirac semimetal Cd3As2. PRL, 135(2), 026601. (www)

  @article{ , abstract = {The quantum geometry, comprising Berry curvature and quantum metric, plays a fundamental role in governing electron transport phenomena in solids. Recent studies show that the quantum metric dipole drives scattering-free nonlinear Hall effect in topological antiferromagnets, prompting the questions of whether this effect can occur in nonmagnetic systems and be externally tuned by a magnetic field. Our work addresses these frontiers by demonstrating that the quantum metric dipole is actively tuned by an external magnetic field to generate a time-reversal-odd nonlinear Hall response in a nonmagnetic topological Dirac semimetal . Alongside the well-known chiral-anomaly-induced negative longitudinal magnetoresistance, an exotic nonlinear planar Hall effect emerges with increasing magnetic field. Careful scaling analysis indicates that this nonlinear planar Hall effect is controlled by the magnetic-field-modulated quantum metric dipole. Constructing a effective model of the Dirac bands under Zeeman and orbital coupling, we derive the evolution of the quantum metric dipole as a function of the magnetic field, providing a comprehensive explanation of the experimental results. Our results establish a band-structure-based strategy for engineering nonlinear magnetotransport in nonmagnetic materials via the quantum metric dipole, opening a pathway toward magnetic-field–tunable nonlinear quantum devices.}, archive = {J_PRL}, author = {Tong-Yang Zhao and An-Qi Wang and Zhen-Tao Zhang and Zheng-Yang Cao and Xing-Yu Liu and Zhi-Min Liao}, doi = {10.1103/bzdt-yxk2}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026601}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic field induced quantum metric dipole in dirac semimetal Cd3As2}, volume = {135}, year = {2025}, }
• (2025). Origin of transitions inversion in rare-earth vanadates. PRL, 135(2), 026508. (www)

  @article{ , abstract = {In correlated transition-metal oxides, orbital-ordering appears to always precede magnetic ordering ( T N < T OO ). The R VO 3 series is the exception: it exhibits an inversion of T N and T OO with increasing rare-earth radius R I . Why vanadates are different is not understood. Here we show that the reason is fundamental: when lattice effects dominate orbital physics, magnetic order follows orbital order, and thus T N < T OO . This is what happens in most transition-metal oxides, and it is what quenches exotic quantum orbital phases. In the R VO 3 series, however, lattice effects become ineffective with increasing R I , while, at the same time, for antiferromagnetic spin order, the orbital-independent dipolar spin-spin interaction dominates. This has consequences well beyond the R VO 3 series itself. In fact, the subtle balance of interactions leading to the T N − T OO inversion not only explains why it is so rare, but also gives the criteria for finding it in other materials. The mechanism behind transitions inversion makes such systems an ideal playground for studying unconventional orbital phases. The results presented here rely on the decomposition of the order parameter into irreducible tensors, which allows us to identify the mechanism driving the transition.}, archive = {J_PRL}, author = {Xue-Jing Zhang and Erik Koch and Eva Pavarini}, doi = {10.1103/qvp2-jn9p}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026508}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of transitions inversion in rare-earth vanadates}, volume = {135}, year = {2025}, }
• (2025). Stabilization of fermi liquid behavior by interactions in disordered metals. PRL, 135(2), 026507. (www)

  @article{ , abstract = {We study the interplay of electron-electron and electron-disorder scattering in correlated Fermi liquids by the disordered Hubbard model using dynamical mean-field theory with an IPT-CPA solver. We find significant violations of Matthiessen’s rule (additivity of scattering mechanisms) that we explain in terms of the screening of the disorder potential by interactions, leading to a protection of the electron-electron inelastic scattering rate against disorder. We also show that large disorder can lead to a surprising enhancement of the electron-electron scattering that contrasts with the competition seen in the elastic channel. Our results compare positively with available resistivity data in the disordered Fermi liquid phase of the correlated organic metals , and rationalize the strong sample dependence of the coefficients observed in the resistivity of correlated perovskite oxides such as .}, archive = {J_PRL}, author = {Arianna Poli and Simone Fratini and Jennifer Coulter and Andrew J. Millis and Sergio Ciuchi}, doi = {10.1103/dvzc-vxhw}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026507}, shortjournal = {Phys. Rev. Lett.}, title = {Stabilization of fermi liquid behavior by interactions in disordered metals}, volume = {135}, year = {2025}, }
• (2025). Identifying and quantifying su-schrieffer-heeger-like interactions with resonant inelastic X-ray scattering. PRL, 135(2), 026506. (www)

  @article{ , abstract = {Su-Schrieffer-Heeger-like (SSH-like) electron-phonon interactions can drive the formation of light (bi)polarons and several novel states of matter. It is, therefore, prudent to develop experimental protocols for identifying such couplings in real materials and quantifying their strength. Here, we investigate how resonant inelastic x-ray scattering (RIXS) probes electron-phonon interactions in the one-dimensional half-filled Hubbard-SSH model with on-site phonons. Using the density matrix renormalization group method, we compute the full RIXS response and find that the lattice excitations generated during the scattering process inevitably couple to the system’s charge and magnetic sectors, resulting in combined multiparticle excitations that cannot be easily disentangled from one another. While this aspect complicates the interpretation of RIXS experiments, we outline how it can be leveraged to identify and quantify SSH-like interactions in quantum materials.}, archive = {J_PRL}, author = {Debshikha Banerjee and Jinu Thomas and Alberto Nocera and Steven Johnston}, doi = {10.1103/mr3k-w171}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026506}, shortjournal = {Phys. Rev. Lett.}, title = {Identifying and quantifying su-schrieffer-heeger-like interactions with resonant inelastic X-ray scattering}, volume = {135}, year = {2025}, }
• (2025). Spontaneous spin-orbit coupling induced by quantum phonon dynamics. PRL, 135(2), 026505. (www)

  @article{ , abstract = {Spin-orbit coupling is a important focus of condensed matter physics as well as electron-phonon interaction. Traditionally spin-orbit coupling is regarded as a single-body effect arising from relativity, and electron-phonon interaction is often considered spin-independent. In this Letter, we bridge spin-orbit coupling and electron-phonon interaction, and propose a novel mechanism to dynamically generate spin-orbit coupling. Based on symmetry analysis, a spin-dependent electron-phonon coupling model is constructed, and is solved by sign-problem-free quantum Monte Carlo simulations. The phase diagram versus phonon frequency ω and coupling constant λ is fully investigated. The spin-orbit coupling emerges as an order in the ground state for any λ in the adiabatic limit, accompanied by a breathing mode of lattice distortion and a staggered loop spin current. This phase dominates in the entire range of ω with λ < λ ∞ , a critical value in the ω → ∞ limit. At λ > λ ∞ , the emergent spin-orbit coupling is suppressed as increasing ω , and a phase transition occurs leading to charge-density-wave ordering degenerate with superconductivity. Our work opens up the possibility of hidden spin-orbit coupling in materials where it is otherwise forbidden by lattice symmetry and paves the way to explore possible materials for spintronics.}, archive = {J_PRL}, author = {Xiangyu Zhang and Da Wang and Congjun Wu}, doi = {10.1103/7hv4-kmhd}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026505}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous spin-orbit coupling induced by quantum phonon dynamics}, volume = {135}, year = {2025}, }
• (2025). 3D conformal field theories with Sp(N) global symmetry on a fuzzy sphere. PRL, 135(2), 026504. (www)

  @article{ , abstract = {The quest to discover new 3D CFTs has been intriguing for physicists. For this purpose, fuzzy sphere regularization that studies interacting quantum systems defined on the lowest Landau level on a sphere has emerged as a powerful tool. In this Letter, we discover a series of new CFTs with global symmetry Sp ( N ) in the fuzzy sphere models that are closely related to the SO(5) deconfined phase transition, and are related to a Sp ( N ) / [ Sp ( M ) × Sp ( N − M ) ] nonlinear sigma model with a Wess-Zumino-Witten term. We numerically verify the emergent conformal symmetry by observing the integer-spaced conformal multiplets, the quality of conformal generators, and studying the finite-size scaling of the conformality. We discuss possible candidates for these newly discovered CFTs, the most plausible ones being Chern-Simons-matter theories which have N flavors of gapless bosons or fermions coupled to a non-Abelian [ viz. Sp(1), Sp(2), etc.] Chern-Simons gauge field. Our Letter provides new avenues for studying interacting CFTs in 3D, possibly facilitating the nonperturbative study of critical gauge theories and previously undiscovered CFTs.}, archive = {J_PRL}, author = {Zheng Zhou (周正 and Yin-Chen He}, doi = {10.1103/xstj-xvcy}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026504}, shortjournal = {Phys. Rev. Lett.}, title = {3D conformal field theories with Sp(N) global symmetry on a fuzzy sphere}, volume = {135}, year = {2025}, }
• (2025). Instability of metals with respect to strong electron-phonon interaction. PRL, 135(2), 026503. (www)

  @article{ , abstract = {We show that thermal equilibrium between conduction electrons and phonons becomes kinetically unstable when the renormalized electron-phonon coupling exceeds a certain threshold. We prove that negative electronic specific heat, C el < 0 , is sufficient to trigger the instability. Specifically, the instability sets in as soon as the quasiparticle weight becomes negative over a range of energies, even before C el turns negative. This is an inherently nonequilibrium phenomenon, occurring prior to the formation of any equilibrium phase. Depending on the system, it can proceed along different pathways, ultimately resulting in a structural transition to an insulating or metallic state.}, archive = {J_PRL}, author = {Emil A. Yuzbashyan and Boris L. Altshuler and Aniket Patra}, doi = {10.1103/sf5p-2g5l}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026503}, shortjournal = {Phys. Rev. Lett.}, title = {Instability of metals with respect to strong electron-phonon interaction}, volume = {135}, year = {2025}, }
• (2025). Exploring novel quantum embedding methods with nonorthogonal decomposition of slater determinants. PRL, 135(2), 026502. (www)

  @article{ , abstract = {The Schmidt decomposition of quantum many-body states, which is the basis of many powerful quantum many-body techniques, relies on a partition of the whole system in terms of orthogonal local basis functions. We propose in this Letter a nonorthogonal decomposition of Slater determinants, which reduces to the conventional Schmidt decomposition in the orthogonal limit. The new decomposition provides a natural tool for building local correlation spaces when the orbitals are overlapping, which can be used to extend some existing embedding methods based on the Schmidt decomposition like density matrix embedding theory (DMET) to overlapping subsystem partitions to achieve greater flexibility and efficiency. We also propose a new quantum embedding strategy that bridges the ab initio model potential (AIMP) embedding and DMET, which circumvents the necessarity of a mean-field calculation of the whole system like AIMP, and is able to capture quantum entanglement like DMET.}, archive = {J_PRL}, author = {Yuhang Ai and Ze-Wei Li and Hong Jiang}, doi = {10.1103/kqx7-fr2m}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026502}, shortjournal = {Phys. Rev. Lett.}, title = {Exploring novel quantum embedding methods with nonorthogonal decomposition of slater determinants}, volume = {135}, year = {2025}, }
• (2025). Efficient projected entangled pair states methods for periodic quantum systems. PRL, 135(2), 026501. (www)

  @article{ , abstract = {Projected entangled pair states (PEPS) are recognized as a potent tool for exploring two-dimensional quantum many-body systems. However, a significant challenge emerges when applying conventional PEPS methodologies to systems with periodic boundary conditions (PBCs), attributed to the prohibitive computational scaling with the bond dimension. This has notably restricted the study of systems with complex boundary conditions. To address this challenge, we have developed a strategy that involves the superposition of PEPS with open boundary conditions (OBCs) to treat systems with PBCs. This approach significantly reduces the computational complexity of such systems while maintaining their translational invariance and the PBCs. We benchmark this method against the Heisenberg model and the J 1 − J 2 model, demonstrating its capability to yield highly accurate results at low computational costs, even for large system sizes. We further apply the method to study the Chern numbers of the hard-core Harper-Hofstadter model at different filling factors using twisted boundary conditions. This advancement significantly broadens the applicability of the PEPS approach, opening new avenues for studying a wide range of quantum many-body phenomena.}, archive = {J_PRL}, author = {Shaojun Dong and Chao Wang and Hao Zhang and Meng Zhang and Lixin He}, doi = {10.1103/fvq2-msr4}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026501}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient projected entangled pair states methods for periodic quantum systems}, volume = {135}, year = {2025}, }
• (2025). Overcoming asymmetric carrier injection in III-nitride light-emitting diodes through defect engineering. PRL, 135(2), 026402. (www)

  @article{ , abstract = {The rapid advancements in the semiconductor industry are often accompanied by a breakthrough in defect engineering. While defects usually hinder device performance, they can also offer new opportunities for manipulating semiconductor properties. In this Letter, we present an effective approach to solving the long-standing asymmetric injection of carriers problem in LEDs by introducing nitrogen vacancies ( ) at the GaN/AlN quantum well (QW) interface. The states function as “steps” as well as sources of perturbation potential to improve the electron relaxation to the bottom of the conduction band through the electron-phonon (el-ph) coupling. The electron relaxation time ( ), initially as long as 8.61 ps, was reduced to 0.15 ps, comparable to the (0.12 ps). Our work not only resolves a persistent bottleneck in GaN-based light sources but also offers a new perspective on utilizing defects to engineer carrier relaxation.}, archive = {J_PRL}, author = {Yuxin Yang and Zhiming Shi and Shunpeng Lv and Hang Zang and Xiaobao Ma and Feng Zhang and Yan Yu and Peng Han and Ke Jiang and Xiaolan Yan and Su-Huai Wei and Xiaojuan Sun and Dabing Li}, doi = {10.1103/kt15-x472}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026402}, shortjournal = {Phys. Rev. Lett.}, title = {Overcoming asymmetric carrier injection in III-nitride light-emitting diodes through defect engineering}, volume = {135}, year = {2025}, }
• (2025). Extracting nonlinear dynamical response functions from time evolution. PRL, 135(2), 026401. (www)

  @article{ , abstract = {We develop a general framework based on the functional derivative to extract nonlinear dynamical response functions from the temporal evolution of physical quantities, without explicitly computing multipoint correlation functions. We validate our approach by calculating the second- and third-order optical responses in the Rice–Mele model and further apply it to a many-body interacting system using a tensor network method. This framework is broadly applicable to any method that can compute real-time dynamics, offering a powerful and versatile tool for investigating nonlinear responses in dynamical systems.}, archive = {J_PRL}, author = {Atsushi Ono}, doi = {10.1103/qsxr-c2pq}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026401}, shortjournal = {Phys. Rev. Lett.}, title = {Extracting nonlinear dynamical response functions from time evolution}, volume = {135}, year = {2025}, }
• (2025). Nonadiabatic renormalization of the phonon dispersion in monolayer and bilayer graphene. PRL, 135(2), 026204. (www)

  @article{ , abstract = {Nonadiabatic effects profoundly influence lattice dynamics, resulting in phonon renormalizations not only at the center of Brillouin zone (BZ), but also across the entire dispersion at finite momenta. These nonadiabatic phenomena exhibit clear dimensional dependencies and remain largely unexplored experimentally in low-dimensional systems. Here, we utilize high-resolution electron energy loss spectroscopy to investigate nonadiabatic phonon dispersion renormalization in monolayer graphene (MLG) and Bernal bilayer graphene (BLG). We present comprehensive phonon spectra measurements for both MLG and BLG across the full BZ. The high-resolution data reveal an intriguing “W” -shaped dispersion for the longitudinal optical phonon in MLG and a “V” -shaped dispersion in BLG near the BZ center, in contrast to the conventional “U” -shaped parabolic dispersions. Combining theoretical analysis, these anomalous phonon renormalizations are demonstrated to originate from nonadiabatic electron-phonon couplings. The comparative study of MLG and BLG gives a generic understanding of the impact of nonadiabatic effects on phonon dispersions in doped two-dimensional systems.}, archive = {J_PRL}, author = {Jiade Li and Jilin Tang and Zhiyu Tao and Ruochen Shi and Xin Gao and Siwei Xue and Xiaoyin Gao and Weiyu Sun and Guangyao Miao and Zhibin Su and Xiongfei Shi and Shiqi Hu and Ruilin Mao and Xiaowen Zhang and Peiyi He and Weihua Wang and Peng Gao and Hailin Peng and Chao Lian and Jiandong Guo and Xuetao Zhu}, doi = {10.1103/4x9y-txyy}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026204}, shortjournal = {Phys. Rev. Lett.}, title = {Nonadiabatic renormalization of the phonon dispersion in monolayer and bilayer graphene}, volume = {135}, year = {2025}, }
• (2025). Meron spin textures in momentum space spawning from bound states in the continuum. PRL, 135(2), 026203. (www)

  @article{ , abstract = {Topological spin textures, such as merons and skyrmions, have shown significance in both fundamental science and practical applications across diverse physical systems. The optical skyrmionic textures in real space have been extensively explored, but those in momentum space are still rarely studied. Here, we report the experimental generation of momentum-space meron spin textures via bound states in the continuum (BICs) in photonic crystal slabs. We show that under circularly polarized illumination, the momentum-space vortex topology of BICs can transform light with meron spin textures in momentum space. These merons exhibit polarity-switchable configurations controlled by incident light polarization. We theoretically and experimentally verify the generation of momentum-space merons and demonstrate their operational flexibility across a broad spectral range. Our results establish a connection between different momentum-space topologies and provide a robust and compact platform for generating topological spin textures.}, archive = {J_PRL}, author = {Lixi Rao and Jiajun Wang and Xinhao Wang and Shunben Wu and Xingqi Zhao and Wenzhe Liu and Rensheng Xie and Yijie Shen and Lei Shi and Jian Zi}, doi = {10.1103/3g3j-mnh9}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026203}, shortjournal = {Phys. Rev. Lett.}, title = {Meron spin textures in momentum space spawning from bound states in the continuum}, volume = {135}, year = {2025}, }
• (2025). Superlubric-locked transition of twist grain boundaries in 3D crystals. PRL, 135(2), 026202. (www)

  @article{ , abstract = {Properties of twist grain boundaries (TGB), long known structurally but not tribologically, are simulated under sliding and load, with Au(111) our test case. The load-free TGB moiré is smooth and superlubric at incommensurate twists. Surprisingly, load provokes a first-order structural transformation, where the highest energy moiré nodes are removed—an unexpected Aubry-type transition for which we provide a Landau theory leading to a full twist-load phase diagram. Upon frictional sliding, the transformation causes a superlubric-locked transition, with a huge friction jump, and irreversible plastic flow. The predicted phenomena are robust, also recovered in a Lennard-Jones lattice TGB, and not exclusive to gold or to metals. Both superlubricity and strong Aubry locking hold promises for studies and applications in micro and nano mechanics and devices.}, archive = {J_PRL}, author = {Jin Wang and Erio Tosatti}, doi = {10.1103/7bbs-q17w}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026202}, shortjournal = {Phys. Rev. Lett.}, title = {Superlubric-locked transition of twist grain boundaries in 3D crystals}, volume = {135}, year = {2025}, }
• (2025). Quantum stochastic rectification in a single molecule. PRL, 135(2), 026201. (www)

  @article{ , abstract = {Quantum stochastic rectification arises from the dc response of a system subjected to both quantum noise and a small, periodic sinusoidal voltage modulation. In this Letter, we demonstrate quantum stochastic rectification by using inelastic electron tunneling spectroscopy with a scanning tunneling microscope to monitor the conformational switching of a single pyrrolidine molecule adsorbed on a Cu(001) surface. By applying quasistatic and nonequilibrium approximations, we elucidate the underlying dynamic response mechanisms. Additionally, we establish a quantitative relationship between the critical driving frequency in rectification measurements and the system’s relaxation time, facilitating the measurement of rapid relaxation rates in single molecules.}, archive = {J_PRL}, author = {Jiang Yao and Siyu Chen and Wenlu Shi and W. Ho}, doi = {10.1103/dqfn-y77k}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum stochastic rectification in a single molecule}, volume = {135}, year = {2025}, }
• (2025). Unified picture of superconductivity and magnetism in CeRh2As2. PRL, 135(2), 026003. (www)

  @article{ , abstract = {We propose a theory for the microscopic origin of the multiple superconducting and magnetic phases observed in based on the existence of Van Hove singularities near the Fermi energy. The nonsymmorphic symmetry of this material implies that these singularities are located away from high-symmetry momenta; i.e., they have so-called type-II character. This allows us to include the significant Rashba spin-orbit coupling in in a parquet renormalization group approach. When Fermi-surface nesting is strong, our analysis reveals two closely competing superconducting states with opposite parities, as well as an instability toward spin-density wave states that support both of them, consistent with the phase diagram of . Type-II Van Hove singularities are generic to nonsymmorphic space groups, and so our theory implies that many other compounds may support closely competing even- and odd-parity superconductivity.}, archive = {J_PRL}, author = {Changhee Lee and Daniel F. Agterberg and P. M. R. Brydon}, doi = {10.1103/dt7w-hh9f}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026003}, shortjournal = {Phys. Rev. Lett.}, title = {Unified picture of superconductivity and magnetism in CeRh2As2}, volume = {135}, year = {2025}, }
• (2025). Topotactical hydrogen induced single-band d-wave superconductivity in La2NiO4. PRL, 135(2), 026002. (www)

  @article{ , abstract = {La 2 NiO 4 is an antiferromagnetic insulator with a structural resemblance to its cuprate counterpart, La 2 CuO 4 . However, La 2 CuO 4 has a Cu 2 + or 3 d 9 electronic configuration that needs to be hole or electron doped for superconductivity, whereas La 2 NiO 4 is 3 d 8 with divalent Ni 2 + . Making a cuprate analog through conventional electron doping is impractical due to the rarity of tetravalent substituents for trivalent La. Here, we propose an alternative route: intercalating topotactical hydrogen, which is possible through electric-field-controlled protonation and transforms La 2 NiO 4 into a 3 d x 2 − y 2 single-band two-dimensional antiferromagnetic Mott insulator analogous to La 2 CuO 4 . This we find through density-functional theory and dynamical mean-field theory calculations. The furthergoing dynamical vertex approximation predicts that H − La 2 NiO 4 can host d -wave superconductivity under 15% hole doping with a critical temperature above 20 K. Our findings not only suggest a new method for tuning the electronic structure of layered nickelates but also provide theoretical evidence for a new nickelate superconductor, awaiting experimental synthesis.}, archive = {J_PRL}, author = {Ying Gao and Wenfeng Wu and Zhaoxin Liu and Karsten Held and Liang Si}, doi = {10.1103/yd8w-frs8}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026002}, shortjournal = {Phys. Rev. Lett.}, title = {Topotactical hydrogen induced single-band d-wave superconductivity in La2NiO4}, volume = {135}, year = {2025}, }
• (2025). Perfect superconducting diode effect in altermagnets. PRL, 135(2), 026001. (www)

  @article{ , abstract = {We investigate intrinsic superconducting diode effect in the unconventional superconducting state of d -wave altermagnets. We find large diode efficiencies in the wide-reaching finite-momentum pairing regimes of the phase diagram. Remarkably, even perfect diode efficiency of 100% can be obtained in the presence of an external magnetic field. We attribute the largest efficiencies to competition between multiple zero-momentum (BCS) and finite-momentum superconducting states, which is connected to a topological nodal-to-nodeless transition in altermagnets with magnetic field, making our results applicable to a wide range of altermagnets.}, archive = {J_PRL}, author = {Debmalya Chakraborty and Annica M. Black-Schaffer}, doi = {10.1103/cv8s-tk4c}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {026001}, shortjournal = {Phys. Rev. Lett.}, title = {Perfect superconducting diode effect in altermagnets}, volume = {135}, year = {2025}, }
• (2025). Observation of fermi acceleration with cold atoms. PRL, 135(2), 025201. (www)

  @article{ , abstract = {Cosmic rays are deemed to be generated by a process known as “Fermi acceleration” in which charged particles scatter against magnetic fluctuations in astrophysical plasmas. The process itself is, however, universal, has both classical and quantum formulations, and is at the basis of dynamical systems with interesting mathematical properties, such as the celebrated Fermi-Ulam model. Despite its effectiveness in accelerating particles, Fermi acceleration has so far eluded unambiguous verifications in laboratory settings. Here, we realize a fully controllable Fermi accelerator by colliding ultracold atoms against engineered movable potential barriers. We demonstrate that our Fermi accelerator, which is only 100 μ m in size, can produce ultracold atomic jets with velocities above 0.5 m / s . Adding dissipation, we also experimentally test Bell’s general argument for the ensuing energy spectra, which is at the basis of any model of cosmic ray acceleration. On the one hand, our Letter effectively opens the window to the use of cold atoms to study phenomena relevant for high energy astrophysics. On the other, the performance of our Fermi accelerator is competitive with those of best-in-class accelerating methods used in quantum technology and quantum colliders, but with substantially simpler implementation no fundamental physics limit.}, archive = {J_PRL}, author = {G. Barontini and V. Naniyil and J. P. Stinton and D. G. Reid and J. M. F. Gunn and H. M. Price and A. B. Deb and D. Caprioli and V. Guarrera}, doi = {10.1103/nrjv-pwy1}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {025201}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of fermi acceleration with cold atoms}, volume = {135}, year = {2025}, }
• (2025). Thermodynamics and statistical equilibrium of large-scale hydroelastic wave turbulence. PRL, 135(2), 024004. (www)

  @article{ , abstract = {Understanding how statistical equilibrium can occur in out-of-equilibrium systems is of paramount interest, as it would enable the use of statistical mechanics tools to these systems. Here, we report the first experimental evidence of statistical equilibrium of the large scales of hydroelastic turbulent waves driven by small-scale random forcing. The wave field statistics at scales larger than the forcing scale, resolved in space and time, align well with the predictions of Rayleigh-Jeans equilibrium spectra over more than a decade. We measure zero net energy flux in this regime, as expected. We also determine the effective temperature, entropy, and heat capacity of this nonequilibrium system, demonstrating that classical thermodynamic concepts apply to describe large scales in statistical equilibrium of turbulent systems.}, archive = {J_PRL}, author = {Marlone Vernet and Eric Falcon}, doi = {10.1103/dmrl-gxhw}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {024004}, shortjournal = {Phys. Rev. Lett.}, title = {Thermodynamics and statistical equilibrium of large-scale hydroelastic wave turbulence}, volume = {135}, year = {2025}, }
• (2025). Elastic pseudoturbulence in polymer solutions. PRL, 135(2), 024003. (www)

  @article{ , abstract = {We study the effects of polymer additives on pseudoturbulence induced by a swarm of bubbles rising in a quiescent fluid. We find that, even in the absence of background shear, beyond a critical polymer concentration, the energy spectra of velocity fluctuations in bubble-induced turbulence decay more steeply with respect to the wave number k . This new scaling is significantly steeper than the classical k − 3 scaling observed for bubbles in Newtonian fluids; it is independent of the gas volume fraction in the inertial limit and occurs within the length scales between the bubble wake length and the bubble diameter. Furthermore, we provide quantitative evidence that the presence of polymers enhances the coherence of the flow, as revealed by Lagrangian stretching statistics, highlighting the significant role of polymer additives in modifying the characteristics of pseudoturbulence. Our findings demonstrate that viscoelastic effects can modulate turbulence even in shear-free environments, offering a new perspective on the role of elastic stresses in complex multiphase flows.}, archive = {J_PRL}, author = {Mithun Ravisankar and Roberto Zenit}, doi = {10.1103/q7xk-18th}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {024003}, shortjournal = {Phys. Rev. Lett.}, title = {Elastic pseudoturbulence in polymer solutions}, volume = {135}, year = {2025}, }
• (2025). Flat elastic disc suspensions are indistinguishable from solutions of long flexible polymers within planar incompressible flows. PRL, 135(2), 024002. (www)

  @article{ , abstract = {We prove analytically that the two fundamental rheological equations for (elastic) disc suspensions and long flexible polymers, the so-called Oldroyd-A and -B models, respectively, predict the same flow and total stress fields in any planar incompressible flow. We illustrate this equivalence for creeping flow in a cross-slot channel and investigate differences arising from three-dimensional effects in a weakly elastic Taylor-Couette flow. Finally, we discuss implications for understanding elastic instabilities, controlling inertial turbulence, and deriving constitutive models for complex fluids.}, archive = {J_PRL}, author = {Fabian Hillebrand and Rebecca J. Hill and Mahdi Davoodi and Simon J. Haward and Amy Q. Shen and Robert J. Poole and Stylianos Varchanis}, doi = {10.1103/pmsq-b1th}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {024002}, shortjournal = {Phys. Rev. Lett.}, title = {Flat elastic disc suspensions are indistinguishable from solutions of long flexible polymers within planar incompressible flows}, volume = {135}, year = {2025}, }
• (2025). Wettability-dependent damping of droplet vibrations on solid surfaces. PRL, 135(2), 024001. (www)

  @article{ , abstract = {Oscillating sessile droplets on a plane, crucial in industrial applications like inkjet printing, spray cooling, and antifogging, present a long-standing challenge in determining viscous damping. Existing solutions are limited to first-order asymptotic approximations of hemispherical droplets, accounting only for viscous dissipation near the wall. Considering further the bulk dissipation that is usually neglected due to its higher-order effect, we obtain a two-term approximation of decay rates for pinned sessile droplets with different contact angles. We demonstrate that the two-term approximation effectively resolves discrepancies between predicted and observed dampings for viscosities in the range of practical interest, supported by experiments and simulations. The two-term approximation also explains why hydrophobic droplets possess much lower damping than hydrophilic ones, and offers a template for damping prediction formulas with potential viscosity measurement applications.}, archive = {J_PRL}, author = {Fei Zhang and Chunyu Zhang and Wanqiu Zhang and Yingjie Yu and Shuguang Zhao and Jingwei Chen and Jiaqi Cheng and Yuanpeng Zhang and Hang Ding and Xinping Zhou}, doi = {10.1103/cml9-n6jh}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {024001}, shortjournal = {Phys. Rev. Lett.}, title = {Wettability-dependent damping of droplet vibrations on solid surfaces}, volume = {135}, year = {2025}, }
• (2025). Imaging-based quantum optomechanics. PRL, 135(2), 023601. (www)

  @article{ , abstract = {In active imaging protocols, information about an object is encoded into the spatial mode of a scattered photon. Recently the quantum limits of active imaging have been explored with levitated nanoparticles, which experience a multimode radiation pressure backaction (the photon recoil force) due to radiative scattering of the probe field. Here we extend the analysis of multimode backaction to compliant surfaces, accessing a broad class of mechanical resonators and fruitful analogies to quantum imaging. As an example, we consider imaging of the flexural modes of a membrane by sorting the spatial modes of a laser reflected from its surface. We show that backaction in this setting can be understood to arise from spatiotemporal photon shot noise, an effect that cannot be observed in single-mode optomechanics. We also derive the imprecision-backaction product in the limit of purely spatial (intermodal) coupling, revealing it to be equivalent to the standard quantum limit for single-mode optomechanical coupling. Finally, we show that optomechanical correlations due to spatiotemporal backaction can give rise to two-mode entangled light, providing a mechanism for entangling desired pairs of spatial modes. In conjunction with high- nanomechanics, our findings point to new opportunities at the interface of quantum imaging and optomechanics, including sensors and networks enhanced by spatial mode entanglement.}, archive = {J_PRL}, author = {C. M. Pluchar and W. He and J. Manley and N. Deshler and S. Guha and D. J. Wilson}, doi = {10.1103/64xv-3fyx}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {023601}, shortjournal = {Phys. Rev. Lett.}, title = {Imaging-based quantum optomechanics}, volume = {135}, year = {2025}, }
• (2025). Counterflow of lattice polarons in harmonically confined optical lattices. PRL, 135(2), 023404. (www)

  @article{ , abstract = {We study a mobile impurity in a one-dimensional harmonically confined optical lattice interacting repulsively with a bosonic bath. The behavior of the impurity across baths with superfluid and Mott-insulator domains is examined, including its full back-action effect on the bath. We characterize the bath-impurity phase diagram and reveal the appearance of a correlated counterflow phase, which we support with an analytical model for a mobile impurity-hole pair. This phase shows an extended combined insulator domain of unity filling but no independent domain of constant density. The transition to this phase features a sudden orthogonality and the change of the shape of the impurity’s profile to that of a free particle in an infinite square well. The findings of this work suggest the appearance of unconventional counterflow in trapped imbalanced atomic mixtures.}, archive = {J_PRL}, author = {Felipe Isaule and Abel Rojo-Francàs and Luis Morales-Molina and Bruno Juliá-Díaz}, doi = {10.1103/9ch1-dnvc}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {023404}, shortjournal = {Phys. Rev. Lett.}, title = {Counterflow of lattice polarons in harmonically confined optical lattices}, volume = {135}, year = {2025}, }
• (2025). Joint estimation of a two-phase spin rotation beyond classical limit. PRL, 135(2), 023403. (www)

  @article{ , abstract = {Quantum metrology employs entanglement to enhance measurement precision [V. Giovannetti et al. , Quantum-enhanced measurements: Beating the standard quantum limit, Science 306 , 1330 (2004) , V. Giovannetti et al. , Advances in quantum metrology, Nat. Photonics 5 , 222 (2011) , and L. Pezzè et al. , Quantum metrology with nonclassical states of atomic ensembles, Rev. Mod. Phys. 90 , 035005 (2018) ]. The focus and progress so far have primarily centered on estimating a single parameter. In diverse application scenarios, estimation of more than one single parameter is often required. Joint estimation of multiple parameters can benefit from additional advantages for further enhanced precision. Here we report quantum-enhanced estimation of simultaneous spin rotations around two orthogonal axes, making use of spin-nematic squeezing in an atomic Bose-Einstein condensate. Aided by the F = 2 atomic ground hyperfine manifold coupled to the nematic-squeezed F = 1 states as an auxiliary field through a sequence of microwave (MW) pulses, multiple spin-1 observables are simultaneously measured, reaching an enhancement factor 3.3 to 6.3 decibels (dB) beyond the classical limit over a wide range of rotation angles. Our work realizes the first quantum enhanced multiparameter estimation using entangled massive particles. The techniques developed and the protocols implemented also highlight the application of two-mode squeezed vacuum states in quantum-enhanced sensing of noncommuting spin rotations simultaneously.}, archive = {J_PRL}, author = {Jiahao Cao and Xinwei Li and Tianwei Mao and Wenxin Xu and Li You}, doi = {10.1103/n4f7-7vd1}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {023403}, shortjournal = {Phys. Rev. Lett.}, title = {Joint estimation of a two-phase spin rotation beyond classical limit}, volume = {135}, year = {2025}, }
• (2025). Observation of spin squeezing with contact interactions in one- and three-dimensional easy-plane magnets. PRL, 135(2), 023402. (www)

  @article{ , abstract = {Spin squeezing in a many-body system is a witness for entanglement and can enable measurement sensitivities beyond those achievable by only classical correlations. Here, working with ultracold Li 7 atoms in an optical lattice, we demonstrate spin squeezing using short-range contact interactions in both one and three dimensions. In 1D, spin squeezing is shown to be insensitive to density fluctuations caused by holes. In 3D, however, we observe that holes strongly modify the squeezing dynamics, hindering the recently predicted emergence of scalable squeezing in 3D X X Z spin systems. By developing a new theoretical model to account for spin-density coupling, we obtain strong quantitative agreement with the observed squeezing dynamics, resulting in ≈ 2 dB at 7% hole fraction. Our observations highlight the importance of understanding spin-density coupling in the dynamics of many interacting spins and lay the groundwork for improved spin squeezing in systems with only short-range interactions.}, archive = {J_PRL}, author = {Yoo Kyung Lee and Maxwell Block and Hanzhen Lin (林翰桢 and Vitaly Fedoseev and Philip J. D. Crowley and Norman Y. Yao and Wolfgang Ketterle}, doi = {10.1103/jqvz-kpwg}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {023402}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of spin squeezing with contact interactions in one- and three-dimensional easy-plane magnets}, volume = {135}, year = {2025}, }
• (2025). Polariton fluids as quantum field theory simulators on tailored curved spacetimes. PRL, 135(2), 023401. (www)

  @article{ , abstract = {Quantum field theory (QFT) in curved spacetimes predicts the amplification of field excitations and the occurrence of classical and quantum correlations, as in the Hawking effect for example. This raises interest in experiments in which the curvature of spacetime can be controlled and amplification measured, as in fluids going from subsonic to supersonic speeds where acoustic excitations are effectively trapped inside an acoustic horizon. Quantum fluctuations of the acoustic field are predicted to yield entangled emission across the horizon, as in black holes. Here, we introduce such a QFT simulator in a one-dimensional polaritonic fluid of light. We demonstrate the unique tunability of our system by engineering smooth and steep horizons, which respectively have quasithermal, but weak, and strong Hawking radiation. We measure the spectrum on either side of the horizon and evidence the excitation of negative energy waves in fluids of light for the first time. Notably, we explicitly show that, beyond phononic excitations as in other systems, our simulator also supports excitations with a massive, relativistic dispersion. In the future, quantum optics techniques offer the possibility to measure entanglement in unexplored regimes, giving insight in this outstanding prediction of relativistic QFT.}, archive = {J_PRL}, author = {Kévin Falque and Adrià Delhom and Quentin Glorieux and Elisabeth Giacobino and Alberto Bramati and Maxime J. Jacquet}, doi = {10.1103/t5dh-rx6w}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {023401}, shortjournal = {Phys. Rev. Lett.}, title = {Polariton fluids as quantum field theory simulators on tailored curved spacetimes}, volume = {135}, year = {2025}, }
• (2025). Optical protection of alkali-metal atoms from spin relaxation. PRL, 135(2), 023201. (www)

  @article{ , abstract = {We present an optical technique for suppressing relaxation in alkali-metal spins using a single off-resonant laser beam. The method harnesses a physical mechanism that synchronizes Larmor precession in the two hyperfine manifolds, protecting magnetic coherence from relaxation caused by spin-exchange and other hyperfine-changing collisions. We experimentally demonstrate up to a ninefold reduction in decoherence of warm cesium vapor, achieving simultaneous protection from both spin-exchange relaxation and partial depolarization from coated cell walls. The technique substantially enhances the spin precession quality factor and maintains a stable gyromagnetic ratio independent of spin polarization, even under frequent collisions. These findings offer a pathway for mitigating dominant relaxation channels in alkali-metal-based applications and experiments, particularly in anti-relaxation-coated cells.}, archive = {J_PRL}, author = {Avraham Berrebi and Mark Dikopoltsev and Ori Katz and Or Katz}, doi = {10.1103/fncz-b3yy}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {023201}, shortjournal = {Phys. Rev. Lett.}, title = {Optical protection of alkali-metal atoms from spin relaxation}, volume = {135}, year = {2025}, }
• (2025). Isospin symmetry breaking disclosed in the decay of three-proton emitter al20. PRL, 135(2), 022502. (www)

  @article{ , abstract = {The previously unknown nucleus Al 20 has been observed for the first time by detecting its in-flight decays. Tracking trajectories of all decay products with silicon microstrip detectors allowed for a conclusion that Al 20 is unbound with respect to three-proton ( 3 p ) emission. The 3 p -decay energy of the Al 20 ground state has been determined to be 1.93 ( − 0.10 + 0.12 ) MeV through a detailed study of angular correlations of its decay products, Ne 17 + p + p + p . This value is significantly smaller than the predictions inferred from the isospin symmetry by using the known neutron separation energy of its mirror nucleus N 20 , which indicates a possible isospin symmetry breaking in the mirror nuclei Al 20 and N 20 . This observed isospin symmetry breaking is supported by the calculations of the continuum embedded theoretical frameworks, describing the observed Al 20 ground state as a 1 p s -wave state with a spin-parity of 1 − , which differs from the spin-parity ( 2 − ) of the N 20 ground state. The Al 20 ground state decays by sequential 1 p − 2 p emission via the intermediate ground state of Mg 19 , which is the first observed case of “daughter” 2 p radioactivity following 1 p decay of the parent state.}, archive = {J_PRL}, author = {X.-D. Xu and I. Mukha and J. G. Li and S. M. Wang and L. Acosta and M. Bajzek and E. Casarejos and D. Cortina-Gil and J. M. Espino and A. Fomichev and H. Geissel and J. Gómez-Camacho and L. V. Grigorenko and O. Kiselev and A. A. Korsheninnikov and D. Kostyleva and N. Kurz and Yu. A. Litvinov and I. Martel and C. Nociforo and M. Pfützner and C. Rodríguez-Tajes and C. Scheidenberger and M. Stanoiu and K. Sümmerer and H. Weick and P. J. Woods and M. V. Zhukov}, doi = {10.1103/hkmy-yfdk}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {022502}, shortjournal = {Phys. Rev. Lett.}, title = {Isospin symmetry breaking disclosed in the decay of three-proton emitter al20}, volume = {135}, year = {2025}, }
• (2025). New class of three-nucleon forces and their implications. PRL, 135(2), 022501. (www)

  @article{ , abstract = {We identify a new class of three-nucleon forces that arises in the low-energy effective theory of nuclear interactions including pions. We estimate their contribution to the energy of neutron and nuclear matter and find that it can be as important as the leading-order three-nucleon forces previously considered in the literature. The magnitude of this force is set by the strength of the coupling of pions to two nucleons and is presently not well constrained by experiments. The implications for nuclei, nuclear matter, and the equation of state of neutron matter are briefly discussed.}, archive = {J_PRL}, author = {Vincenzo Cirigliano and Maria Dawid and Wouter Dekens and Sanjay Reddy}, doi = {10.1103/kn79-f5m9}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {022501}, shortjournal = {Phys. Rev. Lett.}, title = {New class of three-nucleon forces and their implications}, volume = {135}, year = {2025}, }
• (2025). Collision-energy dependence in heavy-ion collisions from nonlinear QCD evolution. PRL, 135(2), 022302. (www)

  @article{ , abstract = {We explore the effects of including the energy dependence determined from evolution equations within the color glass condensate framework on observables in ultrarelativistic heavy-ion collisions. This amounts to integrating the JIMWLK evolution equations into the impact parameter-dependent glasma model, which is then coupled to viscous relativistic hydrodynamics. This methodology allows for a systematic representation of nuclei at specific Bjorken- values, which are probed at different center-of-mass energies of the collision and rapidities of final state particles. Comparing the methodology to the conventional impact parameter-dependent glasma model, we find significant effects on multiplicity distributions and particle spectra, especially in smaller collision systems at the highest center-of-mass energies. Our results highlight the importance of incorporating nonlinear QCD evolution in the description of heavy-ion collisions at varying center-of-mass energies, as the precise extraction of transport coefficients will be affected. This Letter establishes a robust framework for understanding the quark gluon plasma and nuclear structure at high energy, integrating small- physics into the initial conditions of heavy-ion collisions.}, archive = {J_PRL}, author = {Heikki Mäntysaari and Björn Schenke and Chun Shen and Wenbin Zhao}, doi = {10.1103/gf4y-p5j7}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {022302}, shortjournal = {Phys. Rev. Lett.}, title = {Collision-energy dependence in heavy-ion collisions from nonlinear QCD evolution}, volume = {135}, year = {2025}, }
• (2025). Benchmarking nuclear matrix elements of 0νββ decay with high-energy nuclear collisions. PRL, 135(2), 022301. (www)

  @article{ , abstract = {Reducing uncertainties in the nuclear matrix elements (NMEs) remains a critical challenge in designing and interpreting experiments aimed at discovering neutrinoless double-beta ( ) decay. Here, we identify a class of observables, distinct from those employed in low-energy nuclear structure applications, that are strongly correlated with the NMEs: momentum correlations among hadrons produced in high-energy nuclear collisions. Focusing on the transition, we combine a Bayesian analysis of the structure of with simulations of high-energy collisions. We reveal prominent correlations between the NMEs and features of the quark-gluon plasma formed in these processes, such as spatial gradients and anisotropies, that are accessible via collective flow measurements. Our findings demonstrate collider experiments involving decay candidates as a platform for benchmarking theoretical predictions of the NMEs.}, archive = {J_PRL}, author = {Yi Li and Xin Zhang and Giuliano Giacalone and Jiangming Yao}, doi = {10.1103/zymp-tyjj}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {022301}, shortjournal = {Phys. Rev. Lett.}, title = {Benchmarking nuclear matrix elements of 0νββ decay with high-energy nuclear collisions}, volume = {135}, year = {2025}, }
• (2025). Neural-network extraction of unpolarized transverse-momentum-dependent distributions. PRL, 135(2), 021904. (www)

  @article{ , abstract = {We present the first extraction of transverse-momentum-dependent distributions of unpolarized quarks from experimental Drell-Yan data using neural networks to parametrize their nonperturbative part. We show that neural networks outperform traditional parametrizations providing a more accurate description of data. This Letter establishes the feasibility of using neural networks to explore the multidimensional partonic structure of hadrons and paves the way for more accurate determinations based on machine-learning techniques.}, archive = {J_PRL}, author = {MAP (Multi-dimensional Analyses of Partonic distributions) Collaboration and Alessandro Bacchetta and Valerio Bertone and Chiara Bissolotti and Matteo Cerutti and Marco Radici and Simone Rodini and Lorenzo Rossi}, doi = {10.1103/csc2-bj91}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021904}, shortjournal = {Phys. Rev. Lett.}, title = {Neural-network extraction of unpolarized transverse-momentum-dependent distributions}, volume = {135}, year = {2025}, }
• (2025). QCD predictions for physical multimeson scattering amplitudes. PRL, 135(2), 021903. (www)

  @article{ , abstract = {We use lattice QCD calculations of the finite-volume spectra of systems of two and three mesons to determine, for the first time, three-particle scattering amplitudes with physical quark masses. Our results are for combinations of and , at a lattice spacing , and in the isospin-symmetric limit. We also obtain accurate results for maximal-isospin two-meson amplitudes, with those for and being the first determinations at the physical point. Dense lattice spectra are obtained using the stochastic Laplacian-Heaviside method, and the analysis leading to scattering amplitudes is done using the relativistic finite-volume formalism. Results are compared to chiral perturbation theory and to phenomenological fits to experimental data, finding good agreement.}, archive = {J_PRL}, author = {Sebastian M. Dawid and Zachary T. Draper and Andrew D. Hanlon and Ben Hörz and Colin Morningstar and Fernando Romero-López and Stephen R. Sharpe and Sarah Skinner}, doi = {10.1103/6nql-yrhw}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021903}, shortjournal = {Phys. Rev. Lett.}, title = {QCD predictions for physical multimeson scattering amplitudes}, volume = {135}, year = {2025}, }
• (2025). Isolating unisolated upsilons with anomaly detection in CMS open data. PRL, 135(2), 021902. (www)

  @article{ , abstract = {We present the first study of anti-isolated Upsilon decays to two muons ( ϒ → μ + μ − ) in proton-proton collisions at the Large Hadron Collider. Using a machine learning (ML)-based anomaly detection strategy, we “rediscover” the ϒ in 13 TeV CMS Open Data from 2016, despite overwhelming anti-isolated backgrounds. We elevate the signal significance to 6.4 σ using these methods, starting from 1.6 σ using the dimuon mass spectrum alone. Moreover, we demonstrate improved sensitivity from using an ML-based estimate of the multifeature likelihood compared to traditional “cut-and-count” methods. This is the first ever detection of anti-isolated Upsilons, which can be useful in the study of heavy-flavor fragmentation in quantum chromodynamics. Our Letter demonstrates that it is possible and practical to find real signals in experimental collider data using ML-based anomaly detection, and we distill a readily accessible benchmark dataset from the CMS Open Data to facilitate future anomaly detection developments.}, archive = {J_PRL}, author = {Rikab Gambhir and Radha Mastandrea and Benjamin Nachman and Jesse Thaler}, doi = {10.1103/vvv3-5kkl}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021902}, shortjournal = {Phys. Rev. Lett.}, title = {Isolating unisolated upsilons with anomaly detection in CMS open data}, volume = {135}, year = {2025}, }
• (2025). Quark matter at four loops: Hardships and how to overcome them. PRL, 135(2), 021901. (www)

  @article{ , abstract = {Knowledge of the pressure of cold and dense quark matter is known to significantly constrain the equation of state of neutron-star matter, a quantity playing a key role in deciphering the stars’ internal structure. In this Letter, we make important progress toward determining the last unknown contribution to the pressure at next-to-next-to-next-to-leading order in the strong coupling constant , available through the sum of all four-loop vacuum diagrams of dense quantum chromodynamics. We demonstrate the cancellation of both the covariant gauge parameter and all infrared divergences in the sum, showcasing the effective-field-theory paradigm in action. For the remaining infrared-finite four-loop integrals, we demonstrate the efficacy of the dense loop tree duality method—a novel numerical framework for multiloop calculations in thermal field theory. Together, our results show that completing the next-to-next-to-next-to-leading order pressure of cold quark matter is no longer merely possible but for the first time within reach.}, archive = {J_PRL}, author = {Aapeli Kärkkäinen and Pablo Navarrete and Mika Nurmela and Risto Paatelainen and Kaapo Seppänen and Aleksi Vuorinen}, doi = {10.1103/627n-5g6l}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021901}, shortjournal = {Phys. Rev. Lett.}, title = {Quark matter at four loops: Hardships and how to overcome them}, volume = {135}, year = {2025}, }
• (2025). Evidence for B−→D**0τ−ντ¯ decays. PRL, 135(2), 021802. (www)

  @article{ , abstract = {The first evidence for the decay is obtained using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of , at centre-of-mass energies of 7, 8, and 13 TeV. Here, the meson represents any of the three excited charm mesons , and . The signal is measured with a significance of , including systematic uncertainties. The combined branching fraction , where denotes both and contributions, is measured to be , where the last uncertainty reflects that of the branching fraction of the normalization channel . The ratio between the tauonic and muonic semileptonic decays, with the latter taken from world average values, is also determined and found to be .}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and M. Hajheidari and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. M. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and B. Urbach and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/rj9h-n4w1}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021802}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for B−→D**0τ−ντ¯ decays}, volume = {135}, year = {2025}, }
• (2025). Incorporating physical priors into weakly supervised anomaly detection. PRL, 135(2), 021801. (www)

  @article{ , abstract = {We propose a new machine-learning-based anomaly detection strategy for comparing data with a background-only reference (a form of weak supervision). The sensitivity of previous strategies degrades significantly when the signal is too rare or there are many unhelpful features. Our prior-assisted weak supervision (PAWS) method incorporates information from a class of signal models to significantly enhance the search sensitivity of weakly supervised approaches. As long as the true signal is in the prespecified class, PAWS matches the sensitivity of a dedicated, fully supervised method without specifying the exact parameters ahead of time. On the benchmark LHC Olympics anomaly detection dataset, our mix of semisupervised and weakly supervised learning is able to extend the sensitivity over previous methods by a factor of 10 in cross section. Furthermore, if we add irrelevant (noise) dimensions to the inputs, classical methods degrade by another factor of 10 in cross section while PAWS remains insensitive to noise. This new approach could be applied in a number of scenarios and pushes the frontier of sensitivity between completely model-agnostic approaches and fully model-specific searches.}, archive = {J_PRL}, author = {Chi Lung Cheng and Gup Singh and Benjamin Nachman}, doi = {10.1103/8259-wt5p}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021801}, shortjournal = {Phys. Rev. Lett.}, title = {Incorporating physical priors into weakly supervised anomaly detection}, volume = {135}, year = {2025}, }
• (2025). Form factors from string amplitudes. PRL, 135(2), 021603. (www)

  @article{ , abstract = {In this Letter, we propose a stringy model for n -point tree-level form factor with the off-shell operator in the scalar and gluon theories from the bosonic string disk amplitude: n open string states and one closed string state scatter on the disk. In the field-theory limit ( α ′ → 0 ), the “stringy form factor” reduces to the form factor, which helps us to investigate the hidden properties of the field-theory form factors, manifest the factorization and soft behaviors, and uncover more nontrivial relations between form factors and scattering amplitudes.}, archive = {J_PRL}, author = {Qu Cao}, doi = {10.1103/svb5-mhpc}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021603}, shortjournal = {Phys. Rev. Lett.}, title = {Form factors from string amplitudes}, volume = {135}, year = {2025}, }
• (2025). Minimal model renormalization group flows: Noninvertible symmetries and nonperturbative description. PRL, 135(2), 021602. (www)

  @article{ , abstract = {In this Letter we continue the investigation of RG flows between Virasoro minimal models of two-dimensional conformal field theories that are protected by noninvertible symmetries. RG flows leaving unbroken a subcategory of noninvertible symmetries are associated with anomaly matching conditions that we employ systematically to map the space of flows between minimal models beyond the -symmetric proposed recently in the literature. We introduce a family of nonlinear integral equations that appear to encode the exact finite-size, ground-state energies of these flows, including nonintegrable cases, such as the recently proposed . Our family of NLIEs encompasses and generalizes the integrable flows known in the literature: , and . This work uncovers a new interplay between exact solvability and noninvertible symmetries. Furthermore, our nonperturbative description provides a nontrivial test for all the flows conjectured by anomaly matching conditions, but so far not observed by other means.}, archive = {J_PRL}, author = {Federico Ambrosino and Stefano Negro}, doi = {10.1103/dg1s-5vp6}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021602}, shortjournal = {Phys. Rev. Lett.}, title = {Minimal model renormalization group flows: Noninvertible symmetries and nonperturbative description}, volume = {135}, year = {2025}, }
• (2025). Revisiting scattering enhancement from the aharonov-bohm effect. PRL, 135(2), 021601. (www)

  @article{ , abstract = {We revisit the problem of a charged particle scattering off of an Aharonov-Bohm cosmic string. A classic computation gave an infinite total scattering cross section, leading to a Callan-Rubakov-like enhancement which can have important implications on baryon number asymmetry in the early Universe. However, unlike the Callan-Rubakov effect, the Aharonov-Bohm interaction is topological and thus it is surprising that it leads to such a dramatic dynamical effect for single particle scattering. We reexamine this old problem through the modern lens of generalized global symmetries by embedding Aharanov-Bohm strings in a discrete gauge theory. We show that the scattering cross section is suppressed by the core size and there is thus no Callan-Rubakov-like enhancement.}, archive = {J_PRL}, author = {T. Daniel Brennan and Jaipratap Singh Grewal and Eric Y. Yang}, doi = {10.1103/cdns-8bw7}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021601}, shortjournal = {Phys. Rev. Lett.}, title = {Revisiting scattering enhancement from the aharonov-bohm effect}, volume = {135}, year = {2025}, }
• (2025). Firewalls from general covariance. PRL, 135(2), 021501. (www)

  @article{ , abstract = {I define “horizon normalcy” as the approximate validity of semiclassical gravity and effective field theory for the description of observers that approach or cross a black hole horizon. If black holes return information, then horizon normalcy must fail substantially, at least in some global states. It has been proposed that horizon normalcy persists, so long as the Hawking radiation remains in a computationally simple state. Here I argue that state-dependent horizon normalcy—independent of the underlying mechanism and independent of the class of radiation states asserted to guarantee normalcy—requires a breakdown of general covariance far from the black hole, or else horizon normalcy will depend on the infinite future of the exterior. This is because the radiation can be in different states at different events, all spacelike to the horizon crossing event whose normalcy is at stake. I discuss a related effect in AdS/CFT, and I argue that its resolution by timefolds is of no help here.}, archive = {J_PRL}, author = {Raphael Bousso}, doi = {10.1103/xl94-k5rj}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021501}, shortjournal = {Phys. Rev. Lett.}, title = {Firewalls from general covariance}, volume = {135}, year = {2025}, }
• (2025). Computation of the semiclassical outflux emerging from a collapsing spherical null shell. PRL, 135(2), 021401. (www)

  @article{ , abstract = {We consider a minimally coupled, massless quantum scalar field Φ ^ propagating in the background geometry of a four-dimensional black hole formed by the collapse of a spherical thin null shell, with a Minkowski interior and a Schwarzschild exterior. The field is taken in the natural “in” vacuum state, namely, the quantum state in which no excitations arrive from past null infinity. Within the semiclassical framework, we analyze the vacuum polarization ⟨ Φ ^ 2 ⟩ ren and the energy outflux density ⟨ T ^ u u ⟩ ren (where u is the standard null Eddington coordinate) just outside the shell. Using the point-splitting method, we derive closed-form analytical expressions for both of these semiclassical quantities. In particular, our result for ⟨ T ^ u u ⟩ ren reveals that it vanishes like ( 1 − 2 M 0 / r 0 ) 2 as the shell collapses toward the event horizon, where M 0 is the shell’s mass and r 0 is the value of the area coordinate r at the evaluation point. This confirms that, along a late-time outgoing null geodesic (i.e., one that emerges from the shell very close to the event horizon and propagates toward future null infinity), the outflux gradually evolves (from virtually zero) up to its final Hawking-radiation value while the geodesic traverses the strong-field region (rather than the Hawking-radiation outflux being emitted entirely from the collapsing shell, which would lead to significant backreaction effects).}, archive = {J_PRL}, author = {Amos Ori and Noa Zilberman}, doi = {10.1103/p4bk-qg3n}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021401}, shortjournal = {Phys. Rev. Lett.}, title = {Computation of the semiclassical outflux emerging from a collapsing spherical null shell}, volume = {135}, year = {2025}, }
• (2025). Origin of the most recently ejected OB runaway star from the r136 cluster. PRL, 135(2), 021201. (www)

  @article{ , abstract = {The ∼ 60 000 solar-mass ( M ⊙ ) star cluster R136 (NGC 2070) in the Tarantula Nebula in the Large Magellanic Cloud is the host of at least 55 massive stars ( M ≳ 10 M ⊙ ) which move away from the cluster at projected velocities ≥ 27.5 km / s . The origin of the high velocities of such runaway stars have been debated since the 1960s, resulting either from dynamical ejections or from supernova explosions. Because of the Gaia satellite’s outstanding precision, we can now retrace the most recently ejected binary star, Mel 34, back to the center of R136 and reconstruct the events that 52 000 years ago led to its removal from R136; i.e., we establish its dynamical interaction and ejection history. We find that this ejection requires the participation of five stars in a strong interaction between a triple composed of the tight massive binary Mel 39, orbited by the star VFTS 590, and the binary star Mel 34. The participation of five stars is unexpected because runaway stars were not expected to result from triple interactions. The deterministic nature of the Newtonian dynamics in the scattering enables us to reconstruct the encounter that ejected Mel 34. We then predict that Mel 39 is a binary star with an 80 M ⊙ companion star that orbits within ∼ 1 ° in the same plane as Mel 34 and escapes the cluster with a velocity of ∼ 64 km / s . The five stars will undergo supernova explosions in the coming 5 Myr at a distance of ∼ 180 – 332 pc from their birth location (R136). The resulting black hole binaries, however, are not expected to merge within a Hubble time.}, archive = {J_PRL}, author = {Simon Portegies Zwart and Mitchel Stoop and Lex Kaper and Alex de Koter and Steven Rieder and Tomer Shenar}, doi = {10.1103/n43y-wt19}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021201}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of the most recently ejected OB runaway star from the r136 cluster}, volume = {135}, year = {2025}, }
• (2025). Precision spectral measurements of chromium and titanium from 10 to 250 GeV/n and sub-iron to iron ratio with the calorimetric electron telescope on the international space station. PRL, 135(2), 021002. (www)

  @article{ , abstract = {The Calorimetric Electron Telescope (CALET), in operation on the International Space Station since 2015, collected a large sample of cosmic-ray (CR) iron and sub-iron events over a wide energy interval. In this Letter, we report an update of our previous measurement of the iron flux and we present—for the first time—a high statistics measurement of the spectra of two sub-iron elements Cr and Ti in the energy interval from 10 to . The analyses are based on 8 years of data. Differently from older generations of cosmic-ray instruments which, in most cases, could not resolve individual sub-iron elements, CALET can identify each nuclear species from proton to nickel (and beyond) with a measurement of their electric charge. Thanks to the improvement in statistics and a more refined assessment of systematic uncertainties, the iron spectral shape is better resolved, at high energy, than in our previous paper, and we report its flux ratio to chromium and titanium. The measured fluxes of Cr and Ti show energy dependences compatible with a single power law with spectral indices and , respectively.}, archive = {J_PRL}, author = {CALET Collaboration and O. Adriani and Y. Akaike and K. Asano and Y. Asaoka and E. Berti and P. Betti and G. Bigongiari and W. R. Binns and M. Bongi and P. Brogi and A. Bruno and N. Cannady and G. Castellini and C. Checchia and M. L. Cherry and G. Collazuol and G. A. de Nolfo and K. Ebisawa and A. W. Ficklin and H. Fuke and S. Gonzi and T. G. Guzik and T. Hams and K. Hibino and M. Ichimura and M. H. Israel and K. Kasahara and J. Kataoka and R. Kataoka and Y. Katayose and C. Kato and N. Kawanaka and Y. Kawakubo and K. Kobayashi and K. Kohri and H. S. Krawczynski and J. F. Krizmanic and P. Maestro and P. S. Marrocchesi and M. Mattiazzi and A. M. Messineo and J. W. Mitchell and S. Miyake and A. A. Moiseev and M. Mori and N. Mori and H. M. Motz and K. Munakata and S. Nakahira and J. Nishimura and M. Negro and S. Okuno and J. F. Ormes and S. Ozawa and L. Pacini and P. Papini and B. F. Rauch and S. B. Ricciarini and K. Sakai and T. Sakamoto and M. Sasaki and Y. Shimizu and A. Shiomi and P. Spillantini and F. Stolzi and S. Sugita and A. Sulaj and M. Takita and T. Tamura and T. Terasawa and S. Torii and Y. Tsunesada and Y. Uchihori and E. Vannuccini and J. P. Wefel and K. Yamaoka and S. Yanagita and A. Yoshida and K. Yoshida and W. V. Zober}, doi = {10.1103/py17-74rk}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021002}, shortjournal = {Phys. Rev. Lett.}, title = {Precision spectral measurements of chromium and titanium from 10 to 250 GeV/n and sub-iron to iron ratio with the calorimetric electron telescope on the international space station}, volume = {135}, year = {2025}, }
• (2025). Composite heavy axionlike dark matter. PRL, 135(2), 021001. (www)

  @article{ , abstract = {We propose a novel class of dark matter (DM) candidates in the form of a heavy composite axionlike particle (ALP) with highly suppressed electromagnetic interactions populating vast yet unexplored domains in the ALP parameter space. This is achieved for the first time in the simplest dark confining gauge theory yielding a new composite glueball ALP (GALP) DM coupling-mass relation found in terms of two distinct fundamental scales—the large dark fermion mass scale and the dynamical scale of dark confinement. The presence of a heavy fermion portal between the visible (photons) and dark (GALPs) sectors ensures a strong radiative suppression of the GALP-photon coupling naturally without any fine-tuning. The observable features of heavy GALP DM in a minimal realization are controlled by only three physical parameters. Our work paves the road for a novel research field exploring the theory and phenomenology of composite ALPs in multimessenger astrophysics and cosmology.}, archive = {J_PRL}, author = {Pierluca Carenza and Roman Pasechnik and Zhi-Wei Wang}, doi = {10.1103/49pk-z8c8}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {021001}, shortjournal = {Phys. Rev. Lett.}, title = {Composite heavy axionlike dark matter}, volume = {135}, year = {2025}, }
• (2025). Sharp finite statistics for quantum key distribution. PRL, 135(2), 020803. (www)

  @article{ , abstract = {The performance of quantum key distribution (QKD) heavily depends on statistical inference. For a broad class of protocols, the central statistical task is a random sampling problem, customarily addressed using a hypergeometric tail bound due to Serfling. Here, we provide an alternative solution for this task of unprecedented tightness among QKD security analyses. As a by-product, confidence intervals for the average of nonidentical Bernoulli parameters follow too. These naturally fit in statistical analyses of decoy-state QKD and also outperform standard tools. Last, we show that, in a vast parameter regime, the use of tail bounds is not enforced because the cumulative mass function of the hypergeometric distribution is accurately computable. This sharply decreases the minimum block sizes necessary for QKD, and reveals the tightness of our analytical bounds when moderate-to-large blocks are considered.}, archive = {J_PRL}, author = {Vaisakh Mannalath and Víctor Zapatero and Marcos Curty}, doi = {10.1103/l735-x48g}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020803}, shortjournal = {Phys. Rev. Lett.}, title = {Sharp finite statistics for quantum key distribution}, volume = {135}, year = {2025}, }
• (2025). Chip-to-chip quantum photonic controlled-not gate teleportation. PRL, 135(2), 020802. (www)

  @article{ , abstract = {Quantum networks provide a novel framework for quantum information processing, significantly improving system capacity through the interconnection of modular quantum nodes. Beyond the capability to distribute quantum states, the ability to remotely control quantum gates is a pivotal step for quantum networks. Here, we implement high-fidelity quantum controlled- not ( cnot ) gate teleportation with high-dimensional path encoded silicon photonic integrated circuits. Based on on-chip generation of the path-entangled quantum state, cnot gate operation, and chip-to-chip quantum photonic interconnect, the cnot gate is teleported between two remote quantum nodes connected by the single-mode optical fiber. Equip with 5 m (1 km)-long interconnecting fiber, quantum gate teleportation is verified by entangling remote qubits with 95.69 % ± 1.19 % ( 94.07 % ± 1.54 % ) average fidelity and gate tomography with 94.81 % ± 0.81 % ( 93.04 % ± 1.09 % ) fidelity. These results advance the realization of large-scale and practical quantum networks with photonic integrated circuits.}, archive = {J_PRL}, author = {Lan-Tian Feng and Ming Zhang and Di Liu and Yu-Jie Cheng and Xin-Yu Song and Yu-Yang Ding and Dao-Xin Dai and Guo-Ping Guo and Guang-Can Guo and Xi-Feng Ren}, doi = {10.1103/d53g-v8q6}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020802}, shortjournal = {Phys. Rev. Lett.}, title = {Chip-to-chip quantum photonic controlled-not gate teleportation}, volume = {135}, year = {2025}, }
• (2025). One-shot min-entropy calculation of classical-quantum states and its application to quantum cryptography. PRL, 135(2), 020801. (www)

  @article{ , abstract = {In quantum Shannon theory, various kinds of quantum entropies are used to characterize the capacities of noisy physical systems. Among them, min-entropy and its smooth version attract wide interest especially in the field of quantum cryptography as they can be used to bound the information obtained by an adversary. However, calculating the exact value or nontrivial bounds of min-entropy are extremely difficult because the composite system dimension may scale exponentially with the dimension of its subsystem. Here, we develop a one-shot lower bound calculation technique for the min-entropy of a classical-quantum state that is applicable to both finite and infinite dimensional reduced quantum states. Moreover, we show our technique is of practical interest in at least three situations. First, it offers an alternative tight finite-data analysis for the BB84 quantum key distribution scheme. Second, it gives the best finite-key bound known to date for a variant of device independent quantum key distribution protocol. Third, it provides a security proof for a novel source-independent continuous-variable quantum random number generation protocol. These results show the effectiveness and wide applicability of our approach.}, archive = {J_PRL}, author = {Rong Wang and H. F. Chau}, doi = {10.1103/ynm5-k1vq}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020801}, shortjournal = {Phys. Rev. Lett.}, title = {One-shot min-entropy calculation of classical-quantum states and its application to quantum cryptography}, volume = {135}, year = {2025}, }
• (2025). Dark spin-cat states as biased qubits. PRL, 135(2), 020601. (www)

  @article{ , abstract = {We present a biased atomic qubit, universally implementable across all atomic platforms, encoded as a “spin cat” within ground state Zeeman levels. The key characteristic of our configuration is the coupling of the ground state spin manifold of size F g ≫ 1 to an excited Zeeman spin manifold of size F e = F g − 1 using light. This coupling results in eigenstates of the driven atom that include exactly two dark states in the ground state manifold, which are decoupled from light and immune to spontaneous emission from the excited states. These dark states constitute the spin cat, leading to the designation “dark spin cat.” We demonstrate that under strong Rabi drive and for large F g , the dark spin cat is autonomously stabilized against common noise sources and encodes a qubit with significantly biased noise. Specifically, the bit-flip error rate decreases exponentially with F g relative to the dephasing rate. We provide an analysis of dark spin cats and their robustness to noise, and we discuss bias-preserving single qubit and entangling gates, exemplified on a Rydberg tweezer platform.}, archive = {J_PRL}, author = {Andreas Kruckenhauser and Ming Yuan and Han Zheng and Mikhail Mamaev and Pei Zeng and Xuanhui Mao and Qian Xu and Torsten V. Zache and Liang Jiang and Rick van Bijnen and Peter Zoller}, doi = {10.1103/w9zh-jwsx}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020601}, shortjournal = {Phys. Rev. Lett.}, title = {Dark spin-cat states as biased qubits}, volume = {135}, year = {2025}, }
• (2025). Local properties of the rapidity distribution in the lieb-liniger model. PRL, 135(2), 020408. (www)

  @article{ , abstract = {We study the rapidity distribution in the Lieb–Liniger model and derive exact relations for its derivatives at the Fermi level. The latter enables us to treat analytically the free energy of the system at low temperatures and arbitrary interactions. We calculated the leading-order correction to the well-known result obtained using conformal field theory. In contrast to the leading-order term controlled by the sound velocity or the Luttinger liquid parameter, the new term is controlled by an additional dimensionless parameter. We calculated its series expansions in the limiting cases of weak and strong interactions. Our results are generalized to other Galilean-invariant integrable systems.}, archive = {J_PRL}, author = {Miłosz Panfil and Zoran Ristivojevic}, doi = {10.1103/hpfw-sfw1}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020408}, shortjournal = {Phys. Rev. Lett.}, title = {Local properties of the rapidity distribution in the lieb-liniger model}, volume = {135}, year = {2025}, }
• (2025). Counterdiabatic route to entanglement steering and dynamical freezing in the floquet lipkin-meshkov-glick model. PRL, 135(2), 020407. (www)

  @article{ , abstract = {Controlling the dynamics of quantum many-body systems is crucial for developing quantum technologies. This work demonstrates that counterdiabatic (CD) driving provides a powerful tool for steering collective spin systems along entangled trajectories for a long time. In particular, CD driving leads to approximate stroboscopic freezing and eternal entanglement oscillations for a large class of initial states in the periodically driven Lipkin-Meshkov-Glick model. Intriguingly, CD driving generates spin squeezing and its associated metrologically useful multipartite entanglement at the mid-point of every drive cycle, when the system is initially prepared in a fully x -polarized state. The CD driving induced nonergodic dynamics is accompanied by a decrease in the average eigenstate entanglement and inverse participation ratio, thereby signaling greater eigenstate localization. Our work opens a new route to evade Floquet heating and control entanglement generation in collective spin systems.}, archive = {J_PRL}, author = {Nakshatra Gangopadhay and Sayan Choudhury}, doi = {10.1103/bzcf-gm89}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020407}, shortjournal = {Phys. Rev. Lett.}, title = {Counterdiabatic route to entanglement steering and dynamical freezing in the floquet lipkin-meshkov-glick model}, volume = {135}, year = {2025}, }
• (2025). Exceptional stationary state in a dephasing many-body open quantum system. PRL, 135(2), 020406. (www)

  @article{ , abstract = {We study a dephasing many-body open quantum system that hosts, together with the infinite-temperature state, another additional stationary state, that is associated with a nonextensive strong symmetry. This state, that is a pure dark state, is exceptional in that it retains memory of the initial condition, whereas any orthogonal state evolves toward the infinite-temperature state erasing any information on the initial state. We discuss the approach to stationarity of the model focusing in particular on the fate of interfaces between the two states. A simple model based on a membrane picture helps developing an effective large-scale theory, which is different from the usual hydrodynamics since no extensive conserved quantities are present. The fact that the model reaches stationary properties on timescales that diverge with the system size, while the Lindbladian gap is finite, is duly highlighted. We point out the reasons for considering these exceptional stationary states as quantum many-body scars in the open system framework.}, archive = {J_PRL}, author = {Alice Marché and Gianluca Morettini and Leonardo Mazza and Lorenzo Gotta and Luca Capizzi}, doi = {10.1103/zn9v-k73w}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020406}, shortjournal = {Phys. Rev. Lett.}, title = {Exceptional stationary state in a dephasing many-body open quantum system}, volume = {135}, year = {2025}, }
• (2025). Self-discharging mitigated quantum battery. PRL, 135(2), 020405. (www)

  @article{ , abstract = {As a quantum thermodynamic device that utilizes quantum systems for energy storage and delivery, the quantum battery (QB) is expected to offer revolutionary advantages in terms of increasing the charging power and the extractable work by using quantum resources. However, the ubiquitous decoherence in the microscopic world inevitably forces the QB to spontaneously lose its stored energy. This is called the self-discharging of the QB and severely limits its realization. We propose a QB scheme based on the nitrogen-vacancy center in diamond, where the electronic spin serves as the QB. Inspired by our finding that the coherent ergotropy decays more slowly than the incoherent ergotropy, we reveal a mechanism to enhance the inherent robustness of the QB to the self-discharging by improving the ratio of coherent ergotropy to total ergotropy. The unique hyperfine interaction between the electron and the native N 14 nucleus in our scheme allows one to coherently optimize this ratio. Mitigating the self-discharging and optimizing the extractable work simultaneously, our results pave the way for the practical realization of the QB.}, archive = {J_PRL}, author = {Wan-Lu Song and Ji-Ling Wang and Bin Zhou and Wan-Li Yang and Jun-Hong An}, doi = {10.1103/d9k1-75d4}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020405}, shortjournal = {Phys. Rev. Lett.}, title = {Self-discharging mitigated quantum battery}, volume = {135}, year = {2025}, }
• (2025). Quantum thermal analogs of electric circuits: A universal approach. PRL, 135(2), 020404. (www)

  @article{ , abstract = {In this Letter, we develop a panoramic schematic of quantum thermal analogs of electric circuits in the steady state regime. We establish the foundations of said premise by defining the analogs of Kirchhoff’s laws for heat currents and temperature gradients, as well as a quantum thermal step transformer. Using this, we develop two novel quantum thermal circuits, viz., quantum thermal super Wheatstone bridge and quantum thermal adder circuit, paving the way for the corresponding integrated circuits. We further show that our approach encompasses various circuits like thermal diode, transistor, and Wheatstone bridge. This sheds new light on the present architecture of quantum device engineering.}, archive = {J_PRL}, author = {Devvrat Tiwari and Samyadeb Bhattacharya and Subhashish Banerjee}, doi = {10.1103/5x8m-bhgd}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020404}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum thermal analogs of electric circuits: A universal approach}, volume = {135}, year = {2025}, }
• (2025). Pseudoentanglement from tensor networks. PRL, 135(2), 020403. (www)

  @article{ , abstract = {Pseudoentangled states are defined by their ability to hide their entanglement structure: they are indistinguishable from random states to any observer with polynomial resources, yet can have much less entanglement than random states. Existing constructions of pseudoentanglement based on phase and/or subset states are limited in the entanglement structures they can hide, e.g., the states may have low entanglement on a single cut, on all cuts at once, or on local cuts in one dimension. Here, we introduce new constructions of pseudoentangled states based on (pseudo)random tensor networks that afford much more flexibility in the achievable entanglement structures. We illustrate our construction with the simplest example of a matrix product state, realizable as a staircase circuit of pseudorandom unitary gates, which exhibits pseudo-area-law scaling of entanglement in one dimension. We then generalize our construction to arbitrary tensor network structures that admit an isometric realization. A notable application of this result is the construction of pseudoentangled “holographic” states whose entanglement entropy obeys a Ryu-Takayanagi “minimum-cut” formula, answering a question posed in Aaronson et al. [arXiv:2211.00747].}, archive = {J_PRL}, author = {Zihan Cheng and Xiaozhou Feng and Matteo Ippoliti}, doi = {10.1103/7p1r-r2p6}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020403}, shortjournal = {Phys. Rev. Lett.}, title = {Pseudoentanglement from tensor networks}, volume = {135}, year = {2025}, }
• (2025). Measuring decoherence due to quantum vacuum fluctuations. PRL, 135(2), 020402. (www)

  @article{ , abstract = {The interaction of a particle with vacuum fluctuations—which theoretically exist even in the complete absence of matter—can lead to observable irreversible decoherence if it were possible to switch on and off the particle charge suddenly. We compute the leading order decoherence effect for such a scenario and propose an experimental setup for its detection. Such a measurement might provide further insights into the nature of vacuum fluctuations and a novel precision test for the decoherence theory.}, archive = {J_PRL}, author = {Anirudh Gundhi and Hendrik Ulbricht}, doi = {10.1103/s5c9-zjt9}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020402}, shortjournal = {Phys. Rev. Lett.}, title = {Measuring decoherence due to quantum vacuum fluctuations}, volume = {135}, year = {2025}, }
• (2025). Matchgate circuits deeply thermalize. PRL, 135(2), 020401. (www)

  @article{ , abstract = {We study the ensemble of states generated by performing projective measurements on the output of a random matchgate (or free-fermionic) quantum circuit. We rigorously show that this “projected ensemble” exhibits deep thermalization: for large system sizes, it converges toward a universal ensemble that is uniform over the manifold of Gaussian fermionic states. As well as proving momentwise convergence of these ensembles, we demonstrate that the full distribution of any physical observable in the projected ensemble is close to its universal form in Wasserstein-1 distance, which we argue is an appropriate and efficiently computable measure of convergence when studying deep thermalization. Using this metric, we also numerically find that local matchgate circuits deeply thermalize after a timescale t ∼ L 2 set by the diffusive spreading of quantum information. Our work opens up new avenues to experimentally accessible protocols to probe the emergence of quantum statistical mechanics and benchmark quantum simulators.}, archive = {J_PRL}, author = {Mircea Bejan and Benjamin Béri and Max McGinley}, doi = {10.1103/v8kp-39ry}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020401}, shortjournal = {Phys. Rev. Lett.}, title = {Matchgate circuits deeply thermalize}, volume = {135}, year = {2025}, }
• (2025). Experimental characterization of quantumness using the uncertainty principle, coherence, and nonlocality. PRL, 135(2), 020201. (www)

  @article{ , abstract = {Heisenberg’s uncertainty principle, coherence, and Bell nonlocality have been individually examined through many experiments. In this Letter, we systematically characterize all of this quantumness in a unified manner. We first construct universal uncertainty relations to reveal intrinsic features of incompatible measurements, which include all the state-independent uncertainties as special cases. We further extend to witness both quantum coherence and Bell nonlocality. We finally perform experiments with unified two-photon states and validate the uncertainty principle, coherence, and Bell nonlocality within experimental error. Our methods for witnessing quantumness are valuable in characterizing quantum correlations in quantum information processing.}, archive = {J_PRL}, author = {Yan-Han Yang and Xin-Zhu Liu and Xing-Zhou Zheng and Jun-Li Jiang and Xue Yang and Shao-Ming Fei and Zhihao Ma and Zizhu Wang and Ming-Xing Luo}, doi = {10.1103/p5pd-749f}, journal = {Physical Review Letters}, month = {7}, number = {2}, pages = {020201}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental characterization of quantumness using the uncertainty principle, coherence, and nonlocality}, volume = {135}, year = {2025}, }
• (2025). Trushin et al. reply:. PRL, 135(1), 019602. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 019602 (2025)}, archive = {J_PRL}, author = {Egor Trushin and Steffen Fauser and Andreas Mölkner and Jannis Erhard and Andreas Görling}, doi = {10.1103/qhr1-788v}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {019602}, shortjournal = {Phys. Rev. Lett.}, title = {Trushin et al. reply:}, volume = {135}, year = {2025}, }
• (2025). Comment on “Accurate correlation potentials from the self-consistent random phase approximation”. PRL, 135(1), 019601. (www)

  @article{ , abstract = {Phys. Rev. Lett. 135, 019601 (2025)}, archive = {J_PRL}, author = {Chandra Shahi and John P. Perdew}, doi = {10.1103/9wpv-qlwk}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {019601}, shortjournal = {Phys. Rev. Lett.}, title = {Comment on “Accurate correlation potentials from the self-consistent random phase approximation”}, volume = {135}, year = {2025}, }
• (2025). Twisting-induced instabilities in double-helix chiral rods. PRL, 135(1), 018202. (www)

  @article{ , abstract = {Elastic rods exhibit complex, nonlinear mechanical behaviors, especially under combined axial tension and twisting. Our study focuses on the nonlinear response of double-helix chiral rods, structures that combine a cylindrical core with helically coiled reinforcements. Through experiments, analytical modeling, and finite element simulations, we reveal that twisting induces mechanical instabilities, leading to complex deformation patterns. These instabilities are heavily influenced by the interplay between the core and the helical reinforcements, with the resulting deformations showing strong sensitivity to geometric and material characteristics. The findings enhance our understanding of chiral rods, with potential applications in soft robotics and tunable optical devices.}, archive = {J_PRL}, author = {G. Risso and M. Isbled and D. Melancon and K. Bertoldi}, doi = {10.1103/62n4-s7qs}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {018202}, shortjournal = {Phys. Rev. Lett.}, title = {Twisting-induced instabilities in double-helix chiral rods}, volume = {135}, year = {2025}, }
• (2025). Machine learning potential for electrochemical interfaces with hybrid representation of dielectric response. PRL, 135(1), 018003. (www)

  @article{ , abstract = {Understanding electrochemical interfaces at a microscopic level is essential for elucidating important electrochemical processes in electrocatalysis, batteries, and corrosion. While ab initio simulations have provided valuable insights into model systems, the high computational cost limits their use in tackling complex systems of relevance to practical applications. Machine learning potentials offer a solution, but their application in electrochemistry remains challenging due to the difficulty in treating the dielectric response of electronic conductors and insulators simultaneously. In this Letter, we propose a hybrid framework of machine learning potentials that is capable of simulating metal-electrolyte interfaces by unifying the interfacial dielectric response accounting for local electronic polarization in electrolytes and nonlocal charge transfer in metal electrodes. We validate our method by reproducing the bell-shaped differential Helmholtz capacitance at the Pt(111)-electrolyte interface. Furthermore, we apply the machine learning potential to calculate the dielectric profile at the interface, providing new insights into electronic polarization effects. Our Letter lays the foundation for atomistic modeling of complex, realistic electrochemical interfaces using machine learning potential at ab initio accuracy.}, archive = {J_PRL}, author = {Jia-Xin Zhu and Jun Cheng}, doi = {10.1103/48ct-3jxm}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {018003}, shortjournal = {Phys. Rev. Lett.}, title = {Machine learning potential for electrochemical interfaces with hybrid representation of dielectric response}, volume = {135}, year = {2025}, }
• (2025). Near-infrared spectroscopic sensing of hydrogen order in ice XIII. PRL, 135(1), 018002. (www)

  @article{ , abstract = {We identify hydrogen ordering in ices spectroscopically in the near-infrared (NIR) range ( ) based on the example of ices V/XIII. Previously it was thought that hydrogen ordering can only be revealed on the basis of lattice phonons, i.e., intermolecular vibrations. Here we show differences in the overtone spectrum of the intramolecular OH-stretching vibration. This makes NIR spectroscopy the first remote sensing method that is sensitive to different orientations of the water dipoles within ice. As such it will allow for future observations of the hydrogen order of ices in space by the James-Webb Space Telescope or the JUICE mission.}, archive = {J_PRL}, author = {Christina M. Tonauer and Eva-Maria Köck and Raphael Henn and Christoph Kappacher and Christian W. Huck and Thomas Loerting}, doi = {10.1103/x2ph-yp2v}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {018002}, shortjournal = {Phys. Rev. Lett.}, title = {Near-infrared spectroscopic sensing of hydrogen order in ice XIII}, volume = {135}, year = {2025}, }
• (2025). Phyllotactic structures in radially growing spatial symmetry breaking systems. PRL, 135(1), 018001. (www)

  @article{ , abstract = {Phyllotactic patterns, where elements such as leaves, seeds, or droplets arrange along alternate spirals, are fascinating examples of complex structures encountered in nature. In botany, their symmetries develop when a new primordium periodically grows in the largest gap left between the previous one and the apex. Experiments using ferrofluid droplets have shown that phyllotactic patterns can also spontaneously form when identical elements repulsing each other are periodically released at a given distance from an injection center and are advected radially at a constant speed. Here, we show that phyllotactic structures can also genuinely develop in the large class of spatial symmetry breaking systems with an intrinsic wavelength in the case of radial growth. The constraint of maintaining a fixed wavelength between spots while expanding radially either diffusively or advectively generalizes the concept of temporal release of repulsing agents in botany to new classes of systems. We explore this on three different systems: numerically on two models describing reaction-driven phase transitions and spatial Turing patterns, respectively, and experimentally on chemical precipitation patterns. This paves the way to engineer new complex self-organized structures in a panoply of different systems, ranging from spinodal decomposition, chemical, biological or optical Turing structures, and Liesegang patterns, to name a few.}, archive = {J_PRL}, author = {G. Facchini and M. A. Budroni and G. Schuszter and Fabian Brau and A. De Wit}, doi = {10.1103/7tnn-pq49}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {018001}, shortjournal = {Phys. Rev. Lett.}, title = {Phyllotactic structures in radially growing spatial symmetry breaking systems}, volume = {135}, year = {2025}, }
• (2025). Photonic bilayer chern insulator with corner states. PRL, 135(1), 016903. (www)

  @article{ , abstract = {Photonic Chern insulators can be implemented in gyromagnetic photonic crystals with broken time-reversal (TR) symmetry. They exhibit gapless chiral edge states (CESs), enabling unidirectional propagation and demonstrating exceptional resilience to localization even in the presence of defects or disorders. However, when two Chern insulators with opposite Chern numbers are stacked together, this one-way nature can be nullified, causing the originally gapless CESs to become gapped. Recent theoretical works have proposed achieving such a topological phase transition in condensed matter systems using antiferromagnetic thin films such as MnBi 2 Te 4 or by coupling two quantum spin/anomalous Hall insulators, but these approaches have yet to be realized experimentally. In a bilayer gyromagnetic photonic crystal arranged in an antiferromagnetic layer configuration, our experimental observations reveal that interlayer coupling initiates a transition from a Chern insulating phase to a higher-order topological phase. This transition results in the gapping of CESs and triggers the emergence of corner states within the band gap. The corner mode energy within this gap originates from CES interactions, forming a Jackiw-Rebbi-type topological domain wall mode at the corner, which is expected to remain within the bulk band gap without relying on local symmetries such as chiral or particle-hole symmetry. These states exhibit heightened resilience against defects, distinguishing them from their TR-symmetric counterparts.}, archive = {J_PRL}, author = {Subhaskar Mandal and Ziyao Wang and Rimi Banerjee and Hau Tian Teo and Minggui Wei and Peiheng Zhou and Xiang Xi and Zhen Gao and Gui-Geng Liu and Baile Zhang}, doi = {10.1103/33mm-mx88}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016903}, shortjournal = {Phys. Rev. Lett.}, title = {Photonic bilayer chern insulator with corner states}, volume = {135}, year = {2025}, }
• (2025). Quantum orbital-state control of a neutral nitrogen-vacancy center at millikelvin temperatures. PRL, 135(1), 016902. (www)

  @article{ , abstract = {A neutral nitrogen-vacancy center ( ) is promising for realizing strong coupling with a single microwave photon due to its large electric field sensitivity, although it is susceptible to environmental phonon noise at 5 K. Decreasing the temperature to 15 mK results in a tenfold increase in orbital relaxation time compared to that at 5 K. Dynamical decoupling pulses significantly increase the orbital coherence time to more than , representing a 30-fold improvement compared to that without decoupling pulses. Based on these results, a single can reach the strong coupling regime when coupled with a high-impedance microwave resonator, thus opening up the possibility of microwave quantum electrodynamics using a single optically active defect center in diamond.}, archive = {J_PRL}, author = {Hodaka Kurokawa and Shintaro Nakazato and Toshiharu Makino and Hiromitsu Kato and Shinobu Onoda and Yuhei Sekiguchi and Hideo Kosaka}, doi = {10.1103/m1qx-xlpd}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016902}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum orbital-state control of a neutral nitrogen-vacancy center at millikelvin temperatures}, volume = {135}, year = {2025}, }
• (2025). Quasisymmetry-constrained spin ferromagnetism in altermagnets. PRL, 135(1), 016703. (www)

  @article{ , abstract = {Altermagnets break time-reversal symmetry, and their spin-orbit coupling (SOC) allows for an anomalous Hall effect (AHE) that depends on the direction of the Néel ordering vector. The AHE and the ferromagnetic spin moment share the same symmetry and hence are usually proportional. However, density functional theory (DFT) calculations find that the AHE exists with negligible ferromagnetic spin moment for some compounds, whereas it reaches sizable values for other altermagnets. By examining realistic minimal models for altermagnetism in which the DFT phenomenology is captured, we uncover a general SOC-enabled quasisymmetry, the uniaxial spin space group, that provides a natural explanation for the amplitude of the ferromagnetic spin moment across the vast range of different altermagnetic materials. Additionally, we derive analytic expressions for the magnetic anisotropy energy, providing a simple means of identifying the preferred Néel vector orientation for altermagnets.}, archive = {J_PRL}, author = {Mercè Roig and Yue Yu and Rune C. Ekman and Andreas Kreisel and Brian M. Andersen and Daniel F. Agterberg}, doi = {10.1103/839n-rckn}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016703}, shortjournal = {Phys. Rev. Lett.}, title = {Quasisymmetry-constrained spin ferromagnetism in altermagnets}, volume = {135}, year = {2025}, }
• (2025). Strong nonlinear response of strange metals. PRL, 135(1), 016503. (www)

  @article{ , abstract = {We show that nonlinear transport responses in strange metals are strong, larger by a factor of than in Fermi liquids. Within the two-dimensional Yukawa-Sachdev-Ye-Kitaev model of a Fermi surface with a spatially random coupling to a critical scalar, the third order conductivity is found to diverge as at low , indicating the existence of a voltage-temperature scaling regime in the conductance. Its frequency and orientation dependence contains information on relaxation times of heat and electron distribution deformations, providing a new set of tools to characterize strange metals.}, archive = {J_PRL}, author = {Serhii Kryhin and Subir Sachdev and Pavel A. Volkov}, doi = {10.1103/4jxd-z3pm}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016503}, shortjournal = {Phys. Rev. Lett.}, title = {Strong nonlinear response of strange metals}, volume = {135}, year = {2025}, }
• (2025). Toward numerically exact computation of conductivity in the thermodynamic limit of interacting lattice models. PRL, 135(1), 016502. (www)

  @article{ , abstract = {Computing dynamical response functions in interacting lattice models is a long-standing challenge in condensed matter physics. In view of recent results, the dc resistivity in the weak-coupling regime of the Hubbard model is of great interest, yet it is not fully understood. The challenge lies in having to work with large lattices while avoiding analytical continuation. The weak-coupling results were so far computed at the level of the Boltzmann theory and at the level of the Kubo bubble approximation, which neglects vertex corrections. Neither theory was so far rigorously proven to give exact results even at infinitesimal coupling, and the respective dc resistivity results differ greatly. In this Letter we develop, cross-check and apply two state-of-the-art methods for obtaining dynamical response functions. We compute the optical conductivity at weak coupling in the Hubbard model in a fully controlled way, in the thermodynamic limit, and without analytical continuation. We show that vertex corrections persist to infinitesimal coupling, with a constant ratio to the Kubo bubble. We connect our methods with the Boltzmann theory, and show that the latter applies additional approximations that lead to quantitatively incorrect scaling of with respect to the coupling constant.}, archive = {J_PRL}, author = {Jeremija Kovačević and Michel Ferrero and Jakša Vučičević}, doi = {10.1103/mm38-zttx}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016502}, shortjournal = {Phys. Rev. Lett.}, title = {Toward numerically exact computation of conductivity in the thermodynamic limit of interacting lattice models}, volume = {135}, year = {2025}, }
• (2025). Symmetry-based classification of exact flat bands in single and bilayer moiré systems. PRL, 135(1), 016501. (www)

  @article{ , abstract = {Landau levels have been central to the discovery of exotic quantum phases and their unprecedentedly deep roots in geometry and topology. A powerful concept called “vortexability” extends this framework to moiré systems. In this Letter, we show that vortexable systems support not only Landau-level-like flat bands but also entirely new types with distinct topological properties. Notably, while Landau levels have total Chern number , vortexable moiré systems can host flat bands with . We provide a complete classification of such exact flat bands in single and bilayer systems with Dirac or quadratic band crossings, identifying the symmetry conditions that govern their number and topology. Up to six flat bands can be symmetry protected. We construct explicit wave functions, showing that sublattice-polarized states always sum to Chern number and satisfy ideal non-Abelian quantum geometry. When the Berry curvature is sharply peaked, we show that a topological heavy-fermion description remains valid—even for bands with high degeneracy.}, archive = {J_PRL}, author = {Siddhartha Sarkar and Xiaohan Wan and Shi-Zeng Lin and Kai Sun}, doi = {10.1103/nys8-5mg2}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016501}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry-based classification of exact flat bands in single and bilayer moiré systems}, volume = {135}, year = {2025}, }
• (2025). Quantum phases and transitions of bosons on a comb lattice. PRL, 135(1), 016001. (www)

  @article{ , abstract = {Motivated to elucidate the nature of quantum phases and their criticality when entangled with a correlated quantum bath, we study interacting bosons on a “comb lattice”—a one-dimensional backbone (system) coupled at its sites to otherwise independent one-dimensional “teeth” chains (bath). We map out the corresponding phase diagram, detailing the nature of the phases and phase transitions. Controlled by the backbone and teeth hopping amplitudes, short-range interactions, and chemical potential, phases include a Mott insulator, backbone, and teeth Luttinger liquids and the long-range ordered incoherent superfluid. We explore their properties and potential realizations in condensed matter and cold-atom experiments and simulations.}, archive = {J_PRL}, author = {Leo Radzihovsky and Emil Pellett}, doi = {10.1103/dljc-j3z7}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {016001}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum phases and transitions of bosons on a comb lattice}, volume = {135}, year = {2025}, }
• (2025). Particle acceleration in collisionless magnetically arrested disks. PRL, 135(1), 015201. (www)

  @article{ , abstract = {We present the first collisionless realization of two-dimensional axisymmetric black hole accretion consistent with a persistent magnetically arrested disk state. The accretion flow, consisting of an ion-electron disk plasma combined with magnetospheric pair creation effects, is simulated using first-principles general-relativistic particle-in-cell methods. The simulation is evolved over significant dynamical timescales during which a quasisteady accretion state is reached with several magnetic flux eruption cycles. We include a realistic treatment of inverse Compton scattering and pair production, which allows for studying the interaction between the collisionless accretion flow and pair-loaded jet. Our findings indicate that magnetic flux eruptions associated with equatorial magnetic reconnection within the black hole magnetosphere and the formation of spark gaps are locations of maximal particle acceleration. Flux eruptions, starting near the central black hole, can trigger Kelvin-Helmholtz-like vortices at the jet-disk interface that facilitate efficient mixing between disk and jet plasma in this region. Transient periods of increased pair production following magnetic flux eruptions and reconnection events are responsible for most of the highly accelerated particles.}, archive = {J_PRL}, author = {Jesse Vos and Benoît Cerutti and Monika Mościbrodzka and Kyle Parfrey}, doi = {10.1103/5wwb-7t2n}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {015201}, shortjournal = {Phys. Rev. Lett.}, title = {Particle acceleration in collisionless magnetically arrested disks}, volume = {135}, year = {2025}, }
• (2025). Photonic rabi oscillations in defective plasma photonic crystals. PRL, 135(1), 015101. (www)

  @article{ , abstract = {The Rabi oscillation effect, which is among the most celebrated quantum phenomena arising from the wave nature of matter, has been widely studied in two-level quantum systems, superconductors, Bose-Einstein condensates, and photonic crystals. Here we show that the Rabi oscillation can be achieved in a laser-plasma system, in which a femtosecond probe laser pulse interacts with a defective plasma photonic crystal (PPC). The defective PPC is formed in underdense plasma irradiated by two groups of two-color driver laser pulses. By changing the plasma and driver laser parameters, the photonic band structure of defective PPCs as well as the Rabi oscillation frequency of a trapped probe laser pulse can be tuned flexibly. Moreover, the Rabi oscillation may result in the ladder climbing of trapped laser intensity by use of multiple probe pulses in the defective PPC. This not only provides a novel plasma optical approach to investigate the Rabi oscillation in a new system, but also offers a new route to manipulate the propagation of intense laser pulses for various applications.}, archive = {J_PRL}, author = {Xiao-Bo Zhang and Su-Ming Weng and Hong Ai and Xin Qiao and Ju-Kui Xue and Zheng-Ming Sheng}, doi = {10.1103/k2th-m73q}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {015101}, shortjournal = {Phys. Rev. Lett.}, title = {Photonic rabi oscillations in defective plasma photonic crystals}, volume = {135}, year = {2025}, }
• (2025). Wave-kinetic dynamics of forced-dissipated turbulent internal gravity waves. PRL, 135(1), 014101. (www)

  @article{ , abstract = {Internal gravity waves are an essential feature of stratified media, such as oceans and atmospheres. To investigate their dynamics, we perform simulations of the forced-dissipated kinetic equation describing the evolution of the energy spectrum of weakly nonlinear internal gravity waves. During the early evolution, three well-known nonlocal interactions, the elastic scattering, the induced diffusion, and the parametric subharmonic instability, together with a superharmonic resonance play a prominent role. In contrast, local interactions are responsible for anisotropic energy cascade on longer timescales. We reveal emergence of a condensate at small horizontal wave vectors that can be interpreted as a pure wave-wave interaction-mediated layering process.}, archive = {J_PRL}, author = {Vincent Labarre and Giorgio Krstulovic and Sergey Nazarenko}, doi = {10.1103/b82h-z21n}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {014101}, shortjournal = {Phys. Rev. Lett.}, title = {Wave-kinetic dynamics of forced-dissipated turbulent internal gravity waves}, volume = {135}, year = {2025}, }
• (2025). Structured squeezed light allows for high-harmonic generation in classical forbidden geometries. PRL, 135(1), 013801. (www)

  @article{ , abstract = {High-harmonic generation (HHG) is a nonlinear process in which a strong driving field interacts with a material, resulting in the frequency up-conversion of the driver into its high-order harmonics. This process is highly sensitive to the field’s polarization: circular polarization, for instance, inhibits HHG. In this Letter, we demonstrate that the use of nonclassical structured light enables HHG in this otherwise prohibitive configuration for classical drivers. We consider circularly polarized light with nonclassical fluctuations, introduced via squeezing along one polarization direction, and show that these nonclassical features prompt the HHG process. We find that the spectral properties of the emitted harmonics depend on the type of squeezing applied and, by analyzing the inner electron dynamics, we relate the observed differences to modifications of the HHG three-step mechanism induced by the specific squeezing type. This approach opens new pathways for integrating quantum optics in HHG, providing novel means of controlling the light-matter interaction dynamics.}, archive = {J_PRL}, author = {J. Rivera-Dean and P. Stammer and M. F. Ciappina and M. Lewenstein}, doi = {10.1103/4hdl-bdwj}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {013801}, shortjournal = {Phys. Rev. Lett.}, title = {Structured squeezed light allows for high-harmonic generation in classical forbidden geometries}, volume = {135}, year = {2025}, }
• (2025). Thermal effects in the casimir torque between birefringent plates. PRL, 135(1), 013602. (www)

  @article{ , abstract = {The Casimir effect, originating from quantum and thermal fluctuations, is well known for inducing forces between closely spaced surfaces. When these surfaces are optically anisotropic, these interactions can produce a Casimir torque that rotates the surfaces relative to each other. We investigate, for the first time, the influence of thermal fluctuations on the Casimir torque between birefringent plates. Our results reveal that thermal modes significantly diminish the torque, with reductions up to 2 orders of magnitude for highly birefringent materials. Temperature is also shown to alter the angular dependence of the torque, significantly deviating from the typical sinusoidal behavior, and becomes particularly important at large separations that exceed the thermal wavelength. Finally, we demonstrate that systems of dissimilar birefringent plates that exhibit a distance-dependent reversal in the torque’s directions can enable precise control of the torque’s magnitude and sign through temperature manipulation. These findings advance our understanding of quantum and thermal fluctuation interplay and provide a framework for designing innovative nanoscale sensors and devices leveraging Casimir torque phenomena.}, archive = {J_PRL}, author = {Benjamin Spreng and Jeremy N. Munday}, doi = {10.1103/32gq-dbms}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {013602}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal effects in the casimir torque between birefringent plates}, volume = {135}, year = {2025}, }
• (2025). Observation of non-markovian radiative phenomena in structured photonic lattices. PRL, 135(1), 013601. (www)

  @article{ , abstract = {The spectral structure of a photonic reservoir shapes radiation phenomena for embedded quantum emitters. We implement an all-optical analog to study such an effect, particularly to observe the non-Markovian radiation dynamics of an emitter coupled to two-dimensional structured reservoirs. Its dynamics is simulated by light propagating through a photonic lattice, acting as a reservoir for an adjacent waveguide that mimics a coupled quantum emitter. We study radiation dynamics in square and Lieb lattices under different coupling regimes and observe how the flat band properties of the Lieb lattice significantly enhances light-matter coupling and non-Markovianity. Our platform opens a path for the experimental exploration of single-photon quantum optical phenomena in structured reservoirs to enhance light-matter interactions.}, archive = {J_PRL}, author = {Rodrigo A. Vicencio and Fabiola G. L. Cárcamo-Macaya and Diego Román-Cortés and Pablo Solano}, doi = {10.1103/b3kw-vv3s}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {013601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of non-markovian radiative phenomena in structured photonic lattices}, volume = {135}, year = {2025}, }
• (2025). Z=14 magicity revealed by the mass of the proton dripline nucleus si22. PRL, 135(1), 012501. (www)

  @article{ , abstract = {Using the -defined isochronous mass spectrometry technique, we conducted the first mass measurement of the proton dripline nucleus . We confirm that is bound against particle emission with , fixing the proton dripline location for the Si element. By analyzing the mass differences of the neighboring -shell nuclei, we find that exhibits a doubly magic character similar to its mirror partner , and that the mirror energy difference of deviates from the predictions assuming mirror symmetry. Gamow shell-model calculations reveal that the average occupations of valence protons in are nearly identical to those of valence neutrons in , supporting the magicity in . The observed mirror-symmetry breaking is attributed to the extended proton distribution in arising from a small contribution of the unbound orbital.}, archive = {J_PRL}, author = {Y. M. Xing and Y. F. Luo and Y. H. Zhang and M. Wang and X. H. Zhou and J. G. Li and K. H. Li and Q. Yuan and Y. F. Niu and J. Y. Guo and J. C. Pei and F. R. Xu and G. de Angelis and Yu. A. Litvinov and K. Blaum and I. Tanihata and T. Yamaguchi and Y. Yu and X. Zhou and H. S. Xu and Z. Y. Chen and R. J. Chen and H. Y. Deng and C. Y. Fu and W. W. Ge and W. J. Huang and H. Y. Jiao and H. F. Li and T. Liao and J. Y. Shi and M. Si and M. Z. Sun and P. Shuai and X. L. Tu and Q. Wang and X. Xu and X. L. Yan and Y. J. Yuan and M. Zhang}, doi = {10.1103/ffwt-n7yc}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {012501}, shortjournal = {Phys. Rev. Lett.}, title = {Z=14 magicity revealed by the mass of the proton dripline nucleus si22}, volume = {135}, year = {2025}, }
• (2025). Exploiting ne20 isotopes for precision characterizations of collectivity in small systems. PRL, 135(1), 012302. (www)

  @article{ , abstract = {Whether or not femto-scale droplets of quark-gluon plasma (QGP) are formed in so-called small systems at high-energy colliders is a pressing question in the phenomenology of the strong interaction. For proton-proton or proton-nucleus collisions the answer is inconclusive due to the large theoretical uncertainties plaguing the description of these processes. While upcoming data on collisions of O 16 nuclei may mitigate these uncertainties in the near future, here we demonstrate the unique possibilities offered by complementing O 16 + O 16 data with collisions of Ne 20 ions. We couple both nuclear lattice effective field theory (NLEFT) and projected generator coordinate method (PGCM) ab initio descriptions of the structure of Ne 20 and O 16 to hydrodynamic simulations of O 16 + O 16 and Ne 20 + Ne 20 collisions at high energy. We isolate the imprints of the bowling-pin shape of Ne 20 on the collective flow of hadrons, which can be used to perform quantitative tests of the hydrodynamic QGP paradigm. In particular, we predict that the elliptic flow of Ne 20 + Ne 20 collisions is enhanced by as much as 1.174 ( 8 ) stat ( 31 ) syst for NLEFT and 1.139 ( 6 ) stat ( 39 ) syst for PGCM relative to O 16 + O 16 collisions for the 1% most central events. At the same time, theoretical uncertainties largely cancel when studying relative variations of observables between two systems. This demonstrates a method based on experiments with two light-ion species for precision characterizations of the collective dynamics and its emergence in a small system.}, archive = {J_PRL}, author = {Giuliano Giacalone and Benjamin Bally and Govert Nijs and Shihang Shen and Thomas Duguet and Jean-Paul Ebran and Serdar Elhatisari and Mikael Frosini and Timo A. Lähde and Dean Lee and Bing-Nan Lu and Yuan-Zhuo Ma and Ulf-G. Meißner and Jacquelyn Noronha-Hostler and Christopher Plumberg and Tomás R. Rodríguez and Robert Roth and Wilke van der Schee and Vittorio Somà}, doi = {10.1103/k8rb-jgvq}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {012302}, shortjournal = {Phys. Rev. Lett.}, title = {Exploiting ne20 isotopes for precision characterizations of collectivity in small systems}, volume = {135}, year = {2025}, }
• (2025). Effective-range expansion with a long-range force. PRL, 135(1), 011903. (www)

  @article{ , abstract = {The validity range of the time-honored effective range expansion can be very limited due to the presence of a left-hand cut close to the two-particle threshold. Such a left-hand cut arises in the two-particle interaction involving a light particle exchange with a small mass or a mass slightly heavier than the mass difference of the two particles, identified as a long-range force, a scenario encountered in a broad range of systems. This can hinder a precise extraction of low-energy scattering observables and resonance poles. To address this issue, we propose a new parametrization for the low-energy scattering amplitude that accounts for the left-hand cut. The parametrization is like a Padé approximation but with nonanalytic terms from the left-hand cut and can be regarded as an extension of the effective range expansion. This parametrization is versatile and applicable to a broad range of systems with Yukawa-type interactions, including particle, hadronic, nuclear, cold atom, and quantum gas systems. In particular, it should be invaluable in understanding various near-threshold hadron resonances. As byproducts, we also show that the parametrization can be used to extract the couplings of the exchanged particle to the scattering particles, and derive expressions for amplitude zeros caused by the interplay between the short- and long-range interactions.}, archive = {J_PRL}, author = {Meng-Lin Du and Feng-Kun Guo and Bing Wu}, doi = {10.1103/cwdt-dj6z}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011903}, shortjournal = {Phys. Rev. Lett.}, title = {Effective-range expansion with a long-range force}, volume = {135}, year = {2025}, }
• (2025). Bell inequality violation of light quarks in dihadron pair production at lepton colliders. PRL, 135(1), 011902. (www)

  @article{ , abstract = {Spin correlations between particles produced at colliders provide valuable insights for quantum information studies. While traditional studies of quantum information at colliders are typically limited to massive particles with perturbative decay, we propose an innovative method to explore the Bell inequality in massless quark pair systems by analyzing the azimuthal correlations in π + π − dihadron pair production at lepton colliders. Revisiting the Belle data, we have shown the potential to detect Bell inequality violation of light quarks by introducing an additional angular cut, achieving a significance of 2.5 σ even in the worst-case scenario of 100% correlated systematic uncertainties in each bin. The significance substantially exceeds 5 σ when considering uncorrelated systematic uncertainties. Our approach opens avenues for exploring spin quantum information with nonperturbative processes as spin analyzer and leverages existing data for quantum information research.}, archive = {J_PRL}, author = {Kun Cheng and Bin Yan}, doi = {10.1103/gmqz-v4cl}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011902}, shortjournal = {Phys. Rev. Lett.}, title = {Bell inequality violation of light quarks in dihadron pair production at lepton colliders}, volume = {135}, year = {2025}, }
• (2025). Hadronic vacuum polarization for the muon g−2 from lattice QCD: Long-distance and full light-quark connected contribution. PRL, 135(1), 011901. (www)

  @article{ , abstract = {We present results for the dominant light-quark connected contribution to the long-distance window of the hadronic vacuum polarization (HVP) contribution to the muon g − 2 from lattice quantum chromodynamics. Specifically, with a new determination of the lattice scale on MILC’s physical-mass HISQ ensembles, using the Ω − baryon mass, we obtain a result of a μ l l , LD ( conn ) = 400.2 ( 2.3 ) stat ( 3.7 ) syst [ 4.3 ] total × 10 − 10 . Summing this result with our recent determinations of the light-quark connected contributions to the short- and intermediate-distance windows, we obtain a subpercent precision determination of the light-quark-connected contribution to HVP of a μ l l ( conn ) = 655.2 ( 2.3 ) stat ( 3.9 ) syst [ 4.5 ] total × 10 − 10 . Finally, as a consistency check, we verify that an independent analysis of the full contribution is in agreement with the sum of individual windows. We discuss our future plans for improvements of our HVP calculations to meet the target precision of the Fermilab g − 2 experiment.}, archive = {J_PRL}, author = {Fermilab Lattice, HPQCD, and MILC Collaborations and Alexei Bazavov and Claude W. Bernard and David A. Clarke and Christine Davies and Carleton DeTar and Aida X. El-Khadra and Elvira Gámiz and Steven Gottlieb and Anthony V. Grebe and Leon Hostetler and William I. Jay and Hwancheol Jeong and Andreas S. Kronfeld and Shaun Lahert and Jack Laiho and G. Peter Lepage and Michael Lynch and Andrew T. Lytle and Craig McNeile and Ethan T. Neil and Curtis T. Peterson and James N. Simone and Jacob W. Sitison and Ruth S. Van de Water and Alejandro Vaquero}, doi = {10.1103/d583-yhfs}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011901}, shortjournal = {Phys. Rev. Lett.}, title = {Hadronic vacuum polarization for the muon g−2 from lattice QCD: Long-distance and full light-quark connected contribution}, volume = {135}, year = {2025}, }
• (2025). Dark matter internal pair production: A novel direct detection mechanism. PRL, 135(1), 011804. (www)

  @article{ , abstract = {We introduce a new dark matter detection mechanism, dark matter internal pair production (DIPP), to detect dark matter candidates at beam dump facilities. When energetic dark matter scatters in a material, it can create a lepton-antilepton pair by exchanging a virtual photon with the nucleus, akin to the neutrino trident process. We demonstrate this process for dark matter coupled to dark photons in experiments such as DarkQuest, SBND, and DUNE ND. Since the lepton-antilepton pair carries a significant fraction of dark matter energy, it can be clearly distinguished from backgrounds. Utilizing the above features, we show that DIPP is highly effective at probing various dark matter models, particularly at DUNE ND and DarkQuest, by searching for electron-positron and muon-antimuon signatures. At DUNE ND, we find that the sensitivity of DIPP extends over a larger parameter space than the existing limits from electron and nuclear recoil. Additionally, we explore a scenario where dark sector couplings involve quarks and muons only, demonstrating that DIPP can probe a wide variety of dark matter models with different final states.}, archive = {J_PRL}, author = {Bhaskar Dutta and Aparajitha Karthikeyan and Mudit Rai and Hyunyong Kim}, doi = {10.1103/ry3x-dw48}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011804}, shortjournal = {Phys. Rev. Lett.}, title = {Dark matter internal pair production: A novel direct detection mechanism}, volume = {135}, year = {2025}, }
• (2025). Enhancing DUNE’s solar neutrino capabilities with neutral-current detection. PRL, 135(1), 011803. (www)

  @article{ , abstract = {We show that the Deep Underground Neutrino Experiment (DUNE) has the potential to make a precise measurement of the total active flux of B 8 solar neutrinos via neutral-current (NC) interactions with argon. This would complement proposed precise measurements of solar-neutrino fluxes in DUNE via charged-current (CC) interactions with argon and mixed CC / NC interactions with electrons. Together, these would enable DUNE to make a Sudbury Neutrino Observatory (SNO)-like comparison of rates and thus to make the most precise measurements of sin 2 θ 12 and Δ m 21 2 using solar neutrinos. Realizing this potential requires dedicated but realistic efforts to improve DUNE’s low-energy capabilities and separately to reduce neutrino-argon cross-section uncertainties. Comparison of mixing-parameter results obtained using solar neutrinos in DUNE and reactor antineutrinos in the Jiangmen Underground Neutrino Observatory (JUNO) would allow for unprecedented tests of new physics.}, archive = {J_PRL}, author = {Stephan A. Meighen-Berger and Jayden L. Newstead and John F. Beacom and Nicole F. Bell and Matthew J. Dolan}, doi = {10.1103/htfm-tbdq}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011803}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing DUNE’s solar neutrino capabilities with neutral-current detection}, volume = {135}, year = {2025}, }
• (2025). Dark matter search results from 4.2 Tonne−Years of exposure of the LUX-ZEPLIN (LZ) experiment. PRL, 135(1), 011802. (www)

  @article{ , abstract = {We report results of a search for nuclear recoils induced by weakly interacting massive particle (WIMP) dark matter using the LUX-ZEPLIN (LZ) two-phase xenon time projection chamber. This analysis uses a total exposure of tonne-years from 280 live days of LZ operation, of which tonne-years and 220 live days are new. A technique to actively tag background electronic recoils from decays is featured for the first time. Enhanced electron-ion recombination is observed in two-neutrino double electron capture decays of , representing a noteworthy new background. After removal of artificial signal-like events injected into the dataset to mitigate analyzer bias, we find no evidence for an excess over expected backgrounds. World-leading constraints are placed on spin-independent (SI) and spin-dependent WIMP-nucleon cross sections for masses . The strongest SI exclusion set is at the 90% confidence level and the best SI median sensitivity achieved is , both for a mass of .}, archive = {J_PRL}, author = {LZ Collaboration and J. Aalbers and D. S. Akerib and A. K. Al Musalhi and F. Alder and C. S. Amarasinghe and A. Ames and T. J. Anderson and N. Angelides and H. M. Araújo and J. E. Armstrong and M. Arthurs and A. Baker and S. Balashov and J. Bang and J. W. Bargemann and E. E. Barillier and D. Bauer and K. Beattie and T. Benson and A. Bhatti and A. Biekert and T. P. Biesiadzinski and H. J. Birch and E. Bishop and G. M. Blockinger and B. Boxer and C. A. J. Brew and P. Brás and S. Burdin and M. Buuck and M. C. Carmona-Benitez and M. Carter and A. Chawla and H. Chen and J. J. Cherwinka and Y. T. Chin and N. I. Chott and M. V. Converse and R. Coronel and A. Cottle and G. Cox and D. Curran and C. E. Dahl and I. Darlington and S. Dave and A. David and J. Delgaudio and S. Dey and L. de Viveiros and L. Di Felice and C. Ding and J. E. Y. Dobson and E. Druszkiewicz and S. Dubey and S. R. Eriksen and A. Fan and S. Fayer and N. M. Fearon and N. Fieldhouse and S. Fiorucci and H. Flaecher and E. D. Fraser and T. M. A. Fruth and R. J. Gaitskell and A. Geffre and J. Genovesi and C. Ghag and A. Ghosh and R. Gibbons and S. Gokhale and J. Green and M. G. D. van der Grinten and J. J. Haiston and C. R. Hall and T. J. Hall and S. Han and E. Hartigan-O’Connor and S. J. Haselschwardt and M. A. Hernandez and S. A. Hertel and G. Heuermann and G. J. Homenides and M. Horn and D. Q. Huang and D. Hunt and E. Jacquet and R. S. James and J. Johnson and A. C. Kaboth and A. C. Kamaha and Meghna K. K and D. Khaitan and A. Khazov and I. Khurana and J. Kim and Y. D. Kim and J. Kingston and R. Kirk and D. Kodroff and L. Korley and E. V. Korolkova and H. Kraus and S. Kravitz and L. Kreczko and V. A. Kudryavtsev and C. Lawes and D. S. Leonard and K. T. Lesko and C. Levy and J. Lin and A. Lindote and W. H. Lippincott and M. I. Lopes and W. Lorenzon and C. Lu and S. Luitz and P. A. Majewski and A. Manalaysay and R. L. Mannino and C. Maupin and M. E. McCarthy and G. McDowell and D. N. McKinsey and J. McLaughlin and J. B. McLaughlin and R. McMonigle and E. Mizrachi and A. Monte and M. E. Monzani and J. D. Morales Mendoza and E. Morrison and B. J. Mount and M. Murdy and A. St. J. Murphy and A. Naylor and H. N. Nelson and F. Neves and A. Nguyen and C. L. O’Brien and I. Olcina and K. C. Oliver-Mallory and J. Orpwood and K. Y Oyulmaz and K. J. Palladino and J. Palmer and N. J. Pannifer and N. Parveen and S. J. Patton and B. Penning and G. Pereira and E. Perry and T. Pershing and A. Piepke and Y. Qie and J. Reichenbacher and C. A. Rhyne and A. Richards and Q. Riffard and G. R. C. Rischbieter and E. Ritchey and H. S. Riyat and R. Rosero and T. Rushton and D. Rynders and D. Santone and A. B. M. R. Sazzad and R. W. Schnee and G. Sehr and B. Shafer and S. Shaw and T. Shutt and J. J. Silk and C. Silva and G. Sinev and J. Siniscalco and R. Smith and V. N. Solovov and P. Sorensen and J. Soria and I. Stancu and A. Stevens and K. Stifter and B. Suerfu and T. J. Sumner and M. Szydagis and D. R. Tiedt and M. Timalsina and Z. Tong and D. R. Tovey and J. Tranter and M. Trask and M. Tripathi and A. Usón and A. Vacheret and A. C. Vaitkus and O. Valentino and V. Velan and A. Wang and J. J. Wang and Y. Wang and J. R. Watson and L. Weeldreyer and T. J. Whitis and K. Wild and M. Williams and W. J. Wisniewski and L. Wolf and F. L. H. Wolfs and S. Woodford and D. Woodward and C. J. Wright and Q. Xia and J. Xu and Y. Xu and M. Yeh and D. Yeum and W. Zha and E. A. Zweig}, doi = {10.1103/4dyc-z8zf}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011802}, shortjournal = {Phys. Rev. Lett.}, title = {Dark matter search results from 4.2 Tonne−Years of exposure of the LUX-ZEPLIN (LZ) experiment}, volume = {135}, year = {2025}, }
• (2025). Novel approach to investigate ATOMKI anomaly using coherent CAPTAIN-mills detectors. PRL, 135(1), 011801. (www)

  @article{ , abstract = {ATOMKI nuclear anomaly has suggested a new BSM (beyond the standard model) boson with mass emitted from excited nuclei and quickly decays into a pair of . In order to search for the new particle, we propose a new approach that utilizes the ongoing coherent CAPTAIN-Mills (CCM) ten-ton LAr (liquid argon) detectors. The neutrons from the Lujan target can scatter inelastically, but the PMT glass in the CCM detector can produce the new boson which solves the ATOMKI anomaly. The new boson can be detected from its decay to a pair. We find that CCM probes a large area of the anomaly-allowable parameter space. We also show the prediction for a 100-ton LAr detector and five-ton EOS water detector.}, archive = {J_PRL}, author = {Bhaskar Dutta and Bai-Shan Hu and Wei-Chih Huang and Richard G. Van de Water}, doi = {10.1103/34pk-53tf}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011801}, shortjournal = {Phys. Rev. Lett.}, title = {Novel approach to investigate ATOMKI anomaly using coherent CAPTAIN-mills detectors}, volume = {135}, year = {2025}, }
• (2025). Preponderant orbital polarization in relativistic magnetovortical matter. PRL, 135(1), 011601. (www)

  @article{ , abstract = {We establish thermodynamic stability and gauge invariance in the magnetovortical matter of Dirac fermions under the coexistent rotation and strong magnetic field. The corresponding partition function reveals that the orbital contribution to bulk thermodynamics preponderates over the conventional contribution from anomaly-related spin effects. This orbital preponderance macroscopically manifests itself in the sign inversion of the induced charge and current in the magnetovortical matter, and can be tested experimentally as the flip of the angular momentum polarization of magnetovortical matter when the magnetic field strength is increased.}, archive = {J_PRL}, author = {Kenji Fukushima and Koichi Hattori and Kazuya Mameda}, doi = {10.1103/PhysRevLett.135.011601}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011601}, shortjournal = {Phys. Rev. Lett.}, title = {Preponderant orbital polarization in relativistic magnetovortical matter}, volume = {135}, year = {2025}, }
• (2025). Absorption of fermionic dark matter in the PICO-60 C3F8 bubble chamber. PRL, 135(1), 011001. (www)

  @article{ , abstract = {Fermionic dark matter absorption on nuclear targets via neutral current interactions is explored using a nonrelativistic effective field theory framework. An analysis of data from the PICO-60 C 3 F 8 bubble chamber sets leading constraints on spin-independent absorption for dark matter masses below 23 MeV / c 2 and establishes the first limits on spin-dependent absorptive interactions. These results demonstrate the sensitivity of bubble chambers to low-mass dark matter and underscore the importance of absorption searches in expanding the parameter space of direct detection experiments.}, archive = {J_PRL}, author = {PICO Collaboration and E. Adams and B. Ali and R. Anderson-Dornan and I. J. Arnquist and M. Bai and D. Baxter and E. Behnke and B. Broerman and C. J. Chen and K. Clark and J. I. Collar and P. S. Cooper and D. Cranshaw and C. Cripe and M. Crisler and C. E. Dahl and M. Das and S. Das and S. Fallows and J. Farine and R. Filgas and A. García-Viltres and G. Giroux and O. Harris and H. Hawley-Herrera and T. Hillier and E. W. Hoppe and C. M. Jackson and M. Jin and C. B. Krauss and M. Laurin and I. Lawson and A. Leblanc and H. Leng and I. Levine and C. Licciardi and W. H. Lippincott and Q. Malin and P. Mitra and V. Monette and C. Moore and R. Neilson and A. J. Noble and H. Nozard and S. Pal and M.-C. Piro and S. Priya and C. Rethmeier and M. Robert and A. E. Robinson and J. Savoie and S. J. Sekula and A. Sonnenschein and N. Starinski and I. Štekl and M. Tripathi and E. Vázquez-Jáuregui and U. Wichoski and W. Woodley and V. Zacek and J. Zhang}, doi = {10.1103/1cwz-m1c3}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {011001}, shortjournal = {Phys. Rev. Lett.}, title = {Absorption of fermionic dark matter in the PICO-60 C3F8 bubble chamber}, volume = {135}, year = {2025}, }
• (2025). Quantum teleportation from telecom photons to erbium-ion ensembles. PRL, 135(1), 010804. (www)

  @article{ , abstract = {To realize a quantum internet, the distribution of quantum states via quantum teleportation with quantum memories is a key ingredient. Being compatible with existing fiber networks, entangled photons and quantum memories at telecom wavelength are of central interest for such a scalable quantum network. Here, we demonstrate quantum teleportation from a telecom-wavelength photonic qubit to a solid-state quantum memory based on erbium-ion ensembles, which have a native optical transition at telecom C band. To accomplish this, we use chip-scale silicon nitride microresonators to generate entangled photons with narrow linewidth, compatible with the quantum memory. We confirm the quality of the quantum teleportation procedure using quantum state and process tomography techniques, in which both the quantum state and process fidelities exceeds the classical limit. These results pave the way for the realization of scalable quantum networks based on solid-state devices.}, archive = {J_PRL}, author = {Yu-Yang An and Qian He and Wenyi Xue and Ming-Hao Jiang and Chengdong Yang and Yan-Qing Lu and Shining Zhu and Xiao-Song Ma}, doi = {10.1103/3wh8-2gh1}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010804}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum teleportation from telecom photons to erbium-ion ensembles}, volume = {135}, year = {2025}, }
• (2025). Time-optimal transfer of the quantum state in long qubit arrays. PRL, 135(1), 010803. (www)

  @article{ , abstract = {Recent technological advances have allowed the fabrication of large arrays of coupled qubits, serving as prototypes for quantum processors. However, the optimal control of such systems remains notoriously challenging, limiting the potential of large-scale quantum systems. Here, we investigate a model problem of quantum state transfer in a large nearest-neighbor-coupled qubit array. We derive an optimal control strategy that simultaneously achieves maximal fidelity and minimal transfer time, reaching the quantum speed limit in a lattice with time-varying couplings.}, archive = {J_PRL}, author = {Andrei A. Stepanenko and Kseniia S. Chernova and Maxim A. Gorlach}, doi = {10.1103/mxrq-7rl4}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010803}, shortjournal = {Phys. Rev. Lett.}, title = {Time-optimal transfer of the quantum state in long qubit arrays}, volume = {135}, year = {2025}, }
• (2025). Practical framework for analyzing high-dimensional quantum key distribution setups. PRL, 135(1), 010802. (www)

  @article{ , abstract = {High-dimensional (HD) entanglement promises both enhanced key rates and overcoming obstacles faced by modern-day quantum communication. However, modern convex optimization-based security arguments are limited by computational constraints; thus, accessible dimensions are far exceeded by progress in HD photonics, bringing forth a need for efficient methods to compute key rates for large encoding dimensions. In response to this problem, we present a flexible analytic framework facilitated by the dual of a semidefinite program and diagonalizing operators inspired by entanglement-witness theory, enabling the efficient computation of key rates in high-dimensional systems. To facilitate the latter, we show how matrix completion techniques can be incorporated to effectively yield improved, computable bounds on the key rate in paradigmatic high-dimensional systems of time- or frequency-bin entangled photons and beyond, revealing the potential for very high-dimensions to surpass low dimensional protocols already with existing technology. In our accompanying work, (F. Kanitschar and M. Huber, Composable finite-size security of high-dimensional quantum key distribution protocols), available on arXiv, we show how our findings can be used to establish finite-size security against coherent attacks for general HD-QKD protocols both in the fixed- and variable-length scenario.}, archive = {J_PRL}, author = {Florian Kanitschar and Marcus Huber}, doi = {10.1103/PhysRevLett.135.010802}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010802}, shortjournal = {Phys. Rev. Lett.}, title = {Practical framework for analyzing high-dimensional quantum key distribution setups}, volume = {135}, year = {2025}, }
• (2025). Experimental quantum fingerprinting without the shared randomness loophole. PRL, 135(1), 010801. (www)

  @article{ , abstract = {Quantum fingerprinting (QF) promises exponential reduction of information transmission in executing communication complexity tasks. Practicality and quantum advantage of this novel protocol has been recently demonstrated using weak coherent pulses to carry the fingerprinting information. However, all coherent QF implementations rely upon a direct optical link to maintain coherence between the users, which does not comply with the protocol’s rule that the users must not have any access to a shared randomness. To close this loophole, we propose, and experimentally demonstrate, a novel protocol based on asynchronous coincidence pairing from the interference result between coherent optical fields that are remotely and independently prepared. Over a length of 20 km telecom fiber, our QF setup has outperformed the best-known classical algorithm, for the first time without being susceptible to shared randomness. Our result paves the way toward practical applications of QF in communication complexity.}, archive = {J_PRL}, author = {Ao Shen and Yu-Shuo Lu and Xiping Wu and Jinping Lin and Xiao-Yu Cao and Chengfang Ge and Shan-Feng Shao and Hua-Lei Yin and Lai Zhou and Zhiliang Yuan}, doi = {10.1103/v1fc-q1n9}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010801}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental quantum fingerprinting without the shared randomness loophole}, volume = {135}, year = {2025}, }
• (2025). Quantum algorithms for representation-theoretic multiplicities. PRL, 135(1), 010602. (www)

  @article{ , abstract = {Kostka, Littlewood-Richardson, Plethysm, and Kronecker coefficients are the multiplicities of irreducible representations in the decomposition of representations of the symmetric group that play an important role in representation theory, geometric complexity, and algebraic combinatorics. We give quantum algorithms for computing these coefficients whenever the ratio of dimensions of the representations is polynomial. We show that there is an efficient classical algorithm for computing the Kostka numbers under this restriction and conjecture the existence of an analogous algorithm for the Littlewood-Richardson coefficients. We argue why such classical algorithm does not straightforwardly work for the Plethysm and Kronecker coefficients and conjecture that our quantum algorithms lead to superpolynomial speedups. The conjecture about Kronecker coefficients was disproved by Panova [Polynomial time classical versus quantum algorithms for representation theoretic multiplicities, arXiv:2502.20253 ] with a classical algorithm which, if optimal, points to a O ( n 4 + 2 k ) vs Ω ˜ ( n 4 k 2 + 1 ) polynomial gap in quantum vs classical computational complexity for an integer parameter k .}, archive = {J_PRL}, author = {Martín Larocca and Vojtech Havlicek}, doi = {10.1103/k5tx-xtr3}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010602}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum algorithms for representation-theoretic multiplicities}, volume = {135}, year = {2025}, }
• (2025). Classical simulation of circuits with realistic odd-dimensional gottesman-kitaev-preskill states. PRL, 135(1), 010601. (www)

  @article{ , abstract = {Classically simulating circuits with bosonic codes is challenging due to the prohibitive cost of simulating quantum systems with many, possibly infinite, energy levels. We propose an algorithm to simulate circuits with encoded Gottesman-Kitaev-Preskill (GKP) states, specifically for odd-dimensional encoded qudits. Our approach is tailored to be especially effective in the most challenging but practically relevant regime, where the codeword states exhibit high (but finite) squeezing. Our algorithm leverages the Zak-Gross Wigner function introduced by Davis, Fabre, and Chabaud, which represents infinitely squeezed encoded stabilizer states positively. The run-time of the algorithm scales with the negativity of the Wigner function, allowing for efficient simulation of certain large-scale circuits—namely, input stabilizer GKP states undergoing generalized GKP-encoded Clifford operations followed by modular measurement—with a high degree of squeezing. For stabilizer GKP states exhibiting 12 dB of squeezing, our algorithm can simulate circuits with up to 1000 modes with less than double the number of samples required for a single input mode, which is in stark contrast to existing simulators. Therefore, this approach holds significant potential for benchmarking early implementations of quantum computing architectures utilizing bosonic codes.}, archive = {J_PRL}, author = {Cameron Calcluth and Oliver Hahn and Juani Bermejo-Vega and Alessandro Ferraro and Giulia Ferrini}, doi = {10.1103/xmtw-g54f}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010601}, shortjournal = {Phys. Rev. Lett.}, title = {Classical simulation of circuits with realistic odd-dimensional gottesman-kitaev-preskill states}, volume = {135}, year = {2025}, }
• (2025). Estimate of equilibration times of quantum correlation functions in the thermodynamic limit based on lanczos coefficients. PRL, 135(1), 010403. (www)

  @article{ , abstract = {We study the equilibration times of local observables in quantum chaotic systems by considering their autocorrelation functions. Based on the recursion method, we suggest a scheme to estimate from the corresponding Lanczos coefficients that is expected to hold in the thermodynamic limit. We numerically find that, if the observable eventually shows smoothly growing Lanczos coefficients, a finite number of the former is sufficient for a reasonable estimate of the equilibration time. This implies that equilibration occurs on a realistic time scale much shorter than the life of the Universe. The numerical findings are further supported by analytical arguments.}, archive = {J_PRL}, author = {Jiaozi Wang and Merlin Füllgraf and Jochen Gemmer}, doi = {10.1103/ztrj-2tm6}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010403}, shortjournal = {Phys. Rev. Lett.}, title = {Estimate of equilibration times of quantum correlation functions in the thermodynamic limit based on lanczos coefficients}, volume = {135}, year = {2025}, }
• (2025). Quantum dynamics with stochastic non-hermitian hamiltonians. PRL, 135(1), 010402. (www)

  @article{ , abstract = {We study the quantum dynamics generated by a non-Hermitian Hamiltonian subject to stochastic perturbations in its anti-Hermitian part, describing fluctuating gains and losses. The dynamics averaged over the noise is described by an “antidephasing” master equation. We characterize the resulting state evolution and analyze its purity. The properties of such dynamics are illustrated in a stochastic dissipative qubit. Our analytical results show that adding noise allows for a rich control of the dynamics, stabilizing the lossy state and making state purification possible to a greater variety of steady states.}, archive = {J_PRL}, author = {Pablo Martinez-Azcona and Aritra Kundu and Avadh Saxena and Adolfo del Campo and Aurélia Chenu}, doi = {10.1103/5ksl-tjjm}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010402}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum dynamics with stochastic non-hermitian hamiltonians}, volume = {135}, year = {2025}, }
• (2025). Magic monotone for faithful detection of nonstabilizerness in mixed states. PRL, 135(1), 010203. (www)

  @article{ , abstract = {We introduce a monotone to quantify the amount of nonstabilizerness in mixed quantum states. The monotone gives a necessary and sufficient criterion for detecting the presence of nonstabilizerness for both pure and mixed states. The monotone is based on determining the boundaries of the stabilizer polytope in the space of Pauli string expectation values. The boundaries can be described by a set of hyperplane inequations, where violation of any one of these gives a necessary and sufficient condition for nonstabilizerness. The monotone is constructed by finding the hyperplane with the maximum violation and is a type of Minkowski functional. We also introduce a faithful witness based on similar methods. The approach is more computationally efficient than existing faithful mixed state monotones such as robustness of magic due to the smaller number and discrete nature of the parameters to be optimized.}, archive = {J_PRL}, author = {Krzysztof Warmuz and Ernest Dokudowiec and Chandrashekar Radhakrishnan and Tim Byrnes}, doi = {10.1103/2s3j-t22p}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010203}, shortjournal = {Phys. Rev. Lett.}, title = {Magic monotone for faithful detection of nonstabilizerness in mixed states}, volume = {135}, year = {2025}, }
• (2025). Second law of entanglement manipulation with an entanglement battery. PRL, 135(1), 010202. (www)

  @article{ , abstract = {A central question since the beginning of quantum information science is how two distant parties can convert one entangled state into another. It has been conjectured that such conversions could be executed reversibly in an asymptotic regime, mirroring the reversible nature of Carnot cycles in classical thermodynamics. While a conclusive proof of this conjecture has been missing so far, earlier studies have excluded reversible entanglement manipulation in various settings. In this Letter, we show that arbitrary mixed state entanglement transformations can be made reversible under local operations and classical communication, when assisted by an entanglement battery—an auxiliary quantum system that stores and supplies entanglement in a way that ensures no net entanglement is lost. In particular, the rate of transformation in the asymptotic limit can be quantitatively expressed as a ratio of entanglement present within the quantum states involved. Our setting allows us to consider different entanglement quantifiers which give rise to unique principles governing state transformations, effectively constituting diverse manifestations of a “second law” of entanglement manipulation. These findings resolve a long-standing open question on the reversible manipulation of entangled states and are also applicable to multipartite entanglement and other quantum resource theories, including quantum thermodynamics.}, archive = {J_PRL}, author = {Ray Ganardi and Tulja Varun Kondra and Nelly H. Y. Ng and Alexander Streltsov}, doi = {10.1103/kl56-p2vb}, journal = {Physical Review Letters}, month = {7}, number = {1}, pages = {010202}, shortjournal = {Phys. Rev. Lett.}, title = {Second law of entanglement manipulation with an entanglement battery}, volume = {135}, year = {2025}, }
• (2025). Anomalous hard-wall repulsion between polymers in solvent mixtures and its implication for biomolecular condensates. PRL, 135(1), 018201. (www)

  @article{ , abstract = {The system of polymers dissolved in a mixture of different solvents is a widely used coarse-grained model to represent biomolecular condensates in intracellular environments. Here, we apply a variational theory to simultaneously control the center of mass of two polymers and perform the first quantification of their interactions in a mixture of solvent and cosolvent. While the polymer can completely dissolve in both solvents, strong polymer-cosolvent affinity induces the occurrence of polymer-assisted cosolvent condensation. Even though all the molecular interactions are soft, the potential of mean force between two polymer-cosolvent condensates exhibits an anomalous feature of hard-wall repulsion upon contact, which cannot be categorized into any existing types of interchain interactions. This repulsion is enhanced as either the affinity or the bulk cosolvent fraction increases. The underlying mechanism is cosolvent regulation manifested as a discontinuous local condensation of cosolvent as two condensates approach. The hard-wall repulsion provides a kinetic barrier to prevent coalescence of condensates and hence highlights the intrinsic role of proteins as a cosolvent in stabilizing biomolecular condensates.}, archive = {J_PRL}, author = {Luofu Liu and Rui Wang}, doi = {10.1103/7sz2-2n6t}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {018201}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous hard-wall repulsion between polymers in solvent mixtures and its implication for biomolecular condensates}, volume = {135}, year = {2025}, }
• (2025). Entropic origin of polymer nucleation at amorphous solid interfaces. PRL, 135(1), 018101. (www)

  @article{ , abstract = {Interfaces play a pivotal role in various physical, chemical, and biological processes. In polymer crystallization, nucleation often occurs at solid interfaces due to the reduced barrier for heterogeneous nucleation, with the chain conformations and dynamics deviating significantly from their undisturbed (bulk) state. In this Letter, we employed a nanopore-confined system to differentiate between two nucleation scenarios: surface nucleation and homogeneous nucleation, through comprehensive crystal orientation analysis. Experimental findings reveal that surface-induced nucleation in polymers is predominantly driven by an entropic effect, arising from the loss of conformational entropy as polymer chains flatten at weakly interacting solid interfaces. Homogeneous nucleation is, instead, predominant in cases of strong interfacial interactions.}, archive = {J_PRL}, author = {Ming Wang and Zijian Song and Guoming Liu and Dujin Wang}, doi = {10.1103/l2c8-m7k7}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {018101}, shortjournal = {Phys. Rev. Lett.}, title = {Entropic origin of polymer nucleation at amorphous solid interfaces}, volume = {135}, year = {2025}, }
• (2025). Observation of strong nonreciprocal thermal emission. PRL, 135(1), 016901. (www)

  @article{ , abstract = {The Kirchhoff’s law of thermal radiation stating the equivalence of emissivity and absorptivity at the same wavelength, angle, and polarization, has completely constrained emission and absorption processes. Achieving strong nonreciprocal emission points to fundamental advances for applications such as energy harvesting, heat transfer, and sensing, but strong nonreciprocal thermal emission has not been experimentally realized. Here, we observe strong nonreciprocal thermal emission using a custom-designed angle-resolved magnetic thermal emission spectroscopy and an epitaxially transferred gradient-doped metamaterial. We show that under magnetic field, the metamaterial strongly breaks Kirchhoff’s law, with a difference between emissivity and absorptivity at the same wavelength and angle reaching as high as 0.43. Significant nonreciprocal emission persists over broad spectral and angular ranges. The demonstration of strong nonreciprocal thermal emission and the approach can be useful for systematic exploration of nonreciprocal thermal photonics for thermal management, infrared camouflage, and energy conversion.}, archive = {J_PRL}, author = {Zhenong Zhang and Alireza Kalantari Dehaghi and Pramit Ghosh and Linxiao Zhu}, doi = {10.1103/PhysRevLett.135.016901}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {016901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of strong nonreciprocal thermal emission}, volume = {135}, year = {2025}, }
• (2025). Monolayer control of spin-charge conversion in van der waals heterostructures. PRL, 135(1), 016702. (www)

  @article{ , abstract = {The diversity of 2D materials and their van der Waals (vdW) stacking presents fertile ground for engineering novel multifunctional materials and quantum states of matter. This permits unique opportunities to tailor the electronic properties of vdW heterostructures by the insertion of only a single 2D material layer. However, such vdW materials engineering at the atomic scale has yet to be investigated for spin-charge interconversion phenomena. Here, we report on the control of these effects at the monolayer level, where a drastic increase in intensity and change in sign of THz spintronic emission are demonstrated by inserting a single layer of MoSe 2 between PtSe 2 and graphene in a fully epitaxial, large area stacked structure. By using a combination of spin and angle resolved photoemission and density functional theory to reveal the electronic and spin structures, we illustrate two different mechanisms relying on charge transfer and electronic hybridization for the formation of Rashba states, which are responsible for spin-charge conversion and hence the THz spintronic emission. These findings open new pathways to design, at the atomic scale, efficient THz spintronic emitters made of 2D materials and other spintronic devices based on spin-charge interconversion phenomena.}, archive = {J_PRL}, author = {Khasan Abdukayumov and Oliver Paull and Martin Mičica and Fatima Ibrahim and Libor Vojáček and Adrien Wright and Sylvain Massabeau and Federico Mazzola and Vincent Polewczyk and Cyriack Jego and Rahul Sharma and Céline Vergnaud and Alain Marty and Isabelle Gomes de Moraes and Abdelkarim Ouerghi and Hanako Okuno and Anupam Jana and Indrani Kar and Jun Fujii and Ivana Vobornik and Leticia Melo Costa and Olivier Renault and Jing Li and Frédéric Bonell and Mairbek Chshiev and Manuel Bibes and Jean-Marie George and Henri Jaffrès and Sukhdeep Dhillon and Matthieu Jamet}, doi = {10.1103/l41n-qxpd}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {016702}, shortjournal = {Phys. Rev. Lett.}, title = {Monolayer control of spin-charge conversion in van der waals heterostructures}, volume = {135}, year = {2025}, }
• (2025). Electrical switching of altermagnetism. PRL, 135(1), 016701. (www)

  @article{ , abstract = {Switching magnetism using only electricity is of great significance for industrial applications but remains challenging. We find that altermagnetism, as a newly discovered unconventional magnetism, may open an avenue along this effort. Specifically, to have deterministic switching, i.e., reversing current direction must reverse magnetic structure, parity symmetry has to be broken. We discover that, due to their symmetry, which depends on chemical environments, altermagnet devices may naturally carry the parity symmetry breaking required for deterministic electrical switching of magnetism. More importantly, we identify MnTe bilayers (Te-Mn-Te-Mn-Te) as candidate devices, with the help of symmetry analysis, first-principles calculations, and magnetic dynamics simulations. This scheme will inspire further explorations on unconventional magnetism.}, archive = {J_PRL}, author = {Yiyuan Chen and Xiaoxiong Liu and Hai-Zhou Lu and X. C. Xie}, doi = {10.1103/zm5y-vy41}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {016701}, shortjournal = {Phys. Rev. Lett.}, title = {Electrical switching of altermagnetism}, volume = {135}, year = {2025}, }
• (2025). Topological nature of edge states for one-dimensional systems without symmetry protection. PRL, 135(1), 016601. (www)

  @article{ , abstract = {We numerically verify and analytically prove a winding number invariant that correctly predicts the number of edge states in one-dimensional, nearest-neighbor (between unit cells), two-band models with any complex couplings and open boundaries. Our winding number uses analytical continuation of the wave-vector into the complex plane and involves two special points on the full Riemann surface band structure that correspond to bulk eigenvector degeneracies. Our winding number is invariant under unitary or similarity transforms. We emphasize that the topological criteria we propose here differ from what is traditionally defined as a topological or trivial phase in symmetry-protected classification studies. It is a broader invariant for our model that supports non-zero energy edge states and its transition does not coincide with the gap closing condition. When the relevant symmetries are applied, our invariant reduces to well-known Hermitian and non-Hermitian symmetry-protected topological invariants.}, archive = {J_PRL}, author = {Janet Zhong and Heming Wang and Alexander N. Poddubny and Shanhui Fan}, doi = {10.1103/k77w-ft26}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {016601}, shortjournal = {Phys. Rev. Lett.}, title = {Topological nature of edge states for one-dimensional systems without symmetry protection}, volume = {135}, year = {2025}, }
• (2025). Spatial string tension and its effects on screening correlators in a thermal QCD plasma. PRL, 135(1), 012301. (www)

  @article{ , abstract = {We calculate the spatial Wilson line correlator for flavor QCD using highly improved staggered quark discretization for fermions and in quenched QCD for a wide range of temperatures, from the chiral crossover temperature or the deconfinement temperature , respectively, up to 2 GeV. Extracting the spatial string tension for different lattice cutoffs and by performing a continuum extrapolation of this observable, we show that the soft (magnetic) gluons interact nonperturbatively even at temperatures . We provide incriminating evidences to demonstrate that dimensionally reduced effective theories can describe these soft quark and gluon quasi-particles for both quenched and flavor QCD, at temperatures . We also show for the first time the imprints of the nonperturbative pseudopotential in the properties of mesonic screening masses for temperatures ranging from 0.8 to 164 GeV in the quark-gluon plasma.}, archive = {J_PRL}, author = {Dibyendu Bala and Olaf Kaczmarek and Peter Petreczky and Sayantan Sharma and Swagatam Tah}, doi = {10.1103/3tmf-s94w}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {012301}, shortjournal = {Phys. Rev. Lett.}, title = {Spatial string tension and its effects on screening correlators in a thermal QCD plasma}, volume = {135}, year = {2025}, }
• (2025). Robust singularity theorem. PRL, 135(1), 011501. (www)

  @article{ , abstract = {We prove the Penrose-Wall singularity theorem in the full semiclassical gravity regime, significantly expanding its range of validity. To accomplish this, we modify the definition of quantum-trapped surfaces without affecting their genericity. Our theorem excludes controlled “bounces” in the interior of a black hole and in a large class of cosmologies.}, archive = {J_PRL}, author = {Raphael Bousso}, doi = {10.1103/6f9b-3jmx}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {011501}, shortjournal = {Phys. Rev. Lett.}, title = {Robust singularity theorem}, volume = {135}, year = {2025}, }
• (2025). Overcoming quantum metrology singularity through sequential measurements. PRL, 135(1), 010401. (www)

  @article{ , abstract = {The simultaneous estimation of multiple unknown parameters is the most general scenario in quantum sensing. Quantum multiparameter estimation theory provides fundamental bounds on the achievable precision of simultaneous estimation. However, these bounds can become singular (no finite bound exists) in multiparameter sensing due to parameter interdependencies, limited probe accessibility, and insufficient measurement outcomes. Here, we address the singularity issue in quantum sensing through a simple mechanism based on a sequential measurement strategy. This sensing scheme overcomes the singularity constraint and enables the simultaneous estimation of multiple parameters with a local and fixed measurement throughout the sensing protocol. This is because sequential measurements, involving consecutive steps of local measurements followed by probe evolution, inherently produce correlated measurement data that grows exponentially with the number of sequential measurements. Finally, through two different examples, namely a strongly correlated probe and a light-matter system, we demonstrate how such singularities are reflected when inferring the unknown parameters through Bayesian estimation.}, archive = {J_PRL}, author = {Yaoling Yang and Victor Montenegro and Abolfazl Bayat}, doi = {10.1103/gsyv-jllq}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {010401}, shortjournal = {Phys. Rev. Lett.}, title = {Overcoming quantum metrology singularity through sequential measurements}, volume = {135}, year = {2025}, }
• (2025). Sum of entanglement and subsystem coherence is invariant under quantum reference frame transformations. PRL, 135(1), 010201. (www)

  @article{ , abstract = {Recent work on quantum reference frames (QRFs) has demonstrated that superposition and entanglement are properties that change under QRF transformations. Given their utility in quantum information processing, it is important to understand how a mere change of perspective can produce or reduce these resources. Here we prove the existence of a QRF invariant which can be decomposed such that it captures the trade-off between entanglement and subsystem coherence: we demonstrate the invariance of the sum of entanglement and subsystem coherence for two pairs of resource quantifiers. Moreover, we find a weaker trade-off that holds for any possible pair of measures. Finally, we discuss the implications of this interplay for violations of Bell’s inequalities, clarifying that for any choice of QRF, there is a quantum resource responsible for the violation. These findings contribute to a better understanding of the quantum information theoretic aspects of QRFs, offering a foundation for future exploration in both quantum theory and quantum gravity.}, archive = {J_PRL}, author = {Carlo Cepollaro and Ali Akil and Paweł Cieśliński and Anne-Catherine de la Hamette and Časlav Brukner}, doi = {10.1103/h6b3-y4vt}, journal = {Physical Review Letters}, month = {6}, number = {1}, pages = {010201}, shortjournal = {Phys. Rev. Lett.}, title = {Sum of entanglement and subsystem coherence is invariant under quantum reference frame transformations}, volume = {135}, year = {2025}, }
• (2025). Surveying the space of descriptions of a composite system with machine learning. PRL, 134(25), 257401. (www)

  @article{ , abstract = {Multivariate information theory provides a general and principled framework for understanding how the components of a system are connected. Existing analyses are coarse in nature—built up from characterizations of discrete subsystems—and can be computationally prohibitive. In this work, we propose to study the continuous space of possible descriptions of a composite system as a window into its organizational structure. A description consists of specific information conveyed about each of the components, and the space of possible descriptions is equivalent to the space of lossy compression schemes of the components. We introduce a machine-learning framework to optimize descriptions that extremize key information theoretic quantities used to characterize organization, such as total correlation and O-information. Through case studies on spin systems, sudoku boards, and letter sequences from natural language, we identify extremal descriptions that reveal how system-wide variation emerges from individual components. By integrating machine learning into a fine-grained information theoretic analysis of composite random variables, our framework opens a new avenues for probing the structure of real-world complex systems.}, archive = {J_PRL}, author = {Kieran A. Murphy and Yujing Zhang and Dani S. Bassett}, doi = {10.1103/gxrh-2xsv}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {257401}, shortjournal = {Phys. Rev. Lett.}, title = {Surveying the space of descriptions of a composite system with machine learning}, volume = {134}, year = {2025}, }
• (2025). Spring-block theory of feature learning in deep neural networks. PRL, 134(25), 257301. (www)

  @article{ , abstract = {Feature-learning deep nets progressively collapse data to a regular low-dimensional geometry. How this emerges from the collective action of nonlinearity, noise, learning rate, and other factors, has eluded first-principles theories built from microscopic neuronal dynamics. We exhibit a noise–nonlinearity phase diagram that identifies regimes where shallow or deep layers learn more effectively and propose a macroscopic mechanical theory that reproduces the diagram and links feature learning across layers to generalization.}, archive = {J_PRL}, author = {Cheng Shi and Liming Pan and Ivan Dokmanić}, doi = {10.1103/ys4n-2tj3}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {257301}, shortjournal = {Phys. Rev. Lett.}, title = {Spring-block theory of feature learning in deep neural networks}, volume = {134}, year = {2025}, }
• (2025). Master stability for traveling waves on networks. PRL, 134(25), 257201. (www)

  @article{ , abstract = {We present a framework for determining effectively the spectrum and stability of traveling waves on networks with symmetries, such as rings and lattices, by computing master stability curves (MSCs). Unlike traditional methods, MSCs are independent of system size and can be readily used to assess wave destabilization and multistability in small and large networks.}, archive = {J_PRL}, author = {Stefan Ruschel and Andrus Giraldo}, doi = {10.1103/6v64-j5fd}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {257201}, shortjournal = {Phys. Rev. Lett.}, title = {Master stability for traveling waves on networks}, volume = {134}, year = {2025}, }
• (2025). Broadband ptychotomography with a hyperspectral detector. PRL, 134(25), 257001. (www)

  @article{ , abstract = {X-ray ptychography is a robust microscopy technique with nanoscale resolution that requires a spatially and temporally coherent illumination. In a typical setup, the temporal coherence requirements are satisfied by monochromating the x-ray source, e.g., using a crystal monochromator. Recent studies have shown that energy resolving, or hyperspectral, detectors can to some extent replace the role of the monochromator to perform, e.g., edge-subtraction ptychographic imaging with broadband radiation in a single acquisition. Scaling this capability from two dimensions (2D) to three dimensions (3D), and from a single absorption edge to multiple edges, is critical for its applications in structural and elemental characterisation. The method is hitherto limited by the inherently lower maximum count rate of hyperspectral detectors and the chromaticity of the optics often used in x-ray ptychography experiments, namely Fresnel zone plates. In this work, we design an optimized broadband spectroscopic ptychography setup and use it to perform 3D hyperspectral imaging of particles of battery material containing various percentages of nickel, manganese, cobalt (NMC). We show that we can identify different compositions based on their spectral response. We discuss the results and provide guidelines for future exploitation of the method in laboratory settings.}, archive = {J_PRL}, author = {Wiebe Stolp and Frederic van Assche and Ruizhi Tang and Karel Desplenter and Caori Organista Castelblanco and Ralf Ziesche and Silvia Cipiccia and Darren Batey and Matthieu N. Boone}, doi = {10.1103/kbrf-gb9c}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {257001}, shortjournal = {Phys. Rev. Lett.}, title = {Broadband ptychotomography with a hyperspectral detector}, volume = {134}, year = {2025}, }
• (2025). Atomiclike selection rules in free electron scattering. PRL, 134(25), 256902. (www)

  @article{ , abstract = {Phase-shaped electron energy-loss spectroscopy (PSEELS) measures the scattering probability of structured free electron beams by a target. Over the last decade, it was shown that this scheme can be employed to emulate polarized optical spectroscopies with electrons, and therefore to transpose macroscopic optical concepts—such as dichroism—down to the deep subwavelength scale. In this Letter, we theoretically demonstrate that PSEELS can, in fact, go way further than mimicking optics and enables to map a plethora of so far inaccessible nano-optical quantities such as the electric quadrupolar momentum.}, archive = {J_PRL}, author = {Simon Garrigou and Hugo Lourenço-Martins}, doi = {10.1103/l2y2-99jx}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256902}, shortjournal = {Phys. Rev. Lett.}, title = {Atomiclike selection rules in free electron scattering}, volume = {134}, year = {2025}, }
• (2025). Spin noise of a halide perovskite. PRL, 134(25), 256901. (www)

  @article{ , abstract = {We report on the first observation of spin noise in a strongly birefringent semiconductor—halide perovskite single crystal . The observed spin noise resonance is attributed to resident free holes in the bulk of the crystal with one of the longest spin dephasing times . The spin dynamics is found to be affected by the residual light absorption of the crystal providing renormalization of the Larmor frequency. Extended spin noise spectroscopy with a rotating magnetic field allowed us not only to evaluate the -factor anisotropy but also to distinguish two different spin subsystems tentatively associated with twinning of the crystal. This work opens the way to studies of spin physics of bulk anisotropic semiconductors in general and perovskites in particular.}, archive = {J_PRL}, author = {V. O. Kozlov and N. I. Selivanov and C. C. Stoumpos and G. G. Kozlov and V. S. Zapasskii and Yu. V. Kapitonov and D. S. Smirnov and I. I. Ryzhov}, doi = {10.1103/6p4z-shzt}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256901}, shortjournal = {Phys. Rev. Lett.}, title = {Spin noise of a halide perovskite}, volume = {134}, year = {2025}, }
• (2025). Deterministic generation of a single-byte electric skyrmion bubble. PRL, 134(25), 256802. (www)

  @article{ , abstract = {Polar skyrmion bubbles are spherical electric solitons offering multiple new functionalities for the next generation of electronic devices. In this study, we explore the formation of these particlelike entities at room temperature within a ferroelectric nanostructure composed of a nanodot embedded in a thin film. Our findings emphasize the unique capability of this specific geometry to host various types of electric solitons, particularly to allow for a low-power encoding of a single-byte skyrmion bubble at the precise location of the nanodot through a sequence of bias voltage signals. This intricate process is found to be driven by the emergence of a negative nonlocal dielectric response in nanoscale ultrathin film. Our findings offer practical insights into the controlled encoding operations of polar defects at targeted locations, thereby paving the way for the practical implementation of emerging topological ferroelectrics in memory and logic devices.}, archive = {J_PRL}, author = {Peng Chen and Yousra Nahas and Sergei Prokhorenko and Laurent Bellaiche}, doi = {10.1103/p46j-yc89}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256802}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic generation of a single-byte electric skyrmion bubble}, volume = {134}, year = {2025}, }
• (2025). Inverse melting of polar order in chemically substituted BaTiO3. PRL, 134(25), 256801. (www)

  @article{ , abstract = {In many condensed matter systems, long-range order emerges at low temperatures as thermal fluctuations subside. In the presence of competing interactions or quenched disorder, however, some systems can show unusual configurations that become more disordered at low temperature, a rare phenomenon known as “inverse melting.” Here, we discover an inverse melting of the polar order in a ferroelectric oxide with quenched chemical disorder ( ) through direct atomic-scale visualization using in situ scanning transmission electron microscopy. In contrast to the clean parent system in which long-range order tracks lower temperatures, we observe in the doped system that thermally driven fluctuations at high temperature give way to a more ordered state and then to a reentrant disordered configuration at even lower temperature. Such an inverse melting of the polar order is likely linked to the random field generated by Zr dopants, which modulates the energy landscape arising from the competition between thermal fluctuations and random field pinning potential. These visualizations highlight a rich landscape of order and disorder in materials with quenched disorder, which may be key to understanding their advanced functionalities.}, archive = {J_PRL}, author = {Yang Zhang and Suk Hyun Sung and Colin B. Clement and Sang-Wook Cheong and Ismail El Baggari}, doi = {10.1103/62lm-hhw5}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256801}, shortjournal = {Phys. Rev. Lett.}, title = {Inverse melting of polar order in chemically substituted BaTiO3}, volume = {134}, year = {2025}, }
• (2025). Magnetoelastic dynamics of the spin jahn-teller transition in CoTi2O5. PRL, 134(25), 256702. (www)

  @article{ , abstract = {CoTi 2 O 5 has the paradox that low temperature static magnetic order is incompatible with the crystal structure owing to a mirror plane that exactly frustrates magnetic interactions. Despite no observable structural distortion with diffraction, CoTi 2 O 5 does magnetically order below T N ∼ 25 K with the breaking of spin ground state degeneracy proposed to be a realization of the spin Jahn-Teller effect in analogy to the celebrated orbital Jahn-Teller transition. We apply neutron and Raman spectroscopy to study the dynamics of this transition in CoTi 2 O 5 . We find anomalous acoustics associated with a symmetry breaking strain that characterizes the spin Jahn-Teller transition. Crucially, the energy of this phonon coincides with the energy scale of the magnetic excitations, and has the same symmetry of an optic mode, observed with Raman spectroscopy, which atypically softens in energy with decreasing temperature. Taken together, we propose that the energetics of the spin Jahn-Teller effect in CoTi 2 O 5 are related to cooperative magnetoelastic fluctuations as opposed to conventional soft critical dynamics which typically drive large measurable static displacements.}, archive = {J_PRL}, author = {K. Guratinder and R. D. Johnson and D. Prabhakaran and R. A. Taylor and F. Lang and S. J. Blundell and L. S. Taran and S. V. Streltsov and T. J. Williams and S. R. Giblin and T. Fennell and K. Schmalzl and C. Stock}, doi = {10.1103/sr9s-ll1y}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256702}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetoelastic dynamics of the spin jahn-teller transition in CoTi2O5}, volume = {134}, year = {2025}, }
• (2025). Dynamic scaling theory for a field quench near the kasteleyn transition in spin ice. PRL, 134(25), 256701. (www)

  @article{ , abstract = {We present a dynamic scaling theory to describe relaxation dynamics following a magnetic-field quench near an unconventional phase transition in the magnetic material spin ice. Starting from a microscopic model, we derive an effective description for the critical dynamics in terms of the seeding and growth of string excitations, and use this to find scaling forms in terms of time, reduced temperature, and monopole fugacity. We confirm the predictions of scaling theory using Monte Carlo simulations, which also show good quantitative agreement with analytical expressions valid in the limit of low monopole density. As well as being relevant for experiments in the spin ice materials, our results open the way for the study of dynamic critical properties in a family of unconventional classical phase transitions.}, archive = {J_PRL}, author = {Stephen Powell and Sukla Pal}, doi = {10.1103/b9gd-y4y6}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256701}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamic scaling theory for a field quench near the kasteleyn transition in spin ice}, volume = {134}, year = {2025}, }
• (2025). Chiral gapless spin liquid in hyperbolic space. PRL, 134(25), 256604. (www)

  @article{ , abstract = {We analyze the Kitaev model on the hyperbolic lattice. The is formed by a regular tricoordinated tiling of nonagons, where the three-color coding of bonds according to the inequivalent Kitaev Ising spin couplings yields the natural generalization of the original Kitaev model for Euclidean regular honeycomb tiling. Upon investigation of the bulk spectrum for large finite size droplets, we identify a gapless chiral spin liquid state featuring spontaneous time-reversal symmetry breaking. Because of its noncommutative translation group structure, such type of hyperbolic spin liquid is conjectured to feature chiral quasiparticles with a potentially non-Abelian Bloch profile.}, archive = {J_PRL}, author = {Felix Dusel and Tobias Hofmann and Atanu Maity and Rémy Mosseri and Julien Vidal and Yasir Iqbal and Martin Greiter and Ronny Thomale}, doi = {10.1103/PhysRevLett.134.256604}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256604}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral gapless spin liquid in hyperbolic space}, volume = {134}, year = {2025}, }
• (2025). Observation of extrinsic topological phases in floquet photonic lattices. PRL, 134(25), 256603. (www)

  @article{ , abstract = {Discrete-step walks describe the dynamics of particles in a lattice subject to hopping or splitting events at discrete times. Despite being of primordial interest to the physics of quantum walks, the topological properties arising from their discrete-step nature have been hardly explored. Here we report the observation of topological phases unique to discrete-step walks. We use light pulses in a double-fiber ring setup whose dynamics maps into a two-dimensional lattice subject to discrete splitting events. We show that the number of edge states is not simply described by the bulk invariants of the lattice (i.e., the Chern number and the Floquet winding number) as would be the case in static lattices and in lattices subject to smooth modulations. The number of edge states is also determined by a topological invariant associated to the discrete-step unitary operators acting at the edges of the lattice. This situation goes beyond the usual bulk-edge correspondence and allows manipulating the number of edge states without the need to go through a gap closing transition. Our Letter opens new perspectives for the engineering of topological modes for particles subject to quantum walks.}, archive = {J_PRL}, author = {Rajesh Asapanna and Rabih El Sokhen and Albert F. Adiyatullin and Clément Hainaut and Pierre Delplace and Álvaro Gómez-León and Alberto Amo}, doi = {10.1103/tqyx-qyj4}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256603}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of extrinsic topological phases in floquet photonic lattices}, volume = {134}, year = {2025}, }
• (2025). Sliding ferroelectrics induced hybrid-order topological phase transitions. PRL, 134(25), 256602. (www)

  @article{ , abstract = {We propose ferroelectric layer sliding as a new approach to realize and manipulate topological quantum states in two-dimensional (2D) bilayer magnetic van der Waals materials. We show that stacking monolayer ferromagnetic topological states into layer-spin-locked bilayer antiferromagnetic structures, and introducing sliding ferroelectricity leads to asynchronous topological evolution of different layers (spins) owing to the existence of polarization potentials, thereby giving rise to rich layer-resolved topological phases. As a specific example, by means of a lattice model, we show that a bilayer magnetic 2D second order topological insulator (SOTI) reveals an unrecognized spin-hybrid-order topological insulator after undergoing ferroelectric sliding. Interestingly, in such a phase, the spin-up (top layer) and spin-down (bottom layer) channels exhibit first-order and second-order topological properties, respectively. Moreover, other topological phases such as the SOTI, quantum spin Hall insulator, quantum anomalous Hall insulator, and trivial insulator, can also emerge through changes in the parameters of the system; and the relevant topological indices are also discussed. In terms of materials, based on first principles calculations, we predict the material can serve as an ideal platform to realize our proposal. Further, we predict that the anomalous Nernst effect of these several topological phases exhibits distinct differences, and therefore can be used as a signal for experimental probing.}, archive = {J_PRL}, author = {Ning-Jing Yang and Jian-Min Zhang and Xiao-Ping Li and Zeying Zhang and Zhi-Ming Yu and Zhigao Huang and Yugui Yao}, doi = {10.1103/l1n5-1jsm}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256602}, shortjournal = {Phys. Rev. Lett.}, title = {Sliding ferroelectrics induced hybrid-order topological phase transitions}, volume = {134}, year = {2025}, }
• (2025). Topological solitons in square-root graphene nanoribbons controlled by electric fields. PRL, 134(25), 256601. (www)

  @article{ , abstract = {Conjugational defects, also known as solitons, play an important role in the electronic, magnetic, and optical properties of materials. Understanding solitons can uncover intriguing physics and provide insights for designing quantum materials with tailored band structures and electronic properties. Here, we propose a framework to create and control solitons via topological phase transitions in a class of graphene nanoribbons (GNRs) called square-root GNRs, using a transverse electric field. To demonstrate the experimental feasibility, we design and synthesize a representative GNR with a bottom-up approach, with first-principles calculations revealing topological soliton states at the domain wall induced by the electric field. The framework introduced in this Letter can potentially enable direct manipulation of solitons and provide a platform to study them systematically.}, archive = {J_PRL}, author = {Haiyue Huang and Mamun Sarker and Percy Zahl and C. Stephen Hellberg and Jeremy Levy and Ioannis Petrides and Alexander Sinitskii and Prineha Narang}, doi = {10.1103/hjt2-3s9h}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256601}, shortjournal = {Phys. Rev. Lett.}, title = {Topological solitons in square-root graphene nanoribbons controlled by electric fields}, volume = {134}, year = {2025}, }
• (2025). Multiple mechanisms for emerging conductance plateaus in fractional quantum hall states. PRL, 134(25), 256503. (www)

  @article{ , abstract = {Two-terminal conductance quantization in the context of quantum Hall (QH) physics is intimately related to the current carried by a discrete number of chiral edge modes. Upon pinching off a QH bar, one may engineer setups where some modes are fully transmitted (while the others are fully reflected), giving rise to the orthodox theory of quantized conductance plateaus. Here, we note that the observation of quantized plateaus does not uniquely indicate the underlying mechanism. Our Letter demonstrates explicitly that (i) such plateaus may be the manifestations of entirely different mechanisms; (ii) conductance measurements alone will not suffice to distinguish one from the other. We further show that measurements of shot noise (auto- and cross-correlation) at the plateau may discriminate among different mechanisms. While our observations apply to a broad class of QH states, we demonstrate their applicability employing a prototypical example: the bulk state of filling factor ν = 2 / 3 . We present distinctly different scenarios that lead to a conductance plateau G 2 -terminal = e 2 / 3 h (observed previously) and likewise qualitatively different mechanisms leading to e 2 / 2 h (recently observed). We also predict the possibility of a new conductance plateau at 5 e 2 / 9 h , following a nonorthodox scenario.}, archive = {J_PRL}, author = {Sourav Manna and Ankur Das and Yuval Gefen and Moshe Goldstein}, doi = {10.1103/p4y5-trph}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256503}, shortjournal = {Phys. Rev. Lett.}, title = {Multiple mechanisms for emerging conductance plateaus in fractional quantum hall states}, volume = {134}, year = {2025}, }
• (2025). Accurate simulation of the hubbard model with finite fermionic projected entangled pair states. PRL, 134(25), 256502. (www)

  @article{ , abstract = {We demonstrate the use of finite-size fermionic projected entangled pair states, in conjunction with variational Monte Carlo, to perform accurate simulations of the ground state of the 2D Hubbard model. Using bond dimensions of up to , we show that we can surpass state-of-the-art density matrix renormalization group energies that use up to SU(2) multiplets on eight-leg ladders. We further apply our methodology to , and lattices at hole doping and observe the dimensional crossover between stripe orientations. Our Letter shows the power of finite-size fermionic tensor networks to resolve the physics of the 2D Hubbard model and related problems.}, archive = {J_PRL}, author = {Wen-Yuan Liu and Huanchen Zhai and Ruojing Peng and Zheng-Cheng Gu and Garnet Kin-Lic Chan}, doi = {10.1103/r4q9-4yvj}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256502}, shortjournal = {Phys. Rev. Lett.}, title = {Accurate simulation of the hubbard model with finite fermionic projected entangled pair states}, volume = {134}, year = {2025}, }
• (2025). Intrinsic thermal hall effect in mott insulators. PRL, 134(25), 256501. (www)

  @article{ , abstract = {In light of recent experimental data indicating a substantial thermal Hall effect in square lattice antiferromagnetic Mott insulators, we investigate whether a simple Mott insulator can sustain a finite thermal Hall effect. We verify that the answer is “no” if one performs calculations within a spin-only low-energy effective spin model with noninteracting magnons. However, by performing determinant quantum Monte Carlo simulations, we show the single-band Hubbard model coupled to an orbital magnetic field does support a finite thermal Hall effect when and in the Mott insulating phase. We argue that the (carrier agnostic) necessary conditions for observing a finite thermal Hall effect are time-reversal and particle-hole symmetry breaking. By considering magnon-magnon scattering using a semiclassical Boltzmann analysis, we illustrate a physical mechanism by which finite transverse thermal conductivity may arise, consistent with our symmetry argument and numerical results. Our results indicate that square and triangular lattices with SU(2) symmetry can support a finite thermal Hall effect and call for a critical reexamination of thermal Hall effect data in insulating magnets, as the magnon contribution should not be excluded a priori .}, archive = {J_PRL}, author = {Jixun K. Ding and Emily Z. Zhang and Wen O. Wang and Tessa Cookmeyer and Brian Moritz and Yong Baek Kim and Thomas P. Devereaux}, doi = {10.1103/2729-nmyh}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256501}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic thermal hall effect in mott insulators}, volume = {134}, year = {2025}, }
• (2025). Highly tunable valley polarization of potential-trapped moiré excitons in WSe2/WS2 heterojunctions. PRL, 134(25), 256402. (www)

  @article{ , abstract = {Moiré superlattices created by stacking atomic layers of transition metal dichalcogenide semiconductors have emerged as a class of fascinating artificial photonic and electronic materials. An appealing attribute of these structures is the inheritance of the valley degree of freedom from the constituent monolayers. Recent studies show evidence that the valley polarization of the moiré excitons is highly tunable. In heterojunctions of , marked improvement in valley polarization is observed by increasing optical excitation power, a behavior that is quite distinct from the monolayers, and lacks a clear understanding so far. In this Letter, we show that this highly tunable valley property arises from filling of the moiré superlattice, which provides an intriguing mechanism for engineering these quantum opto-valleytronic platforms. Our data further demonstrate that the long-range electron-hole exchange interaction, despite being significantly weakened in the junctions, is the dominant source of moiré exciton intervalley scattering at low population. Using magnetic field tuning, we quantitatively determine the exchange interaction strength to be 0.03 and 0.24 meV for 0° and 60° twisted samples, respectively, in our experiments, about 1 order of magnitude weaker than that in the monolayers.}, archive = {J_PRL}, author = {Yueh-Chun Wu and Matthew DeCapua and ZhongChen Xu and Takashi Taniguchi and Kenji Watanabe and YouGuo Shi and Jun Yan}, doi = {10.1103/PhysRevLett.134.256402}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256402}, shortjournal = {Phys. Rev. Lett.}, title = {Highly tunable valley polarization of potential-trapped moiré excitons in WSe2/WS2 heterojunctions}, volume = {134}, year = {2025}, }
• (2025). Universal exchange-correlation surface asymptotics: Metal slabs versus semi-infinite metal surfaces. PRL, 134(25), 256401. (www)

  @article{ , abstract = {Density-functional theory is well known to rely on approximations to the unknown exchange-correlation ( x c ) energy functional, which can be constructed from the satisfaction of a number of known properties. One of those properties is the asymptotic behavior of exchange and correlation in localized or extended many-electron systems. However, the actual asymptotics of the x c energy and potential in the vacuum region of a metal surface have remained elusive over the years. Here, we report what we consider to be a final word for the asymptotics of the x c energy per particle ϵ x c [ n ] ( z ) and the x c Kohn-Sham potential v x c [ n ] ( z ) in the vacuum side of both an extended semi-infinite metal and a localized metal slab, which are always universal (i.e., electron-density independent), negative, and inversely proportional to the distance from the surface. We find that, contrary to previous conclusions by other authors, while for extended systems the asymptotics are dominated by a type of correlation, for metal slabs they are dominated by exchange, as in the case of systems that are finite in all directions, like atoms, molecules, and metal clusters.}, archive = {J_PRL}, author = {C. M. Horowitz and C. R. Proetto and J. M. Pitarke}, doi = {10.1103/vtg4-bgzk}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal exchange-correlation surface asymptotics: Metal slabs versus semi-infinite metal surfaces}, volume = {134}, year = {2025}, }
• (2025). Relativistic spin-lattice interaction compatible with discrete translation symmetry in solids. PRL, 134(25), 256303. (www)

  @article{ , abstract = {Recent interest in orbital angular momentum has led to a rapid expansion of research on spin-orbit coupling effects in solids, while also highlighting significant technical challenges. The breaking of rotational symmetry renders the orbital angular momentum operator ill defined, causing conceptual and computational issues in describing orbital motion. To address these issues, here we propose an alternative framework. Based on the Bloch representation of the full relativistic interaction, we derive a field that directly couples to electron spins while preserving discrete translational symmetry, thereby eliminating the need for the position operator. Our approach is fully compatible with existing first-principles computational frameworks for both static and time-dependent density functional theory. We demonstrate that this method offers a more effective description of the Edelstein and spin Hall effects compared to conventional orbital angular momentum formalisms.}, archive = {J_PRL}, author = {Bumseop Kim and Noejung Park and Kyoung-Whan Kim}, doi = {10.1103/q46t-hck1}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256303}, shortjournal = {Phys. Rev. Lett.}, title = {Relativistic spin-lattice interaction compatible with discrete translation symmetry in solids}, volume = {134}, year = {2025}, }
• (2025). Electrothermal manipulation of current-induced phase transitions in ferrimagnetic Mn3Si2Te6. PRL, 134(25), 256302. (www)

  @article{ , abstract = {Phase transitions driven by external parameters are fundamental to condensed matter physics, providing critical insights into symmetry breaking and emergent phenomena. Recently, ferrimagnetic Mn 3 Si 2 Te 6 has attracted considerable attention for its magnetic-field-induced insulator-metal transitions and current-driven phase transitions, but the role of applied currents in the magnetic phase remains poorly understood. Here, we employ local magnetization probes and time-resolved transport measurements to investigate the current-induced phase transitions. Magnetic force microscopy with controlled current flow reveals the evolution of ferrimagnetic domains and a first-order-like magnetic phase transition with an abrupt voltage jump. The measurements with rectangular pulsed currents reveal that the time evolution of resistance closely mirrors the resistance-temperature profile, highlighting the role of heat accumulation and a positive-feedback mechanism in the current-induced phase transitions. Furthermore, we demonstrate that the intrinsic current-voltage characteristics adhere to Ohm’s law, displaying linearity across various magnetic fields and temperatures. Our work advocates for a cautious approach in distinguishing between genuine current-induced nonequilibrium quantum states and thermal effects.}, archive = {J_PRL}, author = {Jiaqi Fang and Jiawei Hu and Xintian Chen and Yaotian Liu and Zheng Yin and Zhe Ying and Yunhao Wang and Ziqiang Wang and Zhilin Li and Shiyu Zhu and Yang Xu and Sokrates T. Pantelides and Hong-Jun Gao}, doi = {10.1103/ry2d-bgyy}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256302}, shortjournal = {Phys. Rev. Lett.}, title = {Electrothermal manipulation of current-induced phase transitions in ferrimagnetic Mn3Si2Te6}, volume = {134}, year = {2025}, }
• (2025). Hard and soft phase slips in a fabry-pérot quantum hall interferometer. PRL, 134(25), 256301. (www)

  @article{ , abstract = {Quantum Hall Fabry-Pérot interferometers are sensitive to the properties of bulk quasiparticles enclosed by the interferometer loop, with the interference phase containing information about both the quasiparticle statistics and the Coulomb-mediated bulk-edge coupling. Previous studies have explored the role of the bulk-edge coupling in an equilibrium picture where quasiparticles enter and exit the interferometer rapidly compared to the timescale over which the interferometer phase is measured. Here, we present data from a monolayer graphene quantum Hall interferometer in the integer quantum Hall regime at and . Quantum interference shows phase slips associated with the entrance of quasiparticles to the interferometer bulk. Tracing the dependence of these phase slips on the magnetic field, we show that the equilibration time can become as long as several minutes. We further use our multigated geometry to identify two classes of phase slips. The first is associated with the addition of a quasiparticle to a bulk “puddle” of quasiparticles uniformly coupled to the entire chiral edge state, while the second is associated with the addition of a quasiparticle trapped by a defect site that couples predominantly to the closest portion of the edge.}, archive = {J_PRL}, author = {N. L. Samuelson and L. A. Cohen and W. Wang and S. Blanch and T. Taniguchi and K. Watanabe and M. P. Zaletel and A. F. Young}, doi = {10.1103/kqct-3llf}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256301}, shortjournal = {Phys. Rev. Lett.}, title = {Hard and soft phase slips in a fabry-pérot quantum hall interferometer}, volume = {134}, year = {2025}, }
• (2025). Medium-range order, density fluctuations, and activated relaxation in the equilibrated deep glass regime. PRL, 134(25), 256101. (www)

  @article{ , abstract = {A successful microscopic theory of activated relaxation in metastable supercooled liquids is extended to the equilibrated deep glass regime. Surprisingly, the predicted power-law scaling connections of the dynamic barrier with diverse scalar order parameters (medium-range order correlation length, dimensionless compressibility, shear modulus) remain unchanged up to astronomically long timescales, despite a fundamental crossover of equilibrium thermodynamics and structure near the laboratory kinetic vitrification point. Quantitative tests against experiments on aged to equilibrium glass-forming liquids up to nearly 20 decades in time scale reveal good agreement. This conflicts with the idea of a crossover from super-Arrhenius to literal Arrhenius relaxation around the laboratory glass transition temperature, and supports the robustness of the theoretical idea that ultraslow dynamics is causally related to medium-range structural order. New avenues of experimental and theoretical research in the deep glass regime are suggested.}, archive = {J_PRL}, author = {Baicheng Mei and Kenneth S. Schweizer}, doi = {10.1103/66zz-y23m}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256101}, shortjournal = {Phys. Rev. Lett.}, title = {Medium-range order, density fluctuations, and activated relaxation in the equilibrated deep glass regime}, volume = {134}, year = {2025}, }
• (2025). Distinct electronic origins of superconductivity and nematicity in FeSe. PRL, 134(25), 256002. (www)

  @article{ , abstract = {The complex interplay between superconductivity, nematicity, and magnetism in iron-based superconductors remains a significant challenge in understanding its high-temperature superconductivity. Despite that numerous experiments aim at revealing the underlying mechanisms for superconductivity and nematicity by varying multiple tuning parameters, the inherent entanglement of these parameters complicates the isolation of the fundamental factors that drive the transitions. Here, by introducing a novel hydrothermal treatment to FeSe, we are able to effectively reduce interstitial Fe without altering the crystal structure and magnetic properties. This treatment results in a notable increase in carrier density and mobility, simultaneously enhancing both superconducting and nematic transition temperatures. Combining our experimental results with previous investigations, we reveal distinct pocket-influenced mechanisms: superconducting order is primarily influenced by electron pockets, while nematic order is driven by hole pockets. The results demonstrate the independent mechanisms of superconductivity and nematicity in FeSe, offering new perspectives on high-temperature superconductivity.}, archive = {J_PRL}, author = {Xueying Ma and Keyi Li and Shaoshuai Hou and Helin Mei and Yiwen Dong and Mingshu Tan and Mingtai Xie and Wei Ren and Xingdong Jiang and Zhiwei Li and Anmin Zhang and Qingming Zhang}, doi = {10.1103/zhlp-4gdv}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256002}, shortjournal = {Phys. Rev. Lett.}, title = {Distinct electronic origins of superconductivity and nematicity in FeSe}, volume = {134}, year = {2025}, }
• (2025). Topological landau theory. PRL, 134(25), 256001. (www)

  @article{ , abstract = {We present an extension of Landau’s theory of phase transitions by incorporating the topology of the order parameter. When the order parameter comprises several components arising from multiplicity in the same irreducible representation of symmetry, it can possess a nontrivial topology and acquire a Berry phase under the variation of thermodynamic parameters. To illustrate this idea, we investigate the superconducting phase transition of an electronic system with tetragonal symmetry and an attractive interaction involving two partial waves, both transforming in the trivial representation. By analyzing the time-dependent Ginzburg-Landau equation in the adiabatic limit, we show that the order parameter acquires a Berry phase after a cyclic evolution of parameters. We study two concrete models—one preserving time-reversal symmetry and one breaking it—and demonstrate that the nontrivial topology of the order parameter originates from thermodynamic analogs of gapless Dirac and Weyl points in the phase diagram. Finally, we identify an experimental signature of the topological Berry phase in a Josephson junction.}, archive = {J_PRL}, author = {Canon Sun and Joseph Maciejko}, doi = {10.1103/PhysRevLett.134.256001}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {256001}, shortjournal = {Phys. Rev. Lett.}, title = {Topological landau theory}, volume = {134}, year = {2025}, }
• (2025). Towards the generation of petawatt near-infrared few-cycle light pulses via forward raman amplification in plasma. PRL, 134(25), 255001. (www)

  @article{ , abstract = {Light amplification toward extremely high power in the infrared regime remains a significant challenge due to the lack of suitable gain media. Here we propose a new scheme to amplify a laser pulse with tunable wavelengths toward extremely high power via forward Raman amplification in plasma. Different from previously proposed schemes based upon backward Raman or Brillouin amplification, our scheme involves a pump pulse and a seed pulse copropagating in moderate density plasma, with the phase matching conditions for forward Raman scattering fulfilled. Due to their group velocity difference in plasma, the pump with a shorter wavelength and longer duration will chase the seed and transfer energy to the latter efficiently. Analytical models for both linear and nonlinear stages of amplification as well as particle-in-cell simulation show that, by employing a pump laser, a seed pulse can be amplified times in its intensity and then self-compressed to nearly single-cycle. Our scheme shows the merits of high efficiency, high compactness, and relatively easy implementation with the copropagating configuration, which may provide a unique route toward the petawatt few-cycle infrared laser pulses.}, archive = {J_PRL}, author = {Zhi-Yu Lei and Zheng-Ming Sheng and Su-Ming Weng and Min Chen and Jie Zhang}, doi = {10.1103/cshj-jgz7}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {255001}, shortjournal = {Phys. Rev. Lett.}, title = {Towards the generation of petawatt near-infrared few-cycle light pulses via forward raman amplification in plasma}, volume = {134}, year = {2025}, }
• (2025). Theory of internal conversion of the th229 nuclear isomer in solid-state hosts. PRL, 134(25), 253801. (www)

  @article{ , abstract = {Laser excitation of nuclei in doped wide band gap crystals has been demonstrated recently, opening the possibility of developing ultrastable solid-state clocks and sensitive searches for new physics. We develop a quantitative theory of the internal conversion (IC) of isomeric in solid-state hosts and elucidate a crucial requirement in choosing the solid-state hosts in nuclear clock applications. The IC of the isomer proceeds by resonantly exciting a valence band electron to a defect state, accompanied by multiphonon emission. We demonstrate that, if the process is energetically allowed, it generally quenches the isomer on a millisecond timescales, much faster than the isomer’s radiative lifetime, despite being in the charge state in the valence band.}, archive = {J_PRL}, author = {H. W. T. Morgan and H. B. Tran Tan and R. Elwell and A. N. Alexandrova and Eric R. Hudson and Andrei Derevianko}, doi = {10.1103/9s8f-hv1f}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253801}, shortjournal = {Phys. Rev. Lett.}, title = {Theory of internal conversion of the th229 nuclear isomer in solid-state hosts}, volume = {134}, year = {2025}, }
• (2025). Ultralow loss torsion micropendula for chipscale gravimetry. PRL, 134(25), 253602. (www)

  @article{ , abstract = {We explore a new class of chipscale torsion pendula formed by nanoribbon suspensions. Owing to their unique heirarchy of gravitational, tensile, and elastic stiffness, the devices exhibit damping rates of and parametric gravity sensitivities near that of an ideal pendulum. The suspension nonlinearity can also be used to cancel the pendulum nonlinearity, paving the way toward fully isochronous, high pendulum gravimeters. As a demonstration, we study a 0.1 mg, 32 Hz micropendulum with a damping rate of , a thermal acceleration sensitivity of , and a parametric gravity sensitivity of . We record Allan deviations as low as at 100 seconds, corresponding to a bias stability of . We also demonstrate a 100-fold cancellation of the pendulum nonlinearity. In addition to inertial sensing, our devices are well suited to proposed searches for new physics exploiting low-loss micro- to milligram-scale mechanical oscillators.}, archive = {J_PRL}, author = {C. A. Condos and J. R. Pratt and J. Manley and A. R. Agrawal and S. Schlamminger and C. M. Pluchar and D. J. Wilson}, doi = {10.1103/nmx5-hygh}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253602}, shortjournal = {Phys. Rev. Lett.}, title = {Ultralow loss torsion micropendula for chipscale gravimetry}, volume = {134}, year = {2025}, }
• (2025). Gaussian-to-non-gaussian transition of a quantum spin bath revealed by fourth-order correlation. PRL, 134(25), 253601. (www)

  @article{ , abstract = {Non-Gaussian fluctuations are one of the essential properties of quantum systems. However, the direct detection of non-Gaussian fluctuations has not yet been achieved in experiments since the specific order of correlation has to be isolated from the complex dynamics of the whole system. In this Letter, we measure the second- and fourth-order correlations of nuclear spins around a nitrogen vacancy center in diamond, using the recently developed quantum nonlinear spectroscopy. By adjusting the detection window and the spectral resolution, we observe the Gaussian to non-Gaussian transition of the multispin system. We find that the fourth-order correlation provides a fingerprint signal that can be used to identify individual spins with the same precession frequency, suggesting that Gaussianity is a potential quantum resource for quantum sensing. Our results shed light on the study of nonequilibrium quantum many-body dynamics and quantum materials at the nanoscale.}, archive = {J_PRL}, author = {Fan Xia and Shuowei Li and Xin-Yu Pan and Ping Wang and Gang-Qin Liu}, doi = {10.1103/4fdk-dblq}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253601}, shortjournal = {Phys. Rev. Lett.}, title = {Gaussian-to-non-gaussian transition of a quantum spin bath revealed by fourth-order correlation}, volume = {134}, year = {2025}, }
• (2025). Saturation of thermal and spin conductances in a dissipative superfluid junction. PRL, 134(25), 253403. (www)

  @article{ , abstract = {Fermionic superfluid junctions typically exhibit suppressed thermal and spin transport due to the presence of a pairing gap but allow coherent particle transport. While dissipation generally weakens coherent transport, it can also induce excitations that open other transport channels. In this work, we experimentally study a one-dimensional superfluid junction of strongly interacting fermions with local particle loss and observe dissipation-induced thermal and spin transport that appear to saturate at strong dissipation. Notably, in this regime, the measured thermal and spin conductances are comparable to the universal quantized conductance of one-dimensional ideal Fermi gas. Qualitatively similar behavior is observed for two dissipation mechanisms, either spin-imbalanced or pairwise losses. Our findings provide new insights into transport in interacting open quantum systems and suggest possibilities of dissipative control of spin and thermoelectric transport.}, archive = {J_PRL}, author = {Meng-Zi Huang and Philipp Fabritius and Jeffrey Mohan and Mohsen Talebi and Simon Wili and Tilman Esslinger}, doi = {10.1103/9ks8-zv9b}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253403}, shortjournal = {Phys. Rev. Lett.}, title = {Saturation of thermal and spin conductances in a dissipative superfluid junction}, volume = {134}, year = {2025}, }
• (2025). Stabilizing an ultracold fermi gas against fermi acceleration to superdiffusion through localization. PRL, 134(25), 253402. (www)

  @article{ , abstract = {Anderson localization, i.e., destructive quantum interference of multiple-scattering paths, halts transport entirely. Contrarily, time-dependent random forces expedite transport via Fermi acceleration, proposed as a mechanism for high-energy cosmic rays. Their competition creates interesting dynamics, but experimental observations are scarce. Here, we experimentally study the expansion of an ultracold Fermi gas inside time-dependent disorder and observe distinct regimes from sub- to superdiffusion. Unexpectedly, quantum interference counteracts acceleration in strong disorder before a transition to a diffusive state occurs in the driven system. Our system enables the investigation of Fermi acceleration in the quantum-transport regime.}, archive = {J_PRL}, author = {S. Barbosa and M. Kiefer-Emmanouilidis and F. Lang and J. Koch and A. Widera}, doi = {10.1103/rq4w-377l}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253402}, shortjournal = {Phys. Rev. Lett.}, title = {Stabilizing an ultracold fermi gas against fermi acceleration to superdiffusion through localization}, volume = {134}, year = {2025}, }
• (2025). Vortex to rotons transition in dipolar bose-einstein condensates. PRL, 134(25), 253401. (www)

  @article{ , abstract = {Dipolar Bose-Einstein condensates (dBECs) exhibit a plethora of physics phenomena, from supersolidity to the rotonlike minimum in the elementary excitation spectrum. In this work we first demonstrate the existence of axis-symmetric solitary waves in (quasi-)two-dimensional dBECs: these localized excitations are characterized by quantized vortex dipoles that continuously transit to vortex-free density depletions. We then show how the presence of the roton minimum fundamentally alters the fate of such solutions when approaching Landau’s critical speed: when propagating along the polarization direction where the roton minimum occurs, the solitary wave transits into roton excitations rather than into phonons as for standard contact-interaction BECs. This finding suggests that Feynman’s hypothesis, conjectured for 3D superfluid liquid helium regarding the creation of rotons as fading vortex excitations, is valid in the context of 2D dBECs.}, archive = {J_PRL}, author = {Alberto Villois and Miguel Onorato and Davide Proment}, doi = {10.1103/w9bj-bqq1}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253401}, shortjournal = {Phys. Rev. Lett.}, title = {Vortex to rotons transition in dipolar bose-einstein condensates}, volume = {134}, year = {2025}, }
• (2025). Collisional energy transfer in the highly reactive OH+–H2 system. PRL, 134(25), 253002. (www)

  @article{ , abstract = {Understanding the interplay between inelastic and reactive processes in low temperature molecular collisions is a true theoretical challenge. This study addresses this challenge by employing the statistical adiabatic channel model (SACM) to quantify the rotational excitation processes in the reactive system, such process being key in astrochemistry. The SACM approach demonstrates very good agreement with reduced dimensional close-coupling calculations in describing pure inelastic collisions in the low energy regime and satisfactory agreement with experimental measurement for treating reactive processes. Hence, the SACM approach can be considered as a good alternative to consider molecular collisions in reactive systems characterized by strongly bounded intermediate complexes, in absence of exact calculation in the low energy regime. Our findings reveal that reactive processes dominate the pure collisional excitation at all temperatures studied (5–300 K) by at least about one order of magnitude. This suggests a strong revision of the predicted abundance of in astrophysical environments since astrochemical models are presently significantly overestimating the impact of excitation induced by collisions.}, archive = {J_PRL}, author = {Paul Pirlot Jankowiak and François Lique}, doi = {10.1103/hpcb-q7wh}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253002}, shortjournal = {Phys. Rev. Lett.}, title = {Collisional energy transfer in the highly reactive OH+–H2 system}, volume = {134}, year = {2025}, }
• (2025). Photoelectron circular dichroism of a chiral molecule induced by resonant interatomic coulombic decay from an antenna atom. PRL, 134(25), 253001. (www)

  @article{ , abstract = {We show that a nonchiral atom can act as an antenna to induce a photoelectron circular dichroism in a nearby chiral molecule in a three-step process: The donor atom (antenna) is initially resonantly excited by circularly polarized radiation. It then transfers its excess energy to the acceptor molecule by means of resonant interatomic Coulombic decay. The latter finally absorbs the energy and emits an electron that exhibits the aforementioned circular dichroism in its angular distribution. We study the process on the basis of the retarded dipole–dipole interaction and report an asymptotic analytic expression for the distance-dependent chiral asymmetry of the photoelectron as induced by resonant interatomic Coulombic decay for random line-of-sight and acceptor orientations. In the nonretarded limit, the predicted chiral asymmetry is reversed as compared to that of a direct photoelectron circular dichroism of the molecule.}, archive = {J_PRL}, author = {Stefan Yoshi Buhmann and Andreas Hans and Janine C. Franz and Philipp V. Demekhin}, doi = {10.1103/vrjh-wx5j}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {253001}, shortjournal = {Phys. Rev. Lett.}, title = {Photoelectron circular dichroism of a chiral molecule induced by resonant interatomic coulombic decay from an antenna atom}, volume = {134}, year = {2025}, }
• (2025). Reduction in nuclear size and quadrupole deformation of high-spin isomers of in127,129. PRL, 134(25), 252501. (www)

  @article{ , abstract = {We employed laser spectroscopy of atomic transitions to measure the nuclear charge radii and electromagnetic properties of the high-spin isomeric states in neutron-rich indium isotopes ( ) near the closed proton and neutron shells at and . Our data reveal a reduction in the nuclear charge radius and intrinsic quadrupole moment when protons and neutrons are fully aligned in , to form the high spin isomer. Such a reduction is not observed in , where more complex configurations can be formed by the existence of four neutron holes. These observations are not consistently described by nuclear theory.}, archive = {J_PRL}, author = {A. R. Vernon and C. L. Binnersley and R. F. Garcia Ruiz and K. M. Lynch and T. Miyagi and J. Billowes and M. L. Bissell and T. E. Cocolios and J. P. Delaroche and J. Dobaczewski and M. Dupuis and K. T. Flanagan and W. Gins and M. Girod and G. Georgiev and R. P. de Groote and J. D. Holt and J. Hustings and Á. Koszorús and D. Leimbach and J. Libert and W. Nazarewicz and G. Neyens and N. Pillet and P.-G. Reinhard and S. Rothe and B. K. Sahoo and S. R. Stroberg and S. G. Wilkins and X. F. Yang and Z. Y. Xu and D. T. Yordanov}, doi = {10.1103/m35x-mw7z}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {252501}, shortjournal = {Phys. Rev. Lett.}, title = {Reduction in nuclear size and quadrupole deformation of high-spin isomers of in127,129}, volume = {134}, year = {2025}, }
• (2025). Explaining snowball-in-hell phenomena in heavy-ion collisions using a novel thermodynamic variable. PRL, 134(25), 252301. (www)

  @article{ , abstract = {A loosely bound hadronic molecule produced by a relativistic heavy-ion collision has been described as a “snowball in hell” since it emerges from a hadron resonance gas whose temperature is orders of magnitude larger than the binding energy of the molecule. This remarkable phenomenon can be explained in terms of a novel thermodynamic variable called the “contact” that is conjugate to the binding momentum of the molecule. The production rate of the molecule can be expressed in terms of the contact density at the kinetic freeze-out of the hadron resonance gas. It approaches a nonzero limit as the binding energy goes to 0.}, archive = {J_PRL}, author = {Eric Braaten and Kevin Ingles and Justin Pickett}, doi = {10.1103/7cjr-fgdw}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {252301}, shortjournal = {Phys. Rev. Lett.}, title = {Explaining snowball-in-hell phenomena in heavy-ion collisions using a novel thermodynamic variable}, volume = {134}, year = {2025}, }
• (2025). Jet rates in higgs boson decay at third order in QCD. PRL, 134(25), 251905. (www)

  @article{ , abstract = {We compute the production rates for two, three, four, and five jets in the hadronic decay of a Higgs boson in its two dominant decay modes to bottom quarks and gluons to third order in the QCD coupling constant. The five-, four-, and three-jet rates are obtained from a next-to-next-to-leading order calculation of Higgs decay to three jets, while the two-jet rate is inferred at next-to-next-to-next-to-leading order from the inclusive decay rate. Our results show distinct differences in the dependence of the jet rates on the jet resolution parameter between the two decay modes, supporting the aim of discriminating different Higgs boson decay channels via classic QCD observables.}, archive = {J_PRL}, author = {Elliot Fox and Aude Gehrmann-De Ridder and Thomas Gehrmann and Nigel Glover and Matteo Marcoli and Christian T. Preuss}, doi = {10.1103/1znh-sm96}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251905}, shortjournal = {Phys. Rev. Lett.}, title = {Jet rates in higgs boson decay at third order in QCD}, volume = {134}, year = {2025}, }
• (2025). Thrust distribution in electron-positron annihilation at full next-to-next-to-next-to-leading-logarithmic accuracy including next-to-next-to-leading-order terms in QCD. PRL, 134(25), 251904. (www)

  @article{ , abstract = {We consider the thrust ( ) distribution in electron-positron ( ) annihilation into hadrons and we perform the all-order resummation of the large logarithms of up to full next-to-next-to-next-to-leading logarithmic ( ) accuracy in QCD, also including the impact of next-order logarithmic corrections ( ). We consistently combine resummation with the known fixed-order results up to next-to-next-to-leading order (NNLO). All perturbative terms up to are included in our calculation, which, thanks to a unitarity constraint, exactly reproduces, after integration over , the next-to-next-to-next-to-leading order ( ) result for the total cross section of into hadrons. We perform resummation in the Laplace-conjugated space, which ensures the factorization of the kinematic momentum conservation constraint, and compare our results with those obtained using the resummation formalism in the physical ( ) space. We find that the differences in the spectra obtained with the two different formalisms are sizable. Nonperturbative corrections are included using an analytic hadronization model, depending on two free parameters. Finally, we present a comparison of our spectra with experimental data at the -boson mass ( ) energy, which enables us to extract the value of the QCD coupling , fully consistent with the world average. We explicitly show that resumming Sudakov logarithms in Laplace-conjugated space and evaluating the inverse Laplace transform exactly is crucial in order to obtain an accurate determination of the QCD coupling.}, archive = {J_PRL}, author = {Ugo Giuseppe Aglietti and Giancarlo Ferrera and Wan-Li Ju and Jiahao Miao}, doi = {10.1103/dv7n-qvyp}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251904}, shortjournal = {Phys. Rev. Lett.}, title = {Thrust distribution in electron-positron annihilation at full next-to-next-to-next-to-leading-logarithmic accuracy including next-to-next-to-leading-order terms in QCD}, volume = {134}, year = {2025}, }
• (2025). Energy-energy correlator for jet production in pp and pA collisions. PRL, 134(25), 251903. (www)

  @article{ , abstract = {In this Letter, we study the collinear limit of the energy-energy correlator in single-inclusive jet production in proton-proton and proton-nucleus collisions. We introduce a nonperturbative model that allows us to describe the energy-energy correlator in the entire angular region of the current experiments. Our results for proton-proton collisions show excellent agreement with CMS and ALICE data over a wide range of jet transverse momenta. For proton-nucleus collisions, we include modifications from the nuclear medium, and our predictions align well with the trends observed in recent ALICE measurements.}, archive = {J_PRL}, author = {João Barata and Zhong-Bo Kang and Xoán Mayo López and Jani Penttala}, doi = {10.1103/96xh-bd1w}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251903}, shortjournal = {Phys. Rev. Lett.}, title = {Energy-energy correlator for jet production in pp and pA collisions}, volume = {134}, year = {2025}, }
• (2025). Lattice-QCD computable quark correlation functions at three-loop order and extraction of splitting functions. PRL, 134(25), 251902. (www)

  @article{ , abstract = {We present the first complete next-to-next-to-next-to-leading-order calculation of the matching coefficients that link unpolarized flavor nonsinglet parton distribution functions with lattice QCD computable correlation functions. By using this high-order result, we notice a reduction in theoretical uncertainties compared to relying solely on previously known lower-order matching coefficients. Furthermore, based on this result we have extracted the three-loop unpolarized flavor nonsinglet splitting function, which is in agreement with the state-of-the-art result. Because of the simplicity of our method, it has the potential to advance the calculation of splitting functions to the desired four-loop order.}, archive = {J_PRL}, author = {Chen Cheng and Li-Hong Huang and Xiang Li and Zheng-Yang Li and Yan-Qing Ma}, doi = {10.1103/53ys-3n19}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251902}, shortjournal = {Phys. Rev. Lett.}, title = {Lattice-QCD computable quark correlation functions at three-loop order and extraction of splitting functions}, volume = {134}, year = {2025}, }
• (2025). Sullivan process near threshold and the pion gravitational form factors. PRL, 134(25), 251901. (www)

  @article{ , abstract = {We propose a novel method to experimentally access the gravitational form factors of the charged pion through the Sullivan process in electron-proton scattering. We demonstrate that the cross sections of photoproduction and electroproduction near the respective thresholds are dominated by the gluon gravitational form factor of the pion to next-to-leading order in perturbative QCD. We predict cross sections for the Electron-Ion Collider and the Jefferson Lab experiments.}, archive = {J_PRL}, author = {Yoshitaka Hatta and Jakob Schoenleber}, doi = {10.1103/y9fq-y84c}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251901}, shortjournal = {Phys. Rev. Lett.}, title = {Sullivan process near threshold and the pion gravitational form factors}, volume = {134}, year = {2025}, }
• (2025). First constraints on general neutrino interactions based on KATRIN data. PRL, 134(25), 251801. (www)

  @article{ , abstract = {The precision measurement of the tritium -decay spectrum performed by the KATRIN experiment provides a unique way to search for general neutrino interactions (GNIs). All theoretically allowed GNI terms at dimension 6 involving neutrinos are incorporated into a low-energy effective field theory, and can be identified by specific signatures in the measured tritium spectrum. In this Letter an effective description of the impact of GNIs on the spectrum is formulated and the first constraints on the effective GNI parameters are derived based on the electrons collected in the second measurement campaign of KATRIN in 2019. In addition, constraints on selected types of interactions are investigated, thereby exploring the potential of KATRIN to search for more specific new physics cases, including a right-handed W boson, a charged Higgs boson, or leptoquarks.}, archive = {J_PRL}, author = {KATRIN Collaboration and M. Aker and D. Batzler and A. Beglarian and J. Beisenkötter and M. Biassoni and B. Bieringer and Y. Biondi and F. Block and B. Bornschein and L. Bornschein and M. Böttcher and M. Carminati and A. Chatrabhuti and S. Chilingaryan and B. A. Daniel and M. Descher and D. Díaz Barrero and P. J. Doe and O. Dragoun and G. Drexlin and F. Edzards and K. Eitel and E. Ellinger and R. Engel and S. Enomoto and A. Felden and C. Fengler and C. Fiorini and J. A. Formaggio and C. Forstner and F. M. Fränkle and G. Gagliardi and K. Gauda and A. S. Gavin and W. Gil and F. Glück and R. Grössle and N. Gutknecht and V. Hannen and L. Hasselmann and K. Helbing and H. Henke and S. Heyns and R. Hiller and D. Hillesheimer and D. Hinz and T. Höhn and A. Huber and A. Jansen and K. Khosonthongkee and C. Köhler and L. Köllenberger and A. Kopmann and N. Kovač and L. La Cascio and T. Lasserre and J. Lauer and T. L. Le and O. Lebeda and B. Lehnert and G. Li and A. Lokhov and M. Machatschek and M. Mark and A. Marsteller and K. McMichael and C. Melzer and S. Mertens and S. Mohanty and J. Mostafa and K. Müller and A. Nava and H. Neumann and S. Niemes and A. Onillon and D. S. Parno and M. Pavan and U. Pinsook and A. W. P. Poon and J. M. L. Poyato and F. Priester and J. Ráliš and S. Ramachandran and R. G. H. Robertson and C. Rodenbeck and M. Röllig and R. Sack and A. Saenz and R. Salomon and P. Schäfer and K. Schlösser and M. Schlösser and L. Schlüter and S. Schneidewind and M. Schrank and J. Schürmann and A. K. Schütz and A. Schwemmer and A. Schwenck and J. Seeyangnok and M. Šefčík and D. Siegmann and F. Simon and J. Songwadhana and F. Spanier and D. Spreng and W. Sreethawong and M. Steidl and J. Štorek and X. Stribl and M. Sturm and N. Suwonjandee and N. Tan Jerome and H. H. Telle and L. A. Thorne and T. Thümmler and N. Titov and I. Tkachev and K. Urban and K. Valerius and D. Vénos and C. Weinheimer and S. Welte and J. Wendel and M. Wetter and C. Wiesinger and J. F. Wilkerson and J. Wolf and S. Wüstling and J. Wydra and W. Xu and S. Zadorozhny and G. Zeller}, doi = {10.1103/PhysRevLett.134.251801}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251801}, shortjournal = {Phys. Rev. Lett.}, title = {First constraints on general neutrino interactions based on KATRIN data}, volume = {134}, year = {2025}, }
• (2025). Gluing via intersection theory. PRL, 134(25), 251603. (www)

  @article{ , abstract = {Higher-point functions in super Yang-Mills theory can be constructed using integrability by triangulating the surfaces on which Feynman graphs would be drawn. It remains hard to analytically compute the necessary regluing of the tiles by virtual particles. We propose a new approach to study a series of residues encountered in the two-particle gluing of the planar one-loop five-point function of stress tensor multiplets. After exposing the twisted period nature of the integral functions, we employ intersection theory to derive canonical differential equations and present a solution.}, archive = {J_PRL}, author = {Giulio Crisanti and Burkhard Eden and Maximilian Gottwald and Pierpaolo Mastrolia and Tobias Scherdin}, doi = {10.1103/PhysRevLett.134.251603}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251603}, shortjournal = {Phys. Rev. Lett.}, title = {Gluing via intersection theory}, volume = {134}, year = {2025}, }
• (2025). Complex liouville string. PRL, 134(25), 251602. (www)

  @article{ , abstract = {We introduce the complex Liouville string, a solvable string theory defined by coupling two Liouville theories with complex conjugate central charges on the world sheet. We compute its amplitudes from first principles and establish a duality with a double-scaled two-matrix integral. We also analyze general world sheet boundaries and nonperturbative effects in the genus expansion. By expressing the complex Liouville string as a 2D dilaton gravity theory with a sine potential, we show that it admits both and vacua.}, archive = {J_PRL}, author = {Scott Collier and Lorenz Eberhardt and Beatrix Mühlmann and Victor A. Rodriguez}, doi = {10.1103/k74n-s63l}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251602}, shortjournal = {Phys. Rev. Lett.}, title = {Complex liouville string}, volume = {134}, year = {2025}, }
• (2025). Improved limits on the spin- and velocity-dependent exotic interaction in the micrometer range. PRL, 134(25), 251601. (www)

  @article{ , abstract = {Searching for exotic interactions beyond the standard model of particle physics may solve some of the current puzzles in physics. Here, the authors experimentally explore a spin- and velocity-dependent exotic interaction between the nucleons in a gold sphere and the electrons in a spin source in the micrometer range. The microfabricated spin source provides periodically varying spin density of electrons, resulting in a periodic exotic field. A cantilever glued with a gold sphere is used to measure the force acting on the gold sphere by the spin source. The spin source is driven to oscillate, and then, the imaginary component of the signal is extracted at the 10th harmonic of the oscillation frequency, which effectively separates the exotic interaction from the spurious forces commonly present in such short-range measurements. No signal of the exotic interaction is observed, then, new limits on the coupling constant are set in the interaction range below , with at .}, archive = {J_PRL}, author = {Sumin Li and Wenbo Zhang and Rui Luo and Jinquan Liu and Pengshun Luo}, doi = {10.1103/4bkl-cn8k}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251601}, shortjournal = {Phys. Rev. Lett.}, title = {Improved limits on the spin- and velocity-dependent exotic interaction in the micrometer range}, volume = {134}, year = {2025}, }
• (2025). Relieving scale disparity in binary black hole simulations. PRL, 134(25), 251402. (www)

  @article{ , abstract = {Worldtube excision is a method of reducing computational burden in numerical relativity simulations of binary black holes in situations where there is a good analytical model of the geometry around (one or both of) the objects. Two such scenarios of relevance in gravitational-wave astronomy are (1) the case of mass-disparate systems, and (2) the early inspiral when the separation is still large. Here we illustrate the utility and flexibility of this technique with simulations of the fully self-consistent radiative evolution in the model problem of a scalar charge orbiting a Schwarzschild black hole under the effect of scalar-field radiation reaction. We explore a range of orbital configurations, including inspirals with large eccentricity (which we follow through to the final plunge and ringdown) and hyperbolic scattering.}, archive = {J_PRL}, author = {Nikolas A. Wittek and Leor Barack and Harald P. Pfeiffer and Adam Pound and Nils Deppe and Lawrence E. Kidder and Alexandra Macedo and Kyle C. Nelli and William Throwe and Nils L. Vu}, doi = {10.1103/kskl-8dcj}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251402}, shortjournal = {Phys. Rev. Lett.}, title = {Relieving scale disparity in binary black hole simulations}, volume = {134}, year = {2025}, }
• (2025). One-loop corrections to near-extremal kerr thermodynamics from semiclassical virasoro blocks. PRL, 134(25), 251401. (www)

  @article{ , abstract = {We propose a method to perform an exact calculation of one-loop quantum corrections to black hole entropy in terms of Virasoro semiclassical blocks. We analyze in detail a four-dimensional Kerr black hole and show that in the near-extremal limit a branch of long-lived modes arises. We prove that the contribution of these modes accounts for a correction to the entropy for massless particles of spin , 2. We show that in the full calculation performed in the exact Kerr background the leading contribution actually is sourced by the near-horizon region only, and as such has a universal validity for any asymptotic behavior at infinity.}, archive = {J_PRL}, author = {Paolo Arnaudo and Giulio Bonelli and Alessandro Tanzini}, doi = {10.1103/cd6l-bl2s}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251401}, shortjournal = {Phys. Rev. Lett.}, title = {One-loop corrections to near-extremal kerr thermodynamics from semiclassical virasoro blocks}, volume = {134}, year = {2025}, }
• (2025). First search for ultralight dark matter using a magnetically levitated particle. PRL, 134(25), 251001. (www)

  @article{ , abstract = {We perform the first search for ultralight dark matter using a magnetically levitated particle. A submillimeter permanent magnet is levitated in a superconducting trap with a measured force sensitivity of . We find no evidence of a signal and derive limits on dark matter coupled to the difference between baryon and lepton number, in the mass range . Our most stringent limit on the coupling strength is . We propose the POLONAISE (Probing Oscillations using Levitated Objects for Novel Accelerometry In Searches of Exotic physics) experiment, which features short-, medium-, and long-term upgrades that will give us leading sensitivity in a wide mass range, demonstrating the promise of this novel quantum sensing technology in the hunt for dark matter.}, archive = {J_PRL}, author = {Dorian W. P. Amaral and Dennis G. Uitenbroek and Tjerk H. Oosterkamp and Christopher D. Tunnell}, doi = {10.1103/PhysRevLett.134.251001}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {251001}, shortjournal = {Phys. Rev. Lett.}, title = {First search for ultralight dark matter using a magnetically levitated particle}, volume = {134}, year = {2025}, }
• (2025). Efficient simulation of parametrized quantum circuits under nonunital noise through pauli backpropagation. PRL, 134(25), 250602. (www)

  @article{ , abstract = {As quantum devices continue to grow in size but remain affected by noise, it is crucial to determine when and how they can outperform classical computers on practical tasks. A central piece in this effort is to develop the most efficient classical simulation algorithms possible. Among the most promising approaches are Pauli backpropagation algorithms, which have already demonstrated their ability to efficiently simulate certain classes of parameterized quantum circuits—a leading contender for near-term quantum advantage—under random circuit assumptions and depolarizing noise. However, their efficiency was not previously established for more realistic nonunital noise models, such as amplitude damping, that better capture noise on existing hardware. Here, we close this gap by adapting Pauli backpropagation to nonunital noise, proving that it remains efficient even under these more challenging conditions. Our proof leverages a refined combinatorial analysis to handle the complexities introduced by nonunital channels, thus strengthening Pauli backpropagation as a powerful tool for simulating near-term quantum devices.}, archive = {J_PRL}, author = {Victor Martinez and Armando Angrisani and Ekaterina Pankovets and Omar Fawzi and Daniel Stilck França}, doi = {10.1103/j1gg-s6zb}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {250602}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient simulation of parametrized quantum circuits under nonunital noise through pauli backpropagation}, volume = {134}, year = {2025}, }
• (2025). Exact calculations of coherent information for toric codes under decoherence: Identifying the fundamental error threshold. PRL, 134(25), 250601. (www)

  @article{ , abstract = {The toric code is a canonical example of a topological error-correcting code. Two logical qubits stored within the toric code are robust against local decoherence, ensuring that these qubits can be faithfully retrieved as long as the error rate remains below a certain threshold. Recent studies have explored such a threshold behavior as an intrinsic information-theoretic transition, independent of the decoding protocol. These studies have shown that information-theoretic metrics, calculated using the Renyi (replica) approximation, demonstrate sharp transitions at a specific error rate. However, an exact analytic expression that avoids using the replica trick has not been shown, and the connection between the transition in information-theoretic capacity and the random bond Ising model (RBIM) has only been indirectly established. In this Letter, we present the first analytic expression for the coherent information of a decohered toric code, thereby establishing a rigorous connection between the fundamental error threshold and the criticality of the RBIM.}, archive = {J_PRL}, author = {Jong Yeon Lee}, doi = {10.1103/hlfh-86yz}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {250601}, shortjournal = {Phys. Rev. Lett.}, title = {Exact calculations of coherent information for toric codes under decoherence: Identifying the fundamental error threshold}, volume = {134}, year = {2025}, }
• (2025). Stability and loop models from decohering non-abelian topological order. PRL, 134(25), 250403. (www)

  @article{ , abstract = {Decohering topological order (TO) is central to the many-body physics of open quantum matter and decoding transitions. We identify statistical mechanical models for decohering non-Abelian TOs, which have been crucial for understanding the error threshold of Abelian stabilizer codes. The decohered density matrix can be described by loop models, whose topological loop weight is the quantum dimension of the decohering anyon—reducing to the Ising model if . In particular, the Rényi- moments correspond to coupled loop models. Moreover, by diagonalizing the density matrix at maximal error rate, we connect the fidelity between two logically distinct ground states to random loop and spin models. We find a remarkable stability to quantum channels which proliferate non-Abelian anyons with large quantum dimension, with the possibility of critical phases for smaller dimensions. Intuitively, this stability is due to non-Abelian anyons not admitting finite-depth string operators. We confirm our framework with exact results for Kitaev quantum double models, and with numerical simulations for the non-Abelian phase of the Kitaev honeycomb model. Our work opens up the possibility of non-Abelian TO being robust against maximally proliferating certain anyons, which can inform error-correction studies of these topological memories.}, archive = {J_PRL}, author = {Pablo Sala and Ruben Verresen}, doi = {10.1103/fy9r-hpcw}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {250403}, shortjournal = {Phys. Rev. Lett.}, title = {Stability and loop models from decohering non-abelian topological order}, volume = {134}, year = {2025}, }
• (2025). 1D spontaneous symmetry breaking in thermal equilibrium via non-hermitian construction. PRL, 134(25), 250402. (www)

  @article{ , abstract = {Spontaneous symmetry breaking generally circumvents one-dimensional systems with local interactions in thermal equilibrium. Here, we analyze a category of one-dimensional Hermitian models via local non-Hermitian constructions. Notably, spontaneous symmetry breaking and long-range order may emerge at finite temperatures in such systems under periodic boundary conditions, in sharp contrast to Hermitian constructions. We demonstrate clear numerical evidence, such as order parameters and specific heat, supporting phase diagrams with robust ordered phases. Non-Hermitian physics plays a vital role in prohibiting domain-wall proliferation and promoting spontaneous symmetry breaking. The fermions exhibit an exotic topological nature in their path-integral windings, which uphold nonzero integers—commonly a non-Hermitian signature—in the ordered phases, thus offering a novel and spontaneous origin for both symmetry breaking and non-Hermiticity.}, archive = {J_PRL}, author = {Jia-Bao Wang and Zi-Hao Dong and Yi Zhang}, doi = {10.1103/p5fv-c9dj}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {250402}, shortjournal = {Phys. Rev. Lett.}, title = {1D spontaneous symmetry breaking in thermal equilibrium via non-hermitian construction}, volume = {134}, year = {2025}, }
• (2025). Global becomes local: Efficient many-body dynamics for global master equations. PRL, 134(25), 250401. (www)

  @article{ , abstract = {This Letter makes progress on the issue of global vs local master equations. Global master equations like the Redfield master equation (following from standard Born and Markov approximation) require a full diagonalization of the system Hamiltonian. This is especially challenging for interacting quantum many-body systems. We discuss a short-bath-correlation-time expansion in reciprocal (energy) space, leading to a series expansion of the jump operator, which avoids a diagonalization of the Hamiltonian. For a bath that is coupled locally to one site, this typically leads to an expansion of the global Redfield jump operator in terms of local operators. We additionally map the local Redfield master equation to a novel local Lindblad form, giving an equation which has the same conceptual advantages of traditional local Lindblad approaches while being applicable in a much broader class of systems. Our ideas give rise to a nonheuristic foundation of local master equations, which can be combined with established many-body methods.}, archive = {J_PRL}, author = {Alexander Schnell}, doi = {10.1103/1q5b-p2bf}, journal = {Physical Review Letters}, month = {6}, number = {25}, pages = {250401}, shortjournal = {Phys. Rev. Lett.}, title = {Global becomes local: Efficient many-body dynamics for global master equations}, volume = {134}, year = {2025}, }
• (2025). Erratum: Observation of oriented landau levels and helical zero modes in berry dipole acoustic crystals [Phys. rev. lett. 134, 116604 (2025)]. PRL, 134(24), 249901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 249901 (2025)}, archive = {J_PRL}, author = {Qingyang Mo and Riyi Zheng and Cuicui Lu and Xueqin Huang and Zhengyou Liu and Shuang Zhang}, doi = {10.1103/r853-kbrg}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {249901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Observation of oriented landau levels and helical zero modes in berry dipole acoustic crystals [Phys. rev. lett. 134, 116604 (2025)]}, volume = {134}, year = {2025}, }
• (2025). Scaling law for epithelial tissue rheology. PRL, 134(24), 248401. (www)

  @article{ , abstract = {Epithelial morphogenesis is a process through which simple cellular sheets are shaped into complex tissues and organs in a developing animal. From a physics perspective, understanding any shape change requires knowing the active forces driving its dynamics, as well as the material properties, i.e., the rheology, of the material that is undergoing the deformation. Despite a long-standing effort, rheological properties of embryonic tissues have remained elusive. Here, we develop a minimal theory providing a comprehensive explanation of rheological measurements characterizing the mechanics of epithelia in the early fly embryo. Our theory explains a key experimental observation: when subjected to concentrated pulling force, the embryonic epithelium of the fruit fly Drosophila melanogaster deforms following a power law with an exponent of . All dimensional parameters of our theory are constrained by direct measurements and have allowed us to estimate the spring constant of an individual cellular edge. We show that stress relaxation (attributable to actin turnover), stretching elasticity of individual cellular edges, and the floppy topology of the cellular network are the sole physical properties governing tissue rheology on the developmentally relevant time scale of 1–10 minutes.}, archive = {J_PRL}, author = {M. I. Cheikh and N. Rodriguez and K. Doubrovinski}, doi = {10.1103/v1qt-zg86}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {248401}, shortjournal = {Phys. Rev. Lett.}, title = {Scaling law for epithelial tissue rheology}, volume = {134}, year = {2025}, }
• (2025). Kinetic theory of decentralized learning for smart active matter. PRL, 134(24), 248302. (www)

  @article{ , abstract = {Smart active matter has the ability to control its motion guided by individual policies to achieve collective goals. We introduce a theoretical framework to study a decentralized learning process in which agents can locally exchange policies to adapt their behavior and maximize a predefined reward function. We use our formalism to derive explicit hydrodynamic equations for the policy dynamics. We apply the theory to two different microscopic models where policies correspond either to fixed parameters similar to evolutionary dynamics or to state-dependent controllers known from the field of robotics. We find good agreement between theoretical predictions and agent-based simulations. By deriving fundamental control parameters and uncertainty relations, our work lays the foundations for a statistical physics analysis of decentralized learning.}, archive = {J_PRL}, author = {Gerhard Jung and Misaki Ozawa and Eric Bertin}, doi = {10.1103/5m44-kwhv}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {248302}, shortjournal = {Phys. Rev. Lett.}, title = {Kinetic theory of decentralized learning for smart active matter}, volume = {134}, year = {2025}, }
• (2025). Hyperuniform networks of active magnetic robotic spinners. PRL, 134(24), 248301. (www)

  @article{ , abstract = {Disorder hyperuniform (DHU) systems possess a hidden long-range order manifested as the complete suppression of normalized large-scale density fluctuations like crystals, which endows them with many unique properties. Here, we demonstrate a new organization mechanism for achieving stable DHU structures in active-particle systems via investigating the self-assembly of robotic spinners with threefold symmetric magnetic binding sites up to a heretofore experimentally unattained system size, i.e., with robots. The spinners can self-organize into a wide spectrum of actively rotating three-coordinated network structures, among which a set of stable DHU networks robustly emerge. These DHU networks are topological transformations of a honeycomb network by continuously introducing the Stone-Wales defects, which are resulted from the competition between tunable magnetic binding and local twist due to active rotation of the robots. Our results reveal novel mechanisms for emergent DHU states in active systems and achieving novel DHU materials with desirable properties.}, archive = {J_PRL}, author = {Jing Wang and Zihao Sun and Huaicheng Chen and Gao Wang and Duyu Chen and Guo Chen and Jianwei Shuai and Mingcheng Yang and Yang Jiao and Liyu Liu}, doi = {10.1103/z2rp-21xn}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {248301}, shortjournal = {Phys. Rev. Lett.}, title = {Hyperuniform networks of active magnetic robotic spinners}, volume = {134}, year = {2025}, }
• (2025). Soft spots in shell buckling. PRL, 134(24), 248201. (www)

  @article{ , abstract = {The energy landscape of thin shells under quasistatic loading represents their potential energy as a function of their shape. It has recently been shown for a narrow plate [S. Lachmann and S. M. Rubinstein, Phil. Trans. R. Soc. A 381 , 2244 (2023) ] that lateral probing can induce controlled trajectories in configuration space, providing an experimental method for measuring the energy landscape of a specific structure. In this Letter, we extend this method to explore the prebuckling behavior of poked cylindrical shells through the lens of the energy landscape. This approach offers an intuitive way to combine and synthesize the deformation responses from different probing locations into a cohesive description of the prebuckling dynamics, revealing the presence of local soft spots—regions where the structure is particularly susceptible to deformation. As the system is loaded, these soft spots appear as local minima in the energy barrier to buckling and are experimentally shown to act as attractors of nearby deformation. The energy landscape framework provides a general framework for understanding prebuckling dynamics, highlighting the role of spatially extended deformations and offering a new way of safely estimating shock sensitivity to buckling in real shells.}, archive = {J_PRL}, author = {Sagy Lachmann and Shmuel M. Rubinstein}, doi = {10.1103/m1x2-rx4p}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {248201}, shortjournal = {Phys. Rev. Lett.}, title = {Soft spots in shell buckling}, volume = {134}, year = {2025}, }
• (2025). Stochastic resetting prevails over sharp restart for broad target distributions. PRL, 134(24), 247102. (www)

  @article{ , abstract = {Resetting has been shown to reduce the completion time for a stochastic process, such as the first passage time for a diffusive searcher to find a target. The time between two consecutive resetting events is drawn from a waiting time distribution , which defines the resetting protocol. Previously, it has been shown that deterministic resetting process with a constant time period, referred to as sharp restart, can minimize the mean first passage time to a fixed target. Here, we consider the more realistic problem of a target positioned at a random distance from the resetting site, selected from a given target distribution . We introduce the notion of a conjugate target distribution to a given waiting time distribution. The conjugate target distribution, is that for which extremizes the mean time to locate the target. In the case of diffusion we derive an explicit expression for conjugate to a given that holds in arbitrary spatial dimension. Our results show that stochastic resetting prevails over sharp restart for target distributions with exponential or heavier tails.}, archive = {J_PRL}, author = {Martin R. Evans and Somrita Ray}, doi = {10.1103/2wpq-gl2j}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {247102}, shortjournal = {Phys. Rev. Lett.}, title = {Stochastic resetting prevails over sharp restart for broad target distributions}, volume = {134}, year = {2025}, }
• (2025). Tracer and current fluctuations in driven diffusive systems. PRL, 134(24), 247101. (www)

  @article{ , abstract = {Interacting particles diffusing in single file is a fundamental model of transport in narrow channels where particles cannot bypass each other. An important result has been obtained by Kollmann [ Phys. Rev. Lett. 90 , 180602 (2003) ] for the mean square displacement of a tracer for any single-file model. It applies to any diffusive system, in particular the notable classes of colloidal systems and diffusive stochastic lattice gases. Since then, no analog result has been obtained in the important case where the particles are driven by an external field. Here, we fill this gap and determine the fluctuations and the skewness of the tracer’s position for any driven diffusive system. In addition, we also consider a variety of important observables such as the integrated current, the response of the system to the perturbation induced by the displacement of the tracer, and the correlations between several tracers. Furthermore, we also unveil fundamental relations underlying the out-of-equilibrium dynamics of driven diffusive systems. This work constitutes a step toward the determination of the full distribution of all these observables in driven one-dimensional systems of interacting particles.}, archive = {J_PRL}, author = {Théotim Berlioz and Olivier Bénichou and Aurélien Grabsch}, doi = {10.1103/4j5q-j4ht}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {247101}, shortjournal = {Phys. Rev. Lett.}, title = {Tracer and current fluctuations in driven diffusive systems}, volume = {134}, year = {2025}, }
• (2025). Self-powered pure spin photocurrent in bent CrSBr monolayer. PRL, 134(24), 247001. (www)

  @article{ , abstract = {With the booming development of two-dimensional (2D) flexible devices, flexure has attracted much attention as an emerging means to modulate device performances. Here, the magnetic-optical-electrical multifield coupling mechanism of spin photocurrent in bent CrSBr monolayer is investigated through first-principles calculations. The studies show that simple mechanical bending of monolayer CrSBr can successfully achieve the spatial separation of electrons and holes. The nonequilibrium process of photogenerated carriers in bent CrSBr modulates both the shift current density and the ballistic current density, thereby enabling the photovoltaic effect. Meanwhile, the built-in electric field generated by flexure drives the device toward more efficient self-powered behavior. Moreover, this self-powered polarization devices have excellent spin photovoltaic properties and high polarization sensitivity. The present Letter creates novel opportunities for 2D spintronics and opens new avenues for realizing self-powered polarization devices.}, archive = {J_PRL}, author = {Hongli Chen (陈红丽 and Li Chen (陈立 and Liyuan Chen (陈丽媛 and Liyan Shang (商丽燕 and Yawei Li (李亚巍 and Liangqing Zhu (朱亮清 and Junhao Chu (褚君浩 and Shijing Gong (龚士静 and Zhigao Hu (胡志高}, doi = {10.1103/s8qn-n8tr}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {247001}, shortjournal = {Phys. Rev. Lett.}, title = {Self-powered pure spin photocurrent in bent CrSBr monolayer}, volume = {134}, year = {2025}, }
• (2025). Excited-state trions in a quantum well. PRL, 134(24), 246902. (www)

  @article{ , abstract = {We report on the observation of an excited 2 s state of a trion in a 4.2 nm wide doped GaAs / Al 0.3 Ga 0.7 As quantum well using magneto-optical Kerr effect (MOKE) spectroscopy under out-of-plane magnetic fields up to 6 T. This resonance appears slightly below the 2 s exciton in energy. Strikingly, the 2 s trion is found to be bound only for magnetic fields larger than 1 T. The signature of the 2 s trion is absent in the magnetoreflectance spectra, while it is detectable in the MOKE spectra signifying the importance of the powerful technique. Similar to the 1 s states, the 2 s trion shows an opposite degree of magnetic-field-induced polarization compared to its exciton counterpart, in agreement with our theoretical calculations. This transfer of oscillator strength between the complexes establishes an optical fingerprint of the 2 s excited trion.}, archive = {J_PRL}, author = {Sourabh Jain and Mikhail Glazov and Ashish Arora}, doi = {10.1103/8181-jzj5}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246902}, shortjournal = {Phys. Rev. Lett.}, title = {Excited-state trions in a quantum well}, volume = {134}, year = {2025}, }
• (2025). Cavity spectroscopy for strongly correlated polaritonic systems. PRL, 134(24), 246901. (www)

  @article{ , abstract = {Embedding materials in optical cavities has emerged as an intriguing perspective for controlling quantum materials, but a key challenge lies in measuring properties of the embedded matter. Here, we propose a framework for probing strongly correlated cavity-embedded materials through direct measurements of cavity photons. We derive general relations between photon and matter observables inside the cavity, and show how these can be measured via the emitted photons. As an example, we demonstrate how the entanglement phase transition of an embedded molecule can be accessed by measuring the cavity photon occupation, and showcase how dynamical spin correlation functions can be accessed by measuring dynamical photon correlation functions. Our framework provides an all-optical method to measure static and dynamic properties of cavity-embedded materials.}, archive = {J_PRL}, author = {Lukas Grunwald and Emil Viñas Boström and Mark Kamper Svendsen and Dante M. Kennes and Angel Rubio}, doi = {10.1103/1lpw-22np}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246901}, shortjournal = {Phys. Rev. Lett.}, title = {Cavity spectroscopy for strongly correlated polaritonic systems}, volume = {134}, year = {2025}, }
• (2025). Electrically controlled nonlinear magnon-magnon coupling in a synthetic antiferromagnet. PRL, 134(24), 246704. (www)

  @article{ , abstract = {We investigate the nonlinear coupling between acoustic (ac) and optical (op) modes in the coupled magnetization dynamics of synthetic antiferromagnets, utilizing current-driven resonance spectroscopy. A clear spectral splitting is evident in the ac mode when strongly excited by the radio frequency current at a driving frequency half that of the op mode resonance. The Landau-Lifshitz phenomenology aligns with the experimental observations, affirming the coupling of the radio-frequency-excited ac and op modes through three-magnon mixing. The nonlinearity enables a Rabi-like splitting in an in-plane magnetized synthetic antiferromagnet without breaking its natural symmetries. This discovery holds potential for advancing our understanding of nonlinear antiferromagnetic dynamics.}, archive = {J_PRL}, author = {A. Sud and K. Yamamoto and S. Iihama and K. Ishibashi and S. Fukami and H. Kurebayashi and S. Mizukami}, doi = {10.1103/sc6y-rxbg}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246704}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically controlled nonlinear magnon-magnon coupling in a synthetic antiferromagnet}, volume = {134}, year = {2025}, }
• (2025). Tunneling magnetoresistance in altermagnetic RuO2-based magnetic tunnel junctions. PRL, 134(24), 246703. (www)

  @article{ , abstract = {Altermagnets exhibit characteristics akin to antiferromagnets, with spin-split anisotropic bands in momentum space. has been considered as a prototype altermagnet; however, recent reports have questioned altermagnetic ground state in this material. In this Letter, we demonstrate spin-dependent tunneling magnetoresistance (TMR) in -based magnetic tunnel junctions, which suggests the spin-splitted anisotropic band structure of our films. The observed TMR is contingent on the direction of the Néel vector of and reverse its sign by the inversion of the Néel vector. These results reflect the altermagnetic nature of and highlight its potential for spintronic applications, leveraging the combined strengths of ferromagnetic and antiferromagnetic systems.}, archive = {J_PRL}, author = {Seunghyeon Noh and Gye-Hyeon Kim and Jiyeon Lee and Hyeonjung Jung and Uihyeon Seo and Gimok So and Jaebyeong Lee and Seunghyun Lee and Miju Park and Seungmin Yang and Yoon Seok Oh and Hosub Jin and Changhee Sohn and Jung-Woo Yoo}, doi = {10.1103/nrk5-5zrj}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246703}, shortjournal = {Phys. Rev. Lett.}, title = {Tunneling magnetoresistance in altermagnetic RuO2-based magnetic tunnel junctions}, volume = {134}, year = {2025}, }
• (2025). Probing ultrafast magnetization dynamics via synthetic axion fields. PRL, 134(24), 246702. (www)

  @article{ , abstract = {Spatial structuring of materials at subwavelength scales underlies the concept of metamaterials possessing exotic properties beyond those of the constituent media. Temporal modulation of material parameters enables further functionalities. Here, we show that high-frequency oscillations of spatially uniform magnetization generate an effective dynamic axion field embedding the amplitude and phase of magnetization oscillations. This allows one to map ultrafast magnetization dynamics using a probe signal with much lower frequency.}, archive = {J_PRL}, author = {Leon Shaposhnikov and Eduardo Barredo-Alamilla and Frank Wilczek and Maxim A. Gorlach}, doi = {10.1103/2rrr-glyn}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246702}, shortjournal = {Phys. Rev. Lett.}, title = {Probing ultrafast magnetization dynamics via synthetic axion fields}, volume = {134}, year = {2025}, }
• (2025). Phonon-driven multipolar dynamics in a spin-orbit coupled mott insulator. PRL, 134(24), 246701. (www)

  @article{ , abstract = {Motivated by advances in pump-probe experiments and light-driven phenomena, we theoretically study the impact of pumped and driven phonons in Mott insulators which host multipole moments, thus going beyond conventional dipolar magnetism. As a case study, we examine pseudospin- Mott insulators hosting quadrupolar and octupolar moments, and investigate the effect of resonantly exciting phonon modes which couple linearly to the quadrupoles. We show that this leads to multipolar precession, with the backaction resulting in pseudochiral phonon dynamics in the octupolar ordered phase. We further study the impact of a short-time two-phonon drive, showing that it can induce the buildup of octupolar order or even switch its sign on picosecond timescales. Our results are obtained using a Monte Carlo code incorporating phonons, molecular dynamics simulations to numerically integrate the coupled spin-phonon equations of motion, and analytical Floquet theory. Our work shows how driven phonons can probe and control hidden orders in solids.}, archive = {J_PRL}, author = {Kathleen Hart and Ruairidh Sutcliffe and Gil Refael and Arun Paramekanti}, doi = {10.1103/1rmw-pd6n}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246701}, shortjournal = {Phys. Rev. Lett.}, title = {Phonon-driven multipolar dynamics in a spin-orbit coupled mott insulator}, volume = {134}, year = {2025}, }
• (2025). Movable dirac points with ferroelectrics: Kink states and berry curvature dipoles. PRL, 134(24), 246602. (www)

  @article{ , abstract = {Two-dimensional (2D) Dirac states and Dirac points with linear dispersion are the hallmark of graphene, topological insulators, semimetals, and superconductors. Lowering a symmetry by the ferroelectric polarization opens the gap in Dirac points and introduces finite Berry curvature. Combining this with Dirac points detached from high symmetry points of the Brillouin zone offers additional ways to tailor topological properties. We explore this concept by studying topological phenomena emerging in 2D materials with movable Dirac points and broken out-of-plane mirror reflection. The resulting topological kink states and Berry curvature dipoles are changed by movable 2D Dirac points with experimental signatures in electrical conductance and second-harmonic nonlinear Hall conductivity. We identify materials platforms where our predictions can be realized and support that with the first-principles results for -GeS junction.}, archive = {J_PRL}, author = {Konstantin S. Denisov and Yuntian Liu and Igor Žutić}, doi = {10.1103/ps7y-vmz1}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246602}, shortjournal = {Phys. Rev. Lett.}, title = {Movable dirac points with ferroelectrics: Kink states and berry curvature dipoles}, volume = {134}, year = {2025}, }
• (2025). Fractality-induced topology. PRL, 134(24), 246601. (www)

  @article{ , abstract = {Fractal geometries, characterized by self-similar patterns and noninteger dimensions, provide an intriguing platform for exploring topological phases of matter. In this Letter, we introduce a theoretical framework that leverages isospectral reduction to effectively simplify complex fractal structures, revealing the presence of topologically protected boundary and corner states. Our approach demonstrates that fractals can support topological phases, even in the absence of traditional driving mechanisms such as magnetic fields or spin-orbit coupling. The isospectral reduction not only elucidates the underlying topological features but also makes this framework broadly applicable to a variety of fractal systems. Furthermore, our findings suggest that these topological phases may naturally occur in materials with fractal structures found in nature. This Letter opens new avenues for designing fractal-based topological materials, advancing both theoretical understanding and experimental exploration of topology in complex, self-similar geometries.}, archive = {J_PRL}, author = {L. Eek and Z. F. Osseweijer and C. Morais Smith}, doi = {10.1103/jcrl-9dz6}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246601}, shortjournal = {Phys. Rev. Lett.}, title = {Fractality-induced topology}, volume = {134}, year = {2025}, }
• (2025). Quantum disorder induced by nuclear tunneling in lattice. PRL, 134(24), 246401. (www)

  @article{ , abstract = {Lattice degrees of freedom (d.o.f.) may induce quantum disorder (QD) when nuclear tunneling outvies long-range order, but conventional phonon theory is incapable of describing such QD phases. Here we develop a method based on path-integral molecular dynamics to solve this problem. Its accuracy is verified in a double-well chain model and it is applied to a real material from first principles. A quantum order-disorder-order phase transition sequence is demonstrated when varying the strength of quantum fluctuations using the lattice constants as the tuning factor. Combining the excitation spectra and Rényi entanglement entropy, we pinpoint the QD region. This picture may be general in lattice systems having soft phonon modes, not limited to quantum paraelectricity, in which novel entangled lattice motion and its coupling with other d.o.f. can be expected.}, archive = {J_PRL}, author = {Yu-Cheng Zhu and Jia-Xi Zeng and Qi-Jun Ye and Xin-Zheng Li}, doi = {10.1103/9gkl-w2lm}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum disorder induced by nuclear tunneling in lattice}, volume = {134}, year = {2025}, }
• (2025). Hidden self duality and exact mobility edges in quasiperiodic network models. PRL, 134(24), 246301. (www)

  @article{ , abstract = {In one-dimensional quasiperiodic systems, only a few models with exact mobility edges (MEs) have been constructed using generalized self duality theory, Avila’s global theory, or the renormalization group method. This raises an intriguing question of whether we can realize more physical models with exact solvable MEs. In this Letter, we uncover the hidden self duality within a class of quasiperiodic network models constituted by periodic and quasiperiodic sites. Although the original Hamiltonians appear to lack self duality, their effective Hamiltonians obtained by integrating out the periodic sites exhibit self duality, which yield MEs. The well-studied mosaic model, which is the simplest case of quasiperiodic network models, was previously thought to exhibit MEs due to the absence of self duality, but we show that they actually arise from the hidden self duality. Using the effective Hamiltonian, we further introduce the concept of resonant states to understand the shape of MEs. Finally, we present in detail how to determine the MEs in various network models, including some non-Hermitian models, based on the hidden self duality. These predictions can be experimentally realized using optical and acoustic waveguide arrays. Our work can greatly advance our understanding of MEs in Anderson transition.}, archive = {J_PRL}, author = {Hai-Tao Hu and Xiaoshui Lin and Ai-Min Guo and Guangcan Guo and Zijing Lin and Ming Gong}, doi = {10.1103/rl1f-ptzq}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246301}, shortjournal = {Phys. Rev. Lett.}, title = {Hidden self duality and exact mobility edges in quasiperiodic network models}, volume = {134}, year = {2025}, }
• (2025). Full-gap superconductivity in BaAs/Ferropnictide heterostructures. PRL, 134(24), 246203. (www)

  @article{ , abstract = {Interfacial interactions often promote the emergence of unusual phenomena in two-dimensional systems, including high-temperature superconductivity. Here, we report the observation of full-gap superconductivity with a maximal spectroscopic temperature up to 26 K in a BaAs monolayer grown on ferropnictide Ba ( Fe 1 − x Co x ) 2 As 2 (abbreviated as BFCA) epitaxial films. The superconducting gap remains robust even when the thickness of underlying BFCA is reduced to the monolayer limit, in contrast to the rapid suppression of T c in standalone BFCA thin films. We reveal that the exceptional crystallinity of the BaAs / BFCA heterostructures, featured by their remarkable electronic and geometric uniformities, is crucial for the emergent full-gap superconductivity with mean-field temperature dependence and pronounced bound states within magnetic vortices. Our findings open up new avenues to unravel the mysteries of unconventional superconductivity in ferropnictides and advance the development of FeAs-based heterostructures.}, archive = {J_PRL}, author = {Ming-Qiang Ren and Qiang-Jun Cheng and Hui-Hui He and Ze-Xian Deng and Fang-Jun Cheng and Yong-Wei Wang and Cong-Cong Lou and Qinghua Zhang and Lin Gu and Kai Liu and Xu-Cun Ma and Qi-Kun Xue and Can-Li Song}, doi = {10.1103/jmrh-347m}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246203}, shortjournal = {Phys. Rev. Lett.}, title = {Full-gap superconductivity in BaAs/Ferropnictide heterostructures}, volume = {134}, year = {2025}, }
• (2025). Kibble-zurek dynamics in the anisotropic ising model of the si(001) surface. PRL, 134(24), 246202. (www)

  @article{ , abstract = {As a simplified description of the nonequilibrium dynamics of buckled dimers on the Si(001) surface, we consider the anisotropic two-dimensional (2D) Ising model and study the freezing of spatial correlations during a cooling quench across the critical point. Depending on the cooling rate, we observe a crossover from one-dimensional (1D) to 2D behavior. For rapid cooling, we find effectively 1D behavior in the strongly coupled direction, for which we provide an exact analytic solution of the nonequilibrium dynamics. For slower cooling rates, we start to see 2D behavior where our numerical simulations show an approach to the usual Kibble–Zurek scaling in 2D.}, archive = {J_PRL}, author = {G. Schaller and F. Queisser and S. P. Katoorani and C. Brand and C. Kohlfürst and M. R. Freeman and A. Hucht and P. Kratzer and B. Sothmann and M. Horn-von Hoegen and R. Schützhold}, doi = {10.1103/rmc4-xqb3}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246202}, shortjournal = {Phys. Rev. Lett.}, title = {Kibble-zurek dynamics in the anisotropic ising model of the si(001) surface}, volume = {134}, year = {2025}, }
• (2025). Contribution of water molecules to the electronic dipole moment across the gold-water interface. PRL, 134(24), 246201. (www)

  @article{ , abstract = {Understanding metal-water interfaces is instrumental in developing electrochemical cells for energy conversion. In this Letter, we quantify the relative contribution of the metal surface and the solvent molecules to the electronic component of the interfacial dipole moment enabled by an implementation of partially occupied Wannier functions that allows us to treat interfacial water in contact with metallic surfaces. Our calculations show that the contribution of the solvent is of overriding importance and that it mostly originates from specific deformation of the water lone pairs very close to the metal surface.}, archive = {J_PRL}, author = {Soumya Ghosh and Chanbum Park and Harald Forbert and Dominik Marx}, doi = {10.1103/873j-rx8d}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246201}, shortjournal = {Phys. Rev. Lett.}, title = {Contribution of water molecules to the electronic dipole moment across the gold-water interface}, volume = {134}, year = {2025}, }
• (2025). Neural canonical transformations for quantum anharmonic solids of lithium. PRL, 134(24), 246101. (www)

  @article{ , abstract = {Lithium is a typical quantum solid, characterized by cubic structures at ambient pressure. As the pressure increases, it forms more complex structures and undergoes a metal-to-semiconductor transformation, complicating theoretical and experimental analyses. We employ the neural canonical transformation approach, a variational method based on probabilistic generative models, to investigate the quantum anharmonic effects in lithium solids at finite temperatures. This approach combines a normalizing flow for phonon excited-state wave functions with a probabilistic model for the occupation of energy levels, optimized jointly to minimize the free energy. Our results indicate that quantum anharmonicity lowers the bcc - fcc transition temperature compared to classical molecular dynamics predictions. At high pressures, the predicted fractional coordinates of lithium atoms in the cI16 structure show good quantitative agreement with experimental observations. Finally, contrary to previous beliefs, we find that the poor metallic oC88 structure is stabilized by the potential energy surface obtained via high-accuracy electronic structure calculations, rather than thermal or quantum effects.}, archive = {J_PRL}, author = {Qi Zhang and Xiaoyang Wang and Rong Shi and Xinguo Ren and Han Wang and Lei Wang}, doi = {10.1103/p3th-25bc}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246101}, shortjournal = {Phys. Rev. Lett.}, title = {Neural canonical transformations for quantum anharmonic solids of lithium}, volume = {134}, year = {2025}, }
• (2025). Phase diagram and crystal melting of helium-4 in two dimensions. PRL, 134(24), 246001. (www)

  @article{ , abstract = {We study the zero-temperature phase diagram of two-dimensional helium-4 using neural quantum states. Our variational description allows us to address liquid and solid phases using the same functional form as well as exploring possible melting scenarios—for instance, via an intermediate hexatic phase. Notably, this is achieved by performing fixed pressure variational Monte Carlo calculations. Within the isobaric ensemble framework, we are able to clearly identify the first-order liquid-solid phase transition. We additionally compute the Rényi-2 entanglement entropy across the liquid-solid phase transition and find a sharp decrease upon freezing. Calculations for larger systems follow the metastable liquid and solid branches in the transient region, while signatures of a hexatic order coexisting with a small condensate fraction are observed only for smaller systems as a finite-size effect.}, archive = {J_PRL}, author = {David Linteau and Gabriel Pescia and Jannes Nys and Giuseppe Carleo and Markus Holzmann}, doi = {10.1103/v1g7-m9k4}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {246001}, shortjournal = {Phys. Rev. Lett.}, title = {Phase diagram and crystal melting of helium-4 in two dimensions}, volume = {134}, year = {2025}, }
• (2025). Image rotation in plasmas. PRL, 134(24), 245101. (www)

  @article{ , abstract = {Because of the speed of light compared to material motion, the dragging of light is difficult to observe under laboratory conditions. Here, we report on the first observation of image rotation, i.e., a dragging by the medium of the wave’s transverse structure, of Alfvén waves in plasmas. Exploiting the naturally slow group velocity of these waves, significant wave rotation is achieved for modest angular frequency. Control over the rotation of the wave’s structure is demonstrated through the plasma rotation imposed by biased electrodes. Remarkably, experimental results are well reproduced by light dragging theory derived for isotropic media, even if magnetized plasmas are anisotropic. In addition to offering new insights into the fundamental issue of angular momentum coupling between waves and media, these findings also open possibilities for new remote rotation sensing tools.}, archive = {J_PRL}, author = {Renaud Gueroult and Shreekrishna Tripathi and Jia Han and Patrick Pribyl and Jean-Marcel Rax and Nathaniel J. Fisch}, doi = {10.1103/swrn-w3yf}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {245101}, shortjournal = {Phys. Rev. Lett.}, title = {Image rotation in plasmas}, volume = {134}, year = {2025}, }
• (2025). Acceleration of positive muons by a radio-frequency cavity. PRL, 134(24), 245001. (www)

  @article{ , abstract = {Acceleration of positive muons from thermal energy to 100 keV has been demonstrated. Thermal muons were generated by resonant multiphoton ionization of muonium atoms emitted from a sheet of laser-ablated aerogel. The thermal muons were first electrostatically accelerated to 5.7 keV, followed by further acceleration to 100 keV using a radio-frequency quadrupole with an intensity of 2 × 10 − 3 μ + / pulse . The transverse normalized rms emittance of the accelerated muons in the horizontal and vertical planes were 0.85 ± 0.25 ( s t a t ) − 0.13 + 0.22 ( syst ) π mm mrad and 0.32 ± 0.03 ( stat ) − 0.02 + 0.05 ( syst ) π mm mrad , respectively. The measured emittance values demonstrated phase-space reduction by a factor of 2.0 × 10 2 (horizontal) and 4.1 × 10 2 (vertical) allowing good acceleration efficiency. These results pave the way to realize the first-ever muon accelerator for a variety of applications in particle physics, material science, and other fields.}, archive = {J_PRL}, author = {S. Aritome and K. Futatsukawa and H. Hara and K. Hayasaka and Y. Ibaraki and T. Ichikawa and T. Iijima and H. Iinuma and Y. Ikedo and Y. Imai and K. Inami and K. Ishida and S. Kamal and S. Kamioka and N. Kawamura and M. Kimura and A. Koda and S. Koji and K. Kojima and A. Kondo and Y. Kondo and M. Kuzuba and R. Matsushita and T. Mibe and Y. Miyamoto and J. G. Nakamura and Y. Nakazawa and S. Ogawa and Y. Okazaki and A. Olin and M. Otani and S. Oyama and N. Saito and H. Sato and T. Sato and Y. Sato and K. Shimomura and Z. Shioya and P. Strasser and S. Sugiyama and K. Sumi and K. Suzuki and Y. Takeuchi and M. Tanida and J. Tojo and K. Ueda and S. Uetake and X. H. Xie and M. Yamada and S. Yamamoto and T. Yamazaki and K. Yamura and M. Yoshida and T. Yoshioka and M. Yotsuzuka}, doi = {10.1103/PhysRevLett.134.245001}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {245001}, shortjournal = {Phys. Rev. Lett.}, title = {Acceleration of positive muons by a radio-frequency cavity}, volume = {134}, year = {2025}, }
• (2025). Kolmogorov scaling in bubble-induced turbulence. PRL, 134(24), 244001. (www)

  @article{ , abstract = {Experiments using 3D Lagrangian tracking are used to investigate Kolmogorov scaling below the bubble size in bubble-induced turbulence (BIT). Second- and third-order structure functions reveal approximate Kolmogorov scaling for homogeneous bubble swarms. A new scaling for the kinetic energy dissipation rate is derived and shown to be in excellent agreement with the data. Using this we predict the scale separation below the bubble size as a function of the parameters and find that a large inertial range is not possible in BIT since bubbles of the required size would quickly break down.}, archive = {J_PRL}, author = {Tian Ma and Shiyong Tan and Rui Ni and Hendrik Hessenkemper and Andrew D. Bragg}, doi = {10.1103/v9mh-7pw1}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {244001}, shortjournal = {Phys. Rev. Lett.}, title = {Kolmogorov scaling in bubble-induced turbulence}, volume = {134}, year = {2025}, }
• (2025). Nonlinear non-hermitian skin effect and skin solitons in temporal photonic feedforward lattices. PRL, 134(24), 243805. (www)

  @article{ , abstract = {Here we report the experimental demonstration of the nonlinear non-Hermitian skin effect (NHSE) in an effective Kerr nonlinear temporal photonic lattice, where the high-power requirements and lack of tunability intrinsic to optical materials are overcome by an artificial nonlinearity arising from optoelectronic feedforward. Thanks to Kerr self-trapping, the nonlinear NHSE is demonstrated to possess much better localization strength and robustness at the preferred boundary compared to the linear case. Away from the preferred boundary, Kerr self-trapping can even inhibit NHSE-induced transport and form stable skin solitons. Harnessing the nonlinearity-controlled NHSE, we judiciously design an optical router with a flexibly tuned output port. Our findings promise great applications in robust signal transmission, routing, and processing.}, archive = {J_PRL}, author = {Shulin Wang and Bing Wang and Chenyu Liu and Chengzhi Qin and Lange Zhao and Weiwei Liu and Stefano Longhi and Peixiang Lu}, doi = {10.1103/PhysRevLett.134.243805}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243805}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear non-hermitian skin effect and skin solitons in temporal photonic feedforward lattices}, volume = {134}, year = {2025}, }
• (2025). Robust purcell effect of CsPbI3 quantum dots using nonlocal plasmonic metasurfaces. PRL, 134(24), 243804. (www)

  @article{ , abstract = {Optoelectronic metadevices control and enhance light-matter interactions by modulating the local optical field that interacts with emitters. However, the optical property of the highly localized mode in the plasmonic metasurface is sensitive to local disorders arising from experimental fluctuations. Recently, the nonlocal mode of metasurfaces has been attracting growing interest because the coupling within the array of plasmonics results in long-range ordering and collective resonances. Here we demonstrate the topological edge states and the nonlocal modes of Au bow ties in a photonic crystal (PHC) lattice. The strong coupling between plasmonic modes and PHC bands opens the topological band gap at the edge of the Brillouin zone and forms the nonlocal mode having a resonant energy insensitive to fluctuations in Au length, resulting in a robust Purcell effect for quantum dots (QDs) coupling with the nonlocal mode in metadevices. The topological band gap and robust enhancement indicate great potential for the nonlocal plasmonic metasurface in quantum photonic devices with novel functionalities.}, archive = {J_PRL}, author = {Yu Yuan and Chenjiang Qian and Longlong Yang and Xue-Chen Ru and Yaolong Li and Jingnan Yang and Bowen Fu and Sai Yan and Hancong Li and Zhanchun Zuo and Can Wang and Xiaoyong Hu and Hong-Bin Yao and Kuijuan Jin and Qihuang Gong and Xiulai Xu}, doi = {10.1103/gt4z-gwdw}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243804}, shortjournal = {Phys. Rev. Lett.}, title = {Robust purcell effect of CsPbI3 quantum dots using nonlocal plasmonic metasurfaces}, volume = {134}, year = {2025}, }
• (2025). Reservoir-engineered squeezed lasing through the parametric coupling. PRL, 134(24), 243803. (www)

  @article{ , abstract = {We report the first experimental demonstration of squeezed lasing in a reservoir-engineered optical parametric oscillator (OPO). The OPO provides a basis of squeezed states and parametric amplification in lasing emission, whose vacuum reservoir is coupled to a squeezed vacuum generated by a second OPO. With a precisely controlled squeezing angle and strong squeezing injection, the parametric interaction in the first OPO is exponentially enhanced. It successfully circumvents the decoherence in the system, and eliminates the undesired noise of spontaneous photon emission in the OPO. As a result, the amplified parametric process simultaneously reserves the coherence and quantum properties in the first OPO, and yields a − 6.1 dB squeezed laser in optical domain with a narrow linewidth and high brightness. Our work sheds light on potential applications of squeezed lasing in quantum metrology and quantum optics.}, archive = {J_PRL}, author = {Yuhang Tian and Yajun Wang and Weijie Wang and Xiaocong Sun and Yuhang Li and Shaoping Shi and Long Tian and Yaohui Zheng}, doi = {10.1103/3bdr-njhy}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243803}, shortjournal = {Phys. Rev. Lett.}, title = {Reservoir-engineered squeezed lasing through the parametric coupling}, volume = {134}, year = {2025}, }
• (2025). Ultrasensitive higher-order exceptional points via non-hermitian zero-index materials. PRL, 134(24), 243802. (www)

  @article{ , abstract = {Higher-order exceptional points (EPs) in optical structures enable ultrasensitive responses to perturbations. However, previous investigations on higher-order EPs have predominantly focused on coupled systems, leaving their fundamental physics in open scattering systems largely unexplored. Here, we harness wave interference to realize higher-order EPs in non-Hermitian zero-index materials connected to multiple open channels. Specifically, we show that a three-channel model can give rise to three interesting types of third-order EPs: lasing EP, reflecting EP, and absorbing EP. Notably, near the third-order absorbing EP, we show ultrasensitivity—a drastic change in output power in response to perturbations at the operating frequency—in a purely lossy system. These findings pave the way for achieving higher-order and even arbitrary-order EPs in open scattering systems, offering significant potential for advanced sensing applications.}, archive = {J_PRL}, author = {Dongyang Yan and Alexander S. Shalin and Yongxing Wang and Yun Lai and Yadong Xu and Zhi Hong Hang and Fang Cao and Lei Gao and Jie Luo}, doi = {10.1103/18gg-gvzc}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243802}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrasensitive higher-order exceptional points via non-hermitian zero-index materials}, volume = {134}, year = {2025}, }
• (2025). Nearfield vortex dynamics of supercell bloch modes. PRL, 134(24), 243801. (www)

  @article{ , abstract = {Densely arranged optical vortices are natural solutions of high-symmetry Bloch modes in photonic crystals. However, strict symmetry constraints limit the potential spatial configurations of nearfield vortices, restricting the control over light-matter interaction. Here, we demonstrate a nearfield vortex dynamic within a supercell photonic crystal. By introducing paired rotations of triangular structures, we achieve high-quality-factor Bloch mode transition from evanescent valley modes, to quasibound states in the continuum, frustrated modes, and quasivalleys. Each stage exhibits distinct nearfield vortex distributions, nonlinear overlap properties, and quality factors, revealing diverse physical behaviors for tailoring light-matter interaction. Notably, the asymmetric vortex configuration of frustrated modes enhances second harmonic generation, driven by an optimized nonlinear overlap factor. Our paired-rotation strategy offers a versatile design framework for creating supercell photonic crystals with unique nearfield vortex properties, presenting promising applications in lasing, nonlinear optics and optical forces.}, archive = {J_PRL}, author = {Xiaona Ye and Guangfeng Wang and Xiaoyang Duan and Ziwei Wang and Zengya Li and Tongtong Jia and Tingxin Li and Luqi Yuan and Bo Wang and Xianfeng Chen}, doi = {10.1103/svcj-vgzw}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243801}, shortjournal = {Phys. Rev. Lett.}, title = {Nearfield vortex dynamics of supercell bloch modes}, volume = {134}, year = {2025}, }
• (2025). Time-resolved spectral diffusion of a multimode mechanical memory. PRL, 134(24), 243604. (www)

  @article{ , abstract = {High-frequency phonons hold great promise as carriers of quantum information on chip and as quantum memories. Because of their coherent interaction with several systems, their compact mode volume, and slow group velocity, multiple experiments have recently demonstrated coherent transport of information on chip using phonon modes, interconnecting distinct quantum devices. Strongly confined phonons in waveguidelike geometries are particularly interesting because of their long lifetime. However, spectral diffusion has been observed to substantially limit their coherence times [S. M. Meenehan et al. , Silicon optomechanical crystal resonator at millikelvin temperatures, Phys. Rev. A 90 , 011803(R) (2014) , A. Wallucks et al. , A quantum memory at telecom wavelengths, Nat. Phys. 16 , 772 (2020) , and G. S. MacCabe et al. , Nano-acoustic resonator with ultralong phonon lifetime, Science 370 , 840 (2020) ]. Coupling to two-level systems is suspected to be a major contributor to the diffusion; however, to date, the origin and underlying mechanisms are still not fully understood. Here, we perform a time-domain study on two adjacent mechanical modes (separated by around 5 MHz) and show that the frequency positions of the two modes are not correlated in time, in agreement with our theoretical model and Monte Carlo simulations. This result is an important step in fully understanding the microscopic mechanisms of dephasing in mechanical quantum buses and memories.}, archive = {J_PRL}, author = {Niccolò Fiaschi and Lorenzo Scarpelli and Alexander Rolf Korsch and Amirparsa Zivari and Simon Gröblacher}, doi = {10.1103/tcpy-jhjy}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243604}, shortjournal = {Phys. Rev. Lett.}, title = {Time-resolved spectral diffusion of a multimode mechanical memory}, volume = {134}, year = {2025}, }
• (2025). Squeezing at the normal-mode splitting frequency of a nonlinear coupled cavity. PRL, 134(24), 243603. (www)

  @article{ , abstract = {Coupled optical cavities, which support normal modes, play a critical role in optical filtering, sensing, slow-light generation, and quantum state manipulation. Recent theoretical work has proposed incorporating nonlinear materials into these systems to enable novel quantum technologies. Here, we report the first experimental demonstration of squeezing generated in a quantum-enhanced coupled-cavity system, achieving a quantum noise reduction of 3.3 dB around the normal-mode splitting frequency of 7.47 MHz. We provide a comprehensive analysis of the system’s loss mechanisms and performance limitations, validating theoretical predictions. Our results underscore the promise of coupled-cavity squeezers for advanced quantum applications, including gravitational wave detection and precision sensing.}, archive = {J_PRL}, author = {Jonas Junker and Jiayi Qin and Vaishali B. Adya and Nutsinee Kijbunchoo and Sheon S. Y. Chua and Terry G. McRae and Bram J. J. Slagmolen and David E. McClelland}, doi = {10.1103/PhysRevLett.134.243603}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243603}, shortjournal = {Phys. Rev. Lett.}, title = {Squeezing at the normal-mode splitting frequency of a nonlinear coupled cavity}, volume = {134}, year = {2025}, }
• (2025). Hybrid sub- and superradiant states in emitter arrays with quantized motion. PRL, 134(24), 243602. (www)

  @article{ , abstract = {Ensembles of dipolar emitters which couple collectively to the radiation field display sub- and superradiance. These terms refer to a reduction or an enhancement of photon emission rates due to the interference of emission channels. Arrays of trapped neutral atoms constitute a promising platform for harnessing this phenomenon in technological applications, e.g., for excitation storage, single-photon switches, and mirrors. However, quantum and thermally induced vibrations of the atoms within their traps lead to position fluctuations that entangle the motion and the internal atomic degrees of freedom. We develop here a theory for collective atom-light coupling in the presence of this quantized motion within the Lamb-Dicke limit. We show the existence of sub- and superradiant states that are hybrids of electronic and vibrational excitations, investigate their properties for analytically and numerically efficiently solvable cases, and discuss how a finite temperature affects the collective photon emission.}, archive = {J_PRL}, author = {Beatriz Olmos and Igor Lesanovsky}, doi = {10.1103/q2kj-w3lf}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243602}, shortjournal = {Phys. Rev. Lett.}, title = {Hybrid sub- and superradiant states in emitter arrays with quantized motion}, volume = {134}, year = {2025}, }
• (2025). Measurement uncertainty in infrared spectroscopy with entangled photon pairs. PRL, 134(24), 243601. (www)

  @article{ , abstract = {Spectroscopy with entanglement has shown great potential to break limitations of traditional spectroscopic measurements, yet the role of entanglement in spectroscopic multiparameter joint measurement, particularly in the infrared optical range, remains elusive. Here, we find an uncertain relation that constrains the precision of infrared spectroscopic multiparameter measurements using entangled photon pairs. Under such a relation, we demonstrate a trade-off between the measurement precisions of the refractive index and the absorption coefficient of the medium in the infrared range, and also illustrate how to balance their respective estimation errors. Our work shall provide guidance toward future experimental designs and applications in entanglement-assisted spectroscopy.}, archive = {J_PRL}, author = {Xue Zhang and Zhucheng Zhang and Hui Dong}, doi = {10.1103/z44z-lnwx}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243601}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement uncertainty in infrared spectroscopy with entangled photon pairs}, volume = {134}, year = {2025}, }
• (2025). Confinement-induced resonances in spherical shell traps. PRL, 134(24), 243401. (www)

  @article{ , abstract = {The energy spectrum and corresponding wave functions of two bosonic particles confined in a spherically symmetric shell trap and interacting via a three-dimensional zero-range potential are computed. Confinement-induced resonances, originating entirely from the strong coupling of the relative and center-of-mass motions of the two particles, are identified as avoided crossings for certain values of the shell radius. By working close to the found resonances, these results offer a new way to control the atom-atom interaction in an atomic gas by tuning only the geometrical parameters of the shell.}, archive = {J_PRL}, author = {C. Moritz Carmesin and Maxim A. Efremov}, doi = {10.1103/hfyx-r11q}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243401}, shortjournal = {Phys. Rev. Lett.}, title = {Confinement-induced resonances in spherical shell traps}, volume = {134}, year = {2025}, }
• (2025). Few-electron highly charged muonic ar atoms verified by electronic k x rays. PRL, 134(24), 243001. (www)

  @article{ , abstract = {A highly charged muonic ion is a unique few-body atomic system where a negatively charged muon and a few electrons are simultaneously bound to a single nucleus. We report the first state-selective observation of highly charged muonic Ar ( μ Ar ) by electronic K x-ray spectroscopy using an array of transition-edge sensor microcalorimeters. The high-precision K x-ray spectra provide a clear signature of the presence of muonic atoms with one, two, and three electrons, i.e., H-like, He-like, and Li-like μ Ar . With the aid of theoretical calculations, we confirmed that the peak positions are consistent with the x-ray energies from highly charged Cl ions, and the intensities reflect deexcitation dynamics of highly charged μ Ar .}, archive = {J_PRL}, author = {T. Okumura and T. Azuma and D. A. Bennett and W. B. Doriese and M. S. Durkin and J. W. Fowler and J. D. Gard and T. Hashimoto and R. Hayakawa and Y. Ichinohe and P. Indelicato and T. Isobe and S. Kanda and D. Kato and M. Katsuragawa and N. Kawamura and Y. Kino and N. Kominato and Y. Miyake and K. M. Morgan and H. Noda and G. C. O’Neil and S. Okada and K. Okutsu and N. Paul and C. D. Reintsema and T. Sato and D. R. Schmidt and K. Shimomura and P. Strasser and D. S. Swetz and T. Takahashi and S. Takeda and S. Takeshita and M. Tampo and H. Tatsuno and K. Tőkési and X. M. Tong and Y. Toyama and J. N. Ullom and S. Watanabe and S. Yamada and T. Yamashita}, doi = {10.1103/PhysRevLett.134.243001}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {243001}, shortjournal = {Phys. Rev. Lett.}, title = {Few-electron highly charged muonic ar atoms verified by electronic k x rays}, volume = {134}, year = {2025}, }
• (2025). Next-to-leading-order prediction for the neutrinoless double-beta decay. PRL, 134(24), 242502. (www)

  @article{ , abstract = {The neutrinoless double-beta decay ( 0 ν β β ) of two neutrons n n → p p e e is the elementary subprocess of 0 ν β β decay in nuclei. Accurate knowledge of the n n → p p e e amplitude is required to pin down the short-range contributions in the nuclear matrix elements of the candidate nuclei for large-scale 0 ν β β searches. In this Letter, we report the first next-to-leading-order prediction of the n n → p p e e amplitude, with Bayesian uncertainty quantification. This is made possible by the development of the relativistic chiral effective field theory, in which no unknown contact term is required up to next-to-leading order. The theory is validated by reproducing in a parameter-free way the available data on the charge independence and charge symmetry breaking contributions in the two-nucleon scattering. The present work makes an essential step toward addressing the uncertainty in the theoretical calculations of the nuclear matrix elements relevant for 0 ν β β searches.}, archive = {J_PRL}, author = {Y. L. Yang and P. W. Zhao}, doi = {10.1103/fjy4-wzzq}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {242502}, shortjournal = {Phys. Rev. Lett.}, title = {Next-to-leading-order prediction for the neutrinoless double-beta decay}, volume = {134}, year = {2025}, }
• (2025). Final results of the majorana demonstrator’s search for double-beta decay of ge76 to excited states of se76. PRL, 134(24), 242501. (www)

  @article{ , abstract = {can decay into three possible excited states of , with the emission of two or, if the neutrino is Majorana, zero neutrinos. None of these six transitions have yet been observed. The Majorana Demonstrator was designed to study decay of using a low background array of high purity germanium detectors. With 98.2 kg-y of isotopic exposure, the d emonstrator sets the strongest half-life limits to date for all six transition modes. For to the state of , this search has begun to probe for the first time half-life values predicted using modern many-body nuclear theory techniques, setting a limit of (90% CL).}, archive = {J_PRL}, author = {Majorana Collaboration and I. J. Arnquist and F. T. Avignone, III and A. S. Barabash and E. Blalock and B. Bos and M. Busch and Y.-D. Chan and J. R. Chapman and C. D. Christofferson and P.-H. Chu and C. Cuesta and J. A. Detwiler and Yu. Efremenko and H. Ejiri and S. R. Elliott and N. Fuad and G. K. Giovanetti and M. P. Green and J. Gruszko and I. S. Guinn and V. E. Guiseppe and C. R. Haufe and R. Henning and D. Hervas Aguilar and E. W. Hoppe and I. Kim and R. T. Kouzes and T. E. Lannen, V and A. Li and R. Massarczyk and S. J. Meijer and T. K. Oli and L. S. Paudel and W. Pettus and A. W. P. Poon and D. C. Radford and A. L. Reine and K. Rielage and D. C. Schaper and S. J. Schleich and D. Tedeschi and R. L. Varner and S. Vasilyev and S. L. Watkins and J. F. Wilkerson and C. Wiseman and C.-H. Yu and B. X. Zhu}, doi = {10.1103/PhysRevLett.134.242501}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {242501}, shortjournal = {Phys. Rev. Lett.}, title = {Final results of the majorana demonstrator’s search for double-beta decay of ge76 to excited states of se76}, volume = {134}, year = {2025}, }
• (2025). Thermal dilepton polarization and dynamics of the QCD plasma in relativistic heavy-ion collisions. PRL, 134(24), 242301. (www)

  @article{ , abstract = {We present the first theoretical study of the polarization of lepton pairs produced in s NN = 5.02 TeV Pb + Pb collisions at the LHC, using next-to-leading order (NLO) dilepton emission rates. These calculations employ a multistage framework to simulate the evolution of relativistic heavy-ion collisions, and to explore the sensitivity of polarization to early times. It is found that the intermediate invariant-mass dileptons are indeed probes of the thermal equilibration process, and go beyond the reach of hadronic observables. We compute the polarization anisotropy coefficient obtained with LO dilepton rates, and show that the LO and NLO results differ radically, both in trend and in magnitude, at low and intermediate lepton pair invariant masses.}, archive = {J_PRL}, author = {Xiang-Yu Wu and Han Gao and Bailey Forster and Charles Gale and Greg Jackson and Sangyong Jeon}, doi = {10.1103/c4jv-jxkn}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {242301}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal dilepton polarization and dynamics of the QCD plasma in relativistic heavy-ion collisions}, volume = {134}, year = {2025}, }
• (2025). Observation of charmonium hc radiative decays to multiple light hadrons and the tensor state f2(1270). PRL, 134(24), 241902. (www)

  @article{ , abstract = {Using decays from a data sample of events collected by the BESIII detector at the BEPCII collider, radiative decays to multiple light hadrons below — , and —are observed for the first time, each with a significance greater than . The corresponding branching fractions are measured. Furthermore, intermediate states are investigated, leading to the first observation of the decay process of with a significance of . This observation represents the first instance of radiative decay to a tensor state.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Y. Y. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and K. D. Hao and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and J. L. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and Ch. Rosner and M. Q. Ruan and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and H. L. Song and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and L. F. Tang and M. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and V. Thoren and J. Y. Tian and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Yuan Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. L. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/v4hf-s8x8}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241902}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of charmonium hc radiative decays to multiple light hadrons and the tensor state f2(1270)}, volume = {134}, year = {2025}, }
• (2025). Lanczos algorithm, the transfer matrix, and the signal-to-noise problem. PRL, 134(24), 241901. (www)

  @article{ , abstract = {This Letter introduces a method for determining the energy spectrum of lattice quantum chromodynamics by applying the Lanczos algorithm to the transfer matrix and using a bootstrap generalization of the Cullum-Willoughby method to filter out spurious eigenvalues. Proof-of-principle analyses of the simple harmonic oscillator and the lattice quantum chromodynamics proton mass demonstrate that this method provides faster ground-state convergence than the “effective mass,” which is related to the power-iteration algorithm. Lanczos provides more accurate energy estimates than multistate fits to correlation functions with small imaginary times while achieving comparable statistical precision. Two-sided error bounds are computed for Lanczos results and guarantee that excited-state effects cannot shift Lanczos results far outside their statistical uncertainties.}, archive = {J_PRL}, author = {Michael L. Wagman}, doi = {10.1103/pcvc-734h}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241901}, shortjournal = {Phys. Rev. Lett.}, title = {Lanczos algorithm, the transfer matrix, and the signal-to-noise problem}, volume = {134}, year = {2025}, }
• (2025). Cosmological selection of a small weak scale from large vacuum energy: A minimal approach. PRL, 134(24), 241803. (www)

  @article{ , abstract = {We present a minimal cosmological solution to the hierarchy problem. Our model consists of a light pseudoscalar and an extra Higgs doublet in addition to the standard model field content. We consider a landscape of vacua with varying values of the electroweak vacuum expectation value (VEV). The vacuum energy in our model peaks in a region of the landscape where the electroweak VEV is nonzero and much smaller than the cutoff. During inflation, due to exponential expansion, such regions of the landscape with maximal vacuum energy dominate the universe in volume, thus explaining the observed smallness of the electroweak scale with respect to the cutoff. The pseudoscalar potential in our model is that of a completely generic pseudogoldstone boson—not requiring the clockwork mechanism—and its field value never exceeds its decay constant or the Planck scale. Our mechanism is robust to the variation of other model parameters in the landscape as the electroweak VEV is varied. It also predicts a precise and falsifiable relationship between the masses and couplings of the different Higgs boson mass eigenstates. Moreover, the pseudoscalar in our model can account for the observed dark matter relic density.}, archive = {J_PRL}, author = {Susobhan Chattopadhyay and Dibya S. Chattopadhyay and Rick S. Gupta}, doi = {10.1103/x3fg-c5p2}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241803}, shortjournal = {Phys. Rev. Lett.}, title = {Cosmological selection of a small weak scale from large vacuum energy: A minimal approach}, volume = {134}, year = {2025}, }
• (2025). First constraint on atmospheric millicharged particles with the LUX-ZEPLIN experiment. PRL, 134(24), 241802. (www)

  @article{ , abstract = {We report on a search for millicharged particles (mCPs) produced in cosmic ray atmospheric interactions using data collected during the first science run of the LUX-ZEPLIN experiment. The mCPs produced by two processes—meson decay and proton bremsstrahlung—are considered in this study. This search utilized a novel signature unique to liquid xenon (LXe) time projection chambers, allowing sensitivity to mCPs with masses ranging from 10 to and fractional charges between 0.001 and 0.02 of the electron charge ( ). With an exposure of 60 live days and a 5.5 metric ton fiducial mass, we observed no significant excess over background. This represents the first experimental search for atmospheric mCPs and the first search for mCPs using an underground LXe experiment.}, archive = {J_PRL}, author = {The LZ Collaboration and J. Aalbers and D. S. Akerib and A. K. Al Musalhi and F. Alder and C. S. Amarasinghe and A. Ames and T. J. Anderson and N. Angelides and H. M. Araújo and J. E. Armstrong and M. Arthurs and A. Baker and S. Balashov and J. Bang and J. W. Bargemann and E. E. Barillier and D. Bauer and K. Beattie and T. Benson and A. Bhatti and A. Biekert and T. P. Biesiadzinski and H. J. Birch and E. Bishop and G. M. Blockinger and B. Boxer and C. A. J. Brew and P. Brás and S. Burdin and M. Buuck and M. C. Carmona-Benitez and M. Carter and A. Chawla and H. Chen and J. J. Cherwinka and Y. T. Chin and N. I. Chott and M. V. Converse and R. Coronel and A. Cottle and G. Cox and D. Curran and C. E. Dahl and I. Darlington and S. Dave and A. David and J. Delgaudio and S. Dey and L. de Viveiros and L. Di Felice and C. Ding and J. E. Y. Dobson and E. Druszkiewicz and S. Dubey and S. R. Eriksen and A. Fan and S. Fayer and N. M. Fearon and N. Fieldhouse and S. Fiorucci and H. Flaecher and E. D. Fraser and T. M. A. Fruth and R. J. Gaitskell and A. Geffre and J. Genovesi and C. Ghag and A. Ghosh and R. Gibbons and S. Gokhale and J. Green and M. G. D. van der Grinten and J. J. Haiston and C. R. Hall and T. J. Hall and S. Han and E. Hartigan-O’Connor and S. J. Haselschwardt and M. A. Hernandez and S. A. Hertel and G. Heuermann and G. J. Homenides and M. Horn and D. Q. Huang and D. Hunt and E. Jacquet and R. S. James and J. Johnson and A. C. Kaboth and A. C. Kamaha and M. Kannichankandy and D. Khaitan and A. Khazov and I. Khurana and J. Kim and Y. D. Kim and J. Kingston and R. Kirk and D. Kodroff and L. Korley and E. V. Korolkova and H. Kraus and S. Kravitz and L. Kreczko and V. A. Kudryavtsev and C. Lawes and D. S. Leonard and K. T. Lesko and C. Levy and J. Lin and A. Lindote and W. H. Lippincott and M. I. Lopes and W. Lorenzon and C. Lu and S. Luitz and P. A. Majewski and A. Manalaysay and R. L. Mannino and C. Maupin and M. E. McCarthy and G. McDowell and D. N. McKinsey and J. McLaughlin and J. B. McLaughlin and R. McMonigle and E. Mizrachi and A. Monte and M. E. Monzani and J. D. Morales Mendoza and E. Morrison and B. J. Mount and M. Murdy and A. St. J. Murphy and A. Naylor and H. N. Nelson and F. Neves and A. Nguyen and C. L. O’Brien and I. Olcina and K. C. Oliver-Mallory and J. Orpwood and K. Y Oyulmaz and K. J. Palladino and J. Palmer and N. J. Pannifer and N. Parveen and S. J. Patton and B. Penning and G. Pereira and E. Perry and T. Pershing and A. Piepke and Y. Qie and J. Reichenbacher and C. A. Rhyne and A. Richards and Q. Riffard and G. R. C. Rischbieter and E. Ritchey and H. S. Riyat and R. Rosero and T. Rushton and D. Rynders and D. Santone and A. B. M. R. Sazzad and R. W. Schnee and G. Sehr and B. Shafer and S. Shaw and T. Shutt and J. J. Silk and C. Silva and G. Sinev and J. Siniscalco and R. Smith and V. N. Solovov and P. Sorensen and J. Soria and I. Stancu and A. Stevens and K. Stifter and B. Suerfu and T. J. Sumner and M. Szydagis and D. R. Tiedt and M. Timalsina and Z. Tong and D. R. Tovey and J. Tranter and M. Trask and M. Tripathi and A. Usón and A. Vacheret and A. C. Vaitkus and O. Valentino and V. Velan and A. Wang and J. J. Wang and Y. Wang and J. R. Watson and L. Weeldreyer and T. J. Whitis and K. Wild and M. Williams and W. J. Wisniewski and L. Wolf and F. L. H. Wolfs and S. Woodford and D. Woodward and C. J. Wright and Q. Xia and J. Xu and Y. Xu and M. Yeh and D. Yeum and W. Zha and H. Zhang and E. A. Zweig}, doi = {10.1103/zhs9-65ds}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241802}, shortjournal = {Phys. Rev. Lett.}, title = {First constraint on atmospheric millicharged particles with the LUX-ZEPLIN experiment}, volume = {134}, year = {2025}, }
• (2025). New constraints on cosmic ray-boosted dark matter from the LUX-ZEPLIN experiment. PRL, 134(24), 241801. (www)

  @article{ , abstract = {While dual-phase xenon time projection chambers have driven the sensitivity toward weakly interacting massive particles at the to mass scale, the scope for sub- dark matter particles is hindered by a limited nuclear recoil energy detection threshold. One approach to probe for lighter candidates is to consider cases where they have been boosted by collisions with cosmic rays in the Milky Way, such that the additional kinetic energy lifts their induced signatures above the nominal threshold. In this Letter, we report first results of a search for cosmic ray-boosted dark matter (CRDM) with a combined exposure from the LUX-ZEPLIN experiment. We observe no excess above the expected backgrounds and establish world-leading constraints on the spin-independent CRDM-nucleon cross section as small as at 90% confidence level for sub- masses.}, archive = {J_PRL}, author = {LZ Collaboration and J. Aalbers and D. S. Akerib and A. K. Al Musalhi and F. Alder and C. S. Amarasinghe and A. Ames and T. J. Anderson and N. Angelides and H. M. Araújo and J. E. Armstrong and M. Arthurs and A. Baker and S. Balashov and J. Bang and J. W. Bargemann and E. E. Barillier and K. Beattie and T. Benson and A. Bhatti and A. Biekert and T. P. Biesiadzinski and H. J. Birch and E. Bishop and G. M. Blockinger and B. Boxer and C. A. J. Brew and P. Brás and S. Burdin and M. Buuck and M. C. Carmona-Benitez and M. Carter and A. Chawla and H. Chen and J. J. Cherwinka and Y. T. Chin and N. I. Chott and M. V. Converse and R. Coronel and A. Cottle and G. Cox and D. Curran and C. E. Dahl and I. Darlington and S. Dave and A. David and J. Delgaudio and S. Dey and L. de Viveiros and L. Di Felice and C. Ding and J. E. Y. Dobson and E. Druszkiewicz and S. Dubey and S. R. Eriksen and A. Fan and N. M. Fearon and N. Fieldhouse and S. Fiorucci and H. Flaecher and E. D. Fraser and T. M. A. Fruth and R. J. Gaitskell and A. Geffre and J. Genovesi and C. Ghag and R. Gibbons and S. Gokhale and J. Green and M. G. D. van der Grinten and J. J. Haiston and C. R. Hall and T. Hall and S. Han and E. Hartigan-O’Connor and S. J. Haselschwardt and M. A. Hernandez and S. A. Hertel and G. Heuermann and G. J. Homenides and M. Horn and D. Q. Huang and D. Hunt and E. Jacquet and R. S. James and M. K. Kannichankandy and A. C. Kaboth and A. C. Kamaha and D. Khaitan and A. Khazov and J. Kim and Y. D. Kim and J. Kingston and R. Kirk and D. Kodroff and L. Korley and E. V. Korolkova and H. Kraus and S. Kravitz and L. Kreczko and V. A. Kudryavtsev and C. Lawes and D. S. Leonard and K. T. Lesko and C. Levy and J. Lin and A. Lindote and W. H. Lippincott and M. I. Lopes and W. Lorenzon and C. Lu and S. Luitz and P. A. Majewski and A. Manalaysay and R. L. Mannino and C. Maupin and M. E. McCarthy and G. McDowell and D. N. McKinsey and J. McLaughlin and J. B. McLaughlin and R. McMonigle and E. Mizrachi and M. E. Monzani and E. Morrison and B. J. Mount and M. Murdy and A. St. J. Murphy and H. N. Nelson and F. Neves and A. Nguyen and C. L. O’Brien and I. Olcina and K. C. Oliver-Mallory and J. Orpwood and K. Y. Oyulmaz and K. J. Palladino and J. Palmer and N. J. Pannifer and N. Parveen and S. J. Patton and B. Penning and G. Pereira and E. Perry and T. Pershing and A. Piepke and Y. Qie and J. Reichenbacher and C. A. Rhyne and G. R. C. Rischbieter and E. Ritchey and H. S. Riyat and R. Rosero and T. Rushton and D. Rynders and D. Santone and A. B. M. R. Sazzad and R. W. Schnee and G. Sehr and B. Shafer and S. Shaw and K. Shi and T. Shutt and J. J. Silk and C. Silva and J. Siniscalco and R. Smith and V. N. Solovov and P. Sorensen and J. Soria and I. Stancu and A. Stevens and K. Stifter and B. Suerfu and T. J. Sumner and A. Swain and M. Szydagis and D. R. Tiedt and M. Timalsina and Z. Tong and D. R. Tovey and J. Tranter and M. Trask and M. Tripathi and A. Usón and A. C. Vaitkus and O. Valentino and V. Velan and A. Wang and J. J. Wang and Y. Wang and J. R. Watson and L. Weeldreyer and T. J. Whitis and K. Wild and M. Williams and W. J. Wisniewski and L. Wolf and F. L. H. Wolfs and S. Woodford and D. Woodward and C. J. Wright and Q. Xia and J. Xu and Y. Xu and M. Yeh and D. Yeum and W. Zha and H. Zhang}, doi = {10.1103/nr92-jvt3}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241801}, shortjournal = {Phys. Rev. Lett.}, title = {New constraints on cosmic ray-boosted dark matter from the LUX-ZEPLIN experiment}, volume = {134}, year = {2025}, }
• (2025). Bound states of the schwarzschild black hole. PRL, 134(24), 241401. (www)

  @article{ , abstract = {Understanding the physical significance and spectral stability of black hole quasinormal modes is fundamental to high-precision spectroscopy with future gravitational wave detectors. Inspired by Mashhoon’s idea of relating quasinormal modes of black holes with their equivalent bound states in an inverted potential, we investigate, for the first time, energy levels and eigenfunctions of the Schwarzschild black hole quantitatively. While quasinormal modes describe the characteristic damped oscillations of a black hole, the bound states of the inverted potential are qualitatively more similar to those of the hydrogen atom. Although the physical interpretation of these states may initially be of more academic interest, it furthers our understanding of open problems related to quasinormal modes in a similar spirit to Maggiore’s interpretation of the Schwarzschild quasinormal mode spectrum. One surprising insight from the explicit calculation of bound states is that eigenfunctions corresponding to quasinormal mode overtones become rapidly delocalized and extremely loosely bound. This observation raises immediate questions about the common interpretation of quasinormal modes as excitations of the light ring region. Closely related, as a second application, we also explore the spectral stability of bound states and demonstrate that they can provide complementary insights into the quasinormal mode spectrum.}, archive = {J_PRL}, author = {Sebastian H. Völkel}, doi = {10.1103/tbm2-gzv9}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241401}, shortjournal = {Phys. Rev. Lett.}, title = {Bound states of the schwarzschild black hole}, volume = {134}, year = {2025}, }
• (2025). Axion mass prediction from adaptive mesh refinement cosmological lattice simulations. PRL, 134(24), 241003. (www)

  @article{ , abstract = {The quantum chromodynamics (QCD) axion arises as the pseudo-Goldstone mode of a spontaneously broken Abelian Peccei-Quinn (PQ) symmetry. If the scale of PQ symmetry breaking occurs below the inflationary reheat temperature and the domain wall number is unity, then there is a unique axion mass that gives the observed dark matter (DM) abundance. Computing this mass has been the subject of intensive numerical simulations for decades since the mass prediction informs laboratory experiments. Axion strings develop below the PQ symmetry-breaking temperature, and as the string network evolves, it emits axions that go on to become the DM. A key ingredient in the axion mass prediction is the spectral index of axion radiation emitted by the axion strings. We compute this index in this Letter using the most precise and accurate large-scale simulations to date of the axion-string network leveraging adaptive mesh refinement to achieve the precision that would, otherwise, require a static lattice with 262, lattice sites. We find a scale-invariant axion radiation spectrum to within 1% precision and find no evidence that the spectral index of radiation evolves with time. Accounting for axion production from strings prior to the QCD phase transition leads us to predict that the axion mass should be approximately . However, we provide preliminary evidence that axions are produced in greater quantities from the string-domain-wall network collapse during the QCD phase transition, potentially increasing the mass prediction to as much as .}, archive = {J_PRL}, author = {Joshua N. Benabou and Malte Buschmann and Joshua W. Foster and Benjamin R. Safdi}, doi = {10.1103/6v21-d6sj}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241003}, shortjournal = {Phys. Rev. Lett.}, title = {Axion mass prediction from adaptive mesh refinement cosmological lattice simulations}, volume = {134}, year = {2025}, }
• (2025). Nonconservation of lepton numbers in the neutrino sector could change the prospects for core collapse supernova explosions. PRL, 134(24), 241002. (www)

  @article{ , abstract = {We show that interactions violating the conservation of lepton numbers in the neutrino sector could significantly alter the standard low entropy picture for the presupernova collapsing core of a massive star. A rapid neutrino-antineutrino equilibration leads to entropy generation and enhanced electron capture and, hence, a lower electron fraction than in the standard model. This would affect the downstream core evolution, the prospects for a supernova explosion, and the emergent neutrino signal. If realized by lepton-number-violating neutrino self-interactions (LNV ν SI ), the relevant mediator mass and coupling ranges can be probed by future accelerator-based experiments.}, archive = {J_PRL}, author = {Anna M. Suliga and Patrick Chi-Kit Cheong (張志杰 and Julien Froustey and George M. Fuller and Lukáš Gráf and Kyle Kehrer and Oliver Scholer and Shashank Shalgar}, doi = {10.1103/gnp5-4y8k}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241002}, shortjournal = {Phys. Rev. Lett.}, title = {Nonconservation of lepton numbers in the neutrino sector could change the prospects for core collapse supernova explosions}, volume = {134}, year = {2025}, }
• (2025). Searching for axionlike particles with X-ray observations of alpha centauri. PRL, 134(24), 241001. (www)

  @article{ , abstract = {We investigate the production of axionlike particles (ALPs) in stellar cores, where they interact with electromagnetic fields and electrons, with typical masses between and . These low-energy ALPs are gravitationally trapped in the orbits of stars and subsequently decay into two photons that we detect as monochromatic x-ray lines. We propose to search for these gravitationally trapped ALPs in the Alpha Centauri binary system, our closest stellar neighbor, using sensitive x-ray detectors like Chandra and eROSITA. Our search for ALP decay signals in the energy range of 0.2 keV to 10 keV yielded null results, thus establishing the most stringent limits on ALP interactions to date. In the case of ALP-electron coupling , we have improved the limits on the ALP-photon coupling in ALP mass range between 0.25 keV and 5 keV, compared to previous measurements, including those from GW170817, SN 2023ixf, and other sources, and specially the improvement reaches about 2 orders of magnitude at the mass of 2 keV. Even tighter constraints are set for larger .}, archive = {J_PRL}, author = {Yu-Xuan Chen and Lei Lei and Zi-Qing Xia and Ziwei Wang and Yue-Lin Sming Tsai and Yi-Zhong Fan}, doi = {10.1103/wy1x-1lh7}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {241001}, shortjournal = {Phys. Rev. Lett.}, title = {Searching for axionlike particles with X-ray observations of alpha centauri}, volume = {134}, year = {2025}, }
• (2025). Deterministic generation of frequency-bin-encoded microwave photons. PRL, 134(24), 240803. (www)

  @article{ , abstract = {A distributed quantum computing network requires a quantum communication channel between spatially separated processing units. In superconducting circuits, such a channel can be implemented based on propagating microwave photons to encode and transfer quantum information between an emitter and a receiver. However, traveling microwave photons can be lost during the transmission, leading to the failure of information transfer. Heralding protocols can be used to detect such photon losses. In this Letter, we propose such a protocol and experimentally demonstrate a frequency-bin encoding method of microwave photonic modes using superconducting circuits. We deterministically encode the quantum information from a superconducting qubit by simultaneously emitting its information into two photonic modes at different frequencies, with a process fidelity of 94.9%. The frequency-bin-encoded photonic modes can be used, at the receiver processor, to detect the occurrence of photon loss. Our Letter thus provides a reliable method to implement high-fidelity quantum state transfer in a distributed quantum computing network, incorporating error detection to enhance performance and accuracy.}, archive = {J_PRL}, author = {Jiaying Yang and Maryam Khanahmadi and Ingrid Strandberg and Akshay Gaikwad and Claudia Castillo-Moreno and Anton Frisk Kockum and Muhammad Asad Ullah and Göran Johansson and Axel Martin Eriksson and Simone Gasparinetti}, doi = {10.1103/PhysRevLett.134.240803}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240803}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic generation of frequency-bin-encoded microwave photons}, volume = {134}, year = {2025}, }
• (2025). Ultrafast high-fidelity state readout of single neutral atom. PRL, 134(24), 240802. (www)

  @article{ , abstract = {The capability to measure the state of a neutral atom is vital to an atom-based quantum network, for applications including distributed quantum computing and long-distance quantum communication. However, single neutral atoms suffer from low achievable photon scattering rate and shallow trapping potential, which limits the fidelity and speed of state readout process. Here, by coupling a single neutral atom with a high-finesse fiber-based Fabry-Pérot microcavity in the Purcell regime, we realize strong enhancement of the atomic photoemission rate and high overall system efficiency, which enables ultrafast and high-fidelity discrimination of bright and dark hyperfine states of the atom. The readout fidelity can reach 99.1(2)% within 200 ns and 99.985(8)% within 9 μ s . Furthermore, we demonstrate that state preparation via optical pumping can be efficiently accelerated by a real-time decision protocol based on ultrafast state readout. This work demonstrates the potential to serve as a high-performance atom-photon interface and paves the way to the implementation of a practical atom-based quantum network.}, archive = {J_PRL}, author = {Jian Wang and Dong-Yu Huang and Xiao-Long Zhou and Ze-Min Shen and Si-Jian He and Qi-Yang Huang and Yi-Jia Liu and Chuan-Feng Li and Guang-Can Guo}, doi = {10.1103/PhysRevLett.134.240802}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240802}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrafast high-fidelity state readout of single neutral atom}, volume = {134}, year = {2025}, }
• (2025). Entangled states from sparsely coupled spins for metrology with neutral atoms. PRL, 134(24), 240801. (www)

  @article{ , abstract = {Quantum states featuring extensive multipartite entanglement are a resource for quantum-enhanced metrology, with sensitivity up to the Heisenberg limit. However, robust generation of these states using unitary dynamics typically requires all-to-all interactions among particles. Here, we demonstrate that optimal states for quantum sensing can be generated with sparse interaction graphs featuring only a logarithmic number of couplings per particle. We show that specific sparse graphs with long-range interactions can approximate the dynamics of all-to-all spin models, such as the one-axis twisting model, even for large system sizes. The resulting sparse coupling graphs and protocol can also be efficiently implemented using dynamic reconfiguration of atoms in optical tweezers.}, archive = {J_PRL}, author = {Sridevi Kuriyattil and Pablo M. Poggi and Jonathan D. Pritchard and Johannes Kombe and Andrew J. Daley}, doi = {10.1103/h6sr-yxgw}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240801}, shortjournal = {Phys. Rev. Lett.}, title = {Entangled states from sparsely coupled spins for metrology with neutral atoms}, volume = {134}, year = {2025}, }
• (2025). Classification of qubit cellular automata on hypercubic lattices. PRL, 134(24), 240601. (www)

  @article{ , abstract = {We classify quantum cellular automata whose cells are qubits, on hypercubic lattices Z s , with the von Neumann neighborhood scheme, in terms of realizability as finite-depth quantum circuits. We show the most general structure of such automata and use its characterisation to simulate a few steps of evolution and evaluate the rate of entanglement production between one cell and its surroundings.}, archive = {J_PRL}, author = {Andrea Pizzamiglio and Alessandro Bisio and Paolo Perinotti}, doi = {10.1103/PhysRevLett.134.240601}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240601}, shortjournal = {Phys. Rev. Lett.}, title = {Classification of qubit cellular automata on hypercubic lattices}, volume = {134}, year = {2025}, }
• (2025). Self-similar phase diagram of the fibonacci-driven quantum ising model. PRL, 134(24), 240404. (www)

  @article{ , abstract = {We study a stroboscopic quantum Ising model with Fibonacci dynamics. We use its boundary spin correlation functions in long but finite chains to identify regions in the phase diagram which exhibit Majorana zero modes (MZM) as well as Majorana golden-ratio modes (MGM). We find that these regions evolve in a self-similar manner with increasing simulation time and identify the self-similarity transform which governs this evolution of the phase diagram. Integrability-breaking perturbations lead to a temporal decay of the boundary spin correlations, ultimately limiting the self-similarity of the phase diagram. Our predictions are testable with current quantum information processors.}, archive = {J_PRL}, author = {Harald Schmid and Yang Peng and Gil Refael and Felix von Oppen}, doi = {10.1103/hn66-j8pt}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240404}, shortjournal = {Phys. Rev. Lett.}, title = {Self-similar phase diagram of the fibonacci-driven quantum ising model}, volume = {134}, year = {2025}, }
• (2025). Genuine quantum advantage in anharmonic bosonic quantum batteries. PRL, 134(24), 240403. (www)

  @article{ , abstract = {Finding a quantum battery model that displays a genuine quantum advantage, while being prone to experimental fabrication, is an extremely challenging task. In this Letter we propose a deceptively simple quantum battery model that displays a genuine quantum advantage, saturating the quantum speed limit. It consists of two harmonic oscillators (the charger and the battery), coupled during the charging dynamics by an anharmonic interaction. We first present the model, then certify the genuine quantum advantage, and finally briefly discuss how the battery can be fabricated through the use of superconducting circuits.}, archive = {J_PRL}, author = {Gian Marcello Andolina and Vittoria Stanzione and Vittorio Giovannetti and Marco Polini}, doi = {10.1103/kzvn-dj7v}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240403}, shortjournal = {Phys. Rev. Lett.}, title = {Genuine quantum advantage in anharmonic bosonic quantum batteries}, volume = {134}, year = {2025}, }
• (2025). Roughening dynamics of interfaces in the two-dimensional quantum ising model. PRL, 134(24), 240402. (www)

  @article{ , abstract = {The properties of interfaces are key to understanding the physics of matter. However, the study of quantum interface dynamics has remained an outstanding challenge. Here, we use large-scale tree tensor network simulations to identify the dynamical signature of an interface roughening transition within the ferromagnetic phase of the 2D quantum Ising model. For initial domain wall profiles we find extended prethermal plateaus for smooth interfaces, whereas above the roughening transition the domain wall decays quickly. Our results can be readily explored experimentally in Rydberg atomic systems.}, archive = {J_PRL}, author = {Wladislaw Krinitsin and Niklas Tausendpfund and Matteo Rizzi and Markus Heyl and Markus Schmitt}, doi = {10.1103/9bsk-x9rw}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240402}, shortjournal = {Phys. Rev. Lett.}, title = {Roughening dynamics of interfaces in the two-dimensional quantum ising model}, volume = {134}, year = {2025}, }
• (2025). Topology and spectrum in measurement-induced phase transitions. PRL, 134(24), 240401. (www)

  @article{ , abstract = {Competition among repetitive measurements of noncommuting observables and unitary dynamics can give rise to a wide variety of entanglement phases. Here, we propose a general framework based on Lyapunov analysis to characterize topological properties in monitored quantum systems through their spectrum and many-body topological invariants. We illustrate this framework by analyzing ( )-dimensional monitored circuits for Majorana fermions, which are known to exhibit topological and trivial area-law entangled phases as well as a critical phase with sub-volume-law entanglement. Through the Lyapunov analysis, we identify the presence (absence) of edge-localized zero modes inside the bulk gap in the topological (trivial) phase and a bulk gapless spectrum in the critical phase. Furthermore, by suitably exploiting the fermion parity with twisted measurement outcomes at the boundary, we construct a topological invariant that distinguishes the two area-law phases and dynamically characterizes the critical phase. Our framework thus provides a general route to extend the notion of bulk-edge correspondence to monitored quantum dynamics.}, archive = {J_PRL}, author = {Hisanori Oshima and Ken Mochizuki and Ryusuke Hamazaki and Yohei Fuji}, doi = {10.1103/PhysRevLett.134.240401}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240401}, shortjournal = {Phys. Rev. Lett.}, title = {Topology and spectrum in measurement-induced phase transitions}, volume = {134}, year = {2025}, }
• (2025). Zero curvature condition for quantum criticality. PRL, 134(24), 240202. (www)

  @article{ , abstract = {Quantum criticality often lies beyond the scope of the conventional Landau paradigm, and a unifying framework has yet to emerge, due in part to the wide variety of quantum orders. We propose a geometric approach to quantum phase transitions that shifts focus from microscopic order to the competition between noncommuting operators. This competition is encoded in the boundary geometry of their expectation values, defining a quantum observable space. We show that quantum phase transitions occur at zero-curvature points on the quantum observable space boundary, signaling maximal commutativity and suggesting an underlying integrable structure at criticality.}, archive = {J_PRL}, author = {Chaoming Song}, doi = {10.1103/l3d5-lnr7}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240202}, shortjournal = {Phys. Rev. Lett.}, title = {Zero curvature condition for quantum criticality}, volume = {134}, year = {2025}, }
• (2025). Quantum-classical correspondence of non-hermitian symmetry breaking. PRL, 134(24), 240201. (www)

  @article{ , abstract = {Real-to-complex spectral transitions and the associated spontaneous symmetry breaking of eigenstates are central to non-Hermitian physics, yet a comprehensive and universal theory that precisely describes the underlying physical mechanisms for each individual state remains elusive. Here, we resolve the mystery by employing the complex path integral formalism and developing a generalized Gutzwiller trace formula. These methodologies enable us to establish a universal quantum-classical correspondence that precisely links the real or complex nature of individual energy levels to the symmetry properties of their corresponding semiclassical orbits. Specifically, in systems with a general -pseudo-Hermitian symmetry, real energy levels are quantized along periodic orbits that preserve the corresponding classical symmetry. In contrast, complex conjugate energy levels arise from semiclassical orbits that individually break the symmetry but together form -symmetric pairs. This framework provides a unified explanation for the spectral behaviors in various continuous non-Hermitian models and for the transition in two-level systems. Moreover, we demonstrate that the exceptional point is inherently a quantum phenomenon, as it cannot be described by a single classical orbit. Our Letter uncovers the physical mechanism of non-Hermitian symmetry breaking and introduces a new perspective with broad implications for the control and application of non-Hermitian phenomena.}, archive = {J_PRL}, author = {Zhuo-Ting Cai and Hai-Dong Li and Wei Chen}, doi = {10.1103/vvrx-mljg}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-classical correspondence of non-hermitian symmetry breaking}, volume = {134}, year = {2025}, }
• (2025). Essay: Emergent holographic spacetime from quantum information. PRL, 134(24), 240001. (www)

  @article{ , abstract = {Holographic duality describes gravitational theories in terms of quantum many-body systems. In holography, quantum information theory provides a crucial tool that directly connects microscopic structures of these systems to the geometries of gravitational spacetimes. One manifestation is that the entanglement entropy in quantum many-body systems can be calculated from the area of an extremal surface in the corresponding gravitational spacetime. This implies that a gravitational spacetime can emerge from an enormous number of entangled qubits. In this Essay, I will discuss open problems in this area of research, considering recent developments and outlining future prospects towards a complete understanding of quantum gravity. The first step in this direction is to understand what kind of quantum circuits each holographic spacetime corresponds to, drawing on recent developments in quantum complexity theories and studying concrete examples of holography in string theory. Next, we should extend the concept of holography to general spacetimes, e.g., those spacetimes which appear in realistic cosmologies, by utilizing the connections between quantum information and holography. To address the fundamental question of how time emerges, I will propose the concepts of pseudoentropy and timelike entanglement as a useful tool in our exploration.}, archive = {J_PRL}, author = {Tadashi Takayanagi}, doi = {10.1103/pg4r-fy8n}, journal = {Physical Review Letters}, month = {6}, number = {24}, pages = {240001}, shortjournal = {Phys. Rev. Lett.}, title = {Essay: Emergent holographic spacetime from quantum information}, volume = {134}, year = {2025}, }
• (2025). Nonlinear spontaneous flow instability in active nematics. PRL, 134(23), 238301. (www)

  @article{ , abstract = {Active nematics exhibit spontaneous flows through a well-known linear instability of the uniformly aligned quiescent state. Here, we show that even a linearly stable uniform state can experience a nonlinear instability, resulting in a discontinuous transition to spontaneous flows. In this case, quiescent and flowing states may coexist. Through a weakly nonlinear analysis and a numerical study, we trace the bifurcation diagram of striped patterns and show that the underlying pitchfork bifurcation switches from supercritical (continuous) to subcritical (discontinuous) by varying the flow-alignment parameter. We predict that the discontinuous spontaneous flow transition occurs for a wide range of parameters, including systems of contractile flow-aligning rods. Our predictions are relevant to active nematic turbulence and can potentially be tested in experiments on either cell layers or active cytoskeletal suspensions.}, archive = {J_PRL}, author = {Ido Lavi and Ricard Alert and Jean-François Joanny and Jaume Casademunt}, doi = {10.1103/PhysRevLett.134.238301}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {238301}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear spontaneous flow instability in active nematics}, volume = {134}, year = {2025}, }
• (2025). Fully independent response in disordered solids. PRL, 134(23), 238201. (www)

  @article{ , abstract = {Unlike in crystals, it is difficult to trace emergent material properties of amorphous solids to their underlying structure. Nevertheless, one can tune features of a disordered spring network, ranging from bulk elastic constants to specific allosteric responses, through highly precise alterations of the structure. This has been understood through the notion of independent bond-level response—the observation that, in many cases, different springs have different effects on different properties. While this idea has motivated inverse design in numerous contexts, it has not been formalized and quantified in a general context that not just informs but enables and predicts inverse design. Here, we show how to quantify independent response by linearizing the simultaneous change in multiple emergent features, and introduce the much stronger notion of fully independent response. Remarkably, we find that the mechanical properties of disordered solids are always fully independent across a wide array of scenarios, regardless of the target features, tunable parameters, system size, dimensionality, and class of interactions. Furthermore, our formulation quantifies the susceptibility of features to parameter changes, which is correlated with the maximum linear tunability. We also demonstrate the implications for multifeature inverse design beyond the linear regime. These results formalize our understanding of a key fundamental difference between ordered and disordered solids while also creating a practical tool to both understand and perform inverse design.}, archive = {J_PRL}, author = {Mengjie Zu and Aayush Desai and Carl P. Goodrich}, doi = {10.1103/PhysRevLett.134.238201}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {238201}, shortjournal = {Phys. Rev. Lett.}, title = {Fully independent response in disordered solids}, volume = {134}, year = {2025}, }
• (2025). Double splay nematic order in confined polar fluids. PRL, 134(23), 238101. (www)

  @article{ , abstract = {We report the structure of a modulated phase in the ferroelectric nematic material RM734 under cationic-polymer-coated planar confinement. This phase emerges continuously from the nematic phase upon cooling and transforms into the ferroelectric nematic phase via a first-order transition. Compelling optical evidence, including thickness-dependent periodicity, a sinusoidal variation of the orientation angle, and periodic variations in phase retardance and image intensity, demonstrates that this modulated phase is the theoretically predicted double splay nematic phase. In this phase, splay deformations alternate along two orthogonal directions oriented at 45° to the substrate surfaces, resulting in a maximum modulation wavelength twice the cell thickness. Our experiments with various ionic coatings reveal that only cationic polymer coatings effectively promote this phase configuration, highlighting the crucial role of electrical screening. These findings further provide insights into its distinctive topological defects within confined geometries.}, archive = {J_PRL}, author = {Zhongjie Ma and Miao Jiang and Aile Sun and Shengzhu Yi and Jidan Yang and Mingjun Huang and Satoshi Aya and Qi-Huo Wei}, doi = {10.1103/PhysRevLett.134.238101}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {238101}, shortjournal = {Phys. Rev. Lett.}, title = {Double splay nematic order in confined polar fluids}, volume = {134}, year = {2025}, }
• (2025). Random tree model of meaningful memory. PRL, 134(23), 237402. (www)

  @article{ , abstract = {Traditional studies of memory for meaningful narratives focus on specific stories and their semantic structures but do not address common quantitative features of recall across different narratives. We introduce a statistical ensemble of random trees to represent narratives as hierarchies of key points, where each node is a compressed representation of its descendant leaves, which are the original narrative segments. Recall from this hierarchical representation is constrained by working memory capacity. Our analytical solution aligns with observations from large-scale narrative recall experiments. Specifically, our model explains that (1) average recall length increases sublinearly with narrative length and (2) individuals summarize increasingly longer narrative segments in each recall sentence. Additionally, the theory predicts that for sufficiently long narratives, a universal, scale-invariant limit emerges, where the fraction of a narrative summarized by a single recall sentence follows a distribution independent of narrative length.}, archive = {J_PRL}, author = {Weishun Zhong and Tankut Can and Antonis Georgiou and Ilya Shnayderman and Mikhail Katkov and Misha Tsodyks}, doi = {10.1103/g1cz-wk1l}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {237402}, shortjournal = {Phys. Rev. Lett.}, title = {Random tree model of meaningful memory}, volume = {134}, year = {2025}, }
• (2025). Matrix-weighted networks for modeling multidimensional dynamics: Theoretical foundations and applications to network coherence. PRL, 134(23), 237401. (www)

  @article{ , abstract = {Networks are powerful tools for modeling interactions in complex systems. While traditional networks use scalar edge weights, many real-world systems involve multidimensional interactions. For example, in social networks, individuals often have multiple interconnected opinions that can affect different opinions of other individuals, which can be better characterized by matrices. We propose a general framework for modeling such multidimensional interacting dynamics: matrix-weighted networks (MWNs). We present the mathematical foundations of MWNs and examine consensus dynamics and random walks within this context. Our results reveal that the coherence of MWNs gives rise to nontrivial steady states that generalize the notions of communities and structural balance in traditional networks.}, archive = {J_PRL}, author = {Yu Tian and Sadamori Kojaku and Hiroki Sayama and Renaud Lambiotte}, doi = {10.1103/jw1k-6s7w}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {237401}, shortjournal = {Phys. Rev. Lett.}, title = {Matrix-weighted networks for modeling multidimensional dynamics: Theoretical foundations and applications to network coherence}, volume = {134}, year = {2025}, }
• (2025). Promoting fluctuation theorems into covariant forms. PRL, 134(23), 237102. (www)

  @article{ , abstract = {The principle of covariance, a cornerstone of modern physics, asserts the equivalence of all inertial frames of reference. Fluctuation theorems, as extensions of the second law of thermodynamics, establish universal connections between irreversibility and fluctuation in terms of stochastic thermodynamic quantities. However, these relations typically assume that both the thermodynamic system and the heat bath are at rest with respect to the observer, thereby failing to satisfy the principle of covariance. In this Letter, by introducing covariant work and heat that incorporate both energy-related and momentum-related components, we promote fluctuation theorems into covariant forms applicable to moving thermodynamic systems and moving heat baths. We illustrate this framework with two examples: the work statistics of a relativistic stochastic field and the heat statistics of a relativistic Brownian motion. Although our Letter is carried out in the context of special relativity, the results can be extended to the nonrelativistic limit. Our Letter combines the principle of covariance and fluctuation theorems into a coherent framework and may have applications in the study of thermodynamics relevant to cosmic microwave background as well as the radiative heat transfer and noncontact friction between relatively moving bodies.}, archive = {J_PRL}, author = {Ji-Hui Pei (裴继辉 and Jin-Fu Chen (陈劲夫 and H. T. Quan (全海涛}, doi = {10.1103/xlmq-g6m5}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {237102}, shortjournal = {Phys. Rev. Lett.}, title = {Promoting fluctuation theorems into covariant forms}, volume = {134}, year = {2025}, }
• (2025). Moments of entropy production in dissipative devices. PRL, 134(23), 237101. (www)

  @article{ , abstract = {We characterize the possible moments of entropy production for overdamped stationary Markov processes. We find a general formulation of the problem, and derive a new necessary condition relating the second and third moments. We determine all possible first, second, and third moments of entropy production for a white noise process. As a consequence, we obtain a lower bound for the skewness of the current fluctuations in dissipative devices such as transistors, thereby demonstrating that the Gaussianity assumption widely used, e.g., in electronic engineering is thermodynamically inconsistent.}, archive = {J_PRL}, author = {Jean-Charles Delvenne and Léopold Van Brandt}, doi = {10.1103/jqsx-ycjv}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {237101}, shortjournal = {Phys. Rev. Lett.}, title = {Moments of entropy production in dissipative devices}, volume = {134}, year = {2025}, }
• (2025). Ballast charges for semiconductor spin qubits. PRL, 134(23), 237002. (www)

  @article{ , abstract = {Semiconductor spin qubits are an attractive platform for quantum computing, but their performance is degraded primarily by fluctuating electromagnetic environments. We introduce the concept of ballast charges, which are induced charges on the surface of an additional screening layer situated below the qubits. The counteractive behavior of these charges can significantly reduce the power spectral density associated with fluctuations from two-level systems that contribute to charge noise. Our simulations show that the dephasing time of a single-spin qubit in a Si/SiGe device increases by a factor of 4 to 6 on average when using this method. We also discuss the physical implementation and potential challenges of this approach.}, archive = {J_PRL}, author = {Yujun Choi and John M. Nichol and Edwin Barnes}, doi = {10.1103/81qt-48bl}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {237002}, shortjournal = {Phys. Rev. Lett.}, title = {Ballast charges for semiconductor spin qubits}, volume = {134}, year = {2025}, }
• (2025). Causal-constraint broadband sound absorption under isothermal process. PRL, 134(23), 237001. (www)

  @article{ , abstract = {Causality, a cornerstone of physical laws, fundamentally links a system’s structural characteristics to its wave interaction properties, such as the minimum thickness of acoustic absorbers required for specific absorption spectra. Traditional causality principles for sound absorption are derived under the assumption of adiabatic sound propagation. In this Letter, we propose a generalized causal framework that incorporates isothermal processes, accounting for nonslip boundary conditions at the fluid-solid interface. These conditions introduce velocity and temperature gradients, challenging the conventional adiabatic assumption. To validate our framework, we analyze two distinct absorber types: a metamaterial with multiresonant units and a metafoam with multilayer double-porosity structures. Our theoretical and experimental studies reveal that absorber thickness can exceed the adiabatic limit, being instead governed by isothermal constraints. This paradigm shift deepens the understanding of sound absorption mechanisms and paves the way for designing high-performance acoustic devices that approach fundamental performance limits.}, archive = {J_PRL}, author = {Chuanhao Ge and Nengyin Wang and Xu Wang and Yong Li}, doi = {10.1103/jwvm-ntts}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {237001}, shortjournal = {Phys. Rev. Lett.}, title = {Causal-constraint broadband sound absorption under isothermal process}, volume = {134}, year = {2025}, }
• (2025). Coherent interaction of 2s and 1s exciton states in transition-metal dichalcogenide monolayers. PRL, 134(23), 236901. (www)

  @article{ , abstract = {We use femtosecond pump-probe spectroscopy to study the coherent interaction of excited exciton states in and monolayers via the optical Stark effect. For cocircularly polarized pump and probe, we measure a blueshift that points to a repulsive interaction between the and exciton states. The determined interaction strength is on par with that of the in agreement with the semiconductor Bloch equations. Furthermore, we demonstrate the existence of a biexciton bound state in the cross-circular configuration in both materials and determine their binding energy.}, archive = {J_PRL}, author = {Max Wegerhoff and Moritz Scharfstädt and Stefan Linden and Andrea Bergschneider}, doi = {10.1103/PhysRevLett.134.236901}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236901}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent interaction of 2s and 1s exciton states in transition-metal dichalcogenide monolayers}, volume = {134}, year = {2025}, }
• (2025). Field-free superconducting diode effect in layered superconductor FeSe. PRL, 134(23), 236703. (www)

  @article{ , abstract = {The superconducting diode effect (SDE), where zero-resistance states appear nonreciprocally during current injection, is receiving tremendous interest in both fundamental and applied physics because the SDE is a novel manifestation of symmetry breaking and enables the creation of a novel diode. In particular, magnetic-field-free SDEs have been extensively investigated because of their potential to serve as building blocks for superconducting circuit technology. In this Letter, we report the field-free SDE in a layered superconductor, FeSe. Its underlying physics is clarified by systematic controlled experiments to be an interplay of a large thermoelectric response and geometrical asymmetry in FeSe. Our findings can pave a new avenue for the construction of novel material and device platforms utilizing SDEs.}, archive = {J_PRL}, author = {Utane Nagata and Motomi Aoki and Akito Daido and Shigeru Kasahara and Yuichi Kasahara and Ryo Ohshima and Yuichiro Ando and Youichi Yanase and Yuji Matsuda and Masashi Shiraishi}, doi = {10.1103/PhysRevLett.134.236703}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236703}, shortjournal = {Phys. Rev. Lett.}, title = {Field-free superconducting diode effect in layered superconductor FeSe}, volume = {134}, year = {2025}, }
• (2025). Direct evidence for anisotropic magnetic interaction in α−RuCl3 from polarized inelastic neutron scattering. PRL, 134(23), 236702. (www)

  @article{ , abstract = {Polarized neutron scattering experiments reveal anisotropy of magnetic correlations in the candidate Kitaev material α − RuCl 3 . The anisotropy of the inelastic response at the magnetic Bragg positions is opposite to the expectation for a simple Heisenberg model. Near the antiferromagnetic propagation vector, there are no low-energy transversal magnon modes and the response is always uniaxially polarized. These observations directly prove the fully anisotropic and bond-directional character of the magnetic interaction in α − RuCl 3 . However, other findings disagree with a simple or strongly dominant Kitaev component.}, archive = {J_PRL}, author = {Markus Braden and Xiao Wang and Alexandre Bertin and Paul Steffens and Yixi Su}, doi = {10.1103/vlzq-swfm}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236702}, shortjournal = {Phys. Rev. Lett.}, title = {Direct evidence for anisotropic magnetic interaction in α−RuCl3 from polarized inelastic neutron scattering}, volume = {134}, year = {2025}, }
• (2025). Magnetic switching of phonon angular momentum in a ferrimagnetic insulator. PRL, 134(23), 236701. (www)

  @article{ , abstract = {Circularly polarized phonons offer a new route for mediating angular momentum in solids. However, controlling phonon angular momentum without altering the material’s structure or composition remains challenging. Here, we demonstrate the nonvolatile switching of angular momentum-carrying phonons by leveraging intrinsic ferrimagnetism in an insulator. We find a pair of chiral phonons with giant energy splitting, reaching 20% of the phonon frequency due to spontaneously broken time-reversal symmetry. With a moderate magnetic field, the phonon angular momentum of the two chiral phonon branches can be switched along with the magnetization. Notably, near the critical temperature, the effective phonon magnetic moment is enhanced, reaching 2.62 Bohr magneton, exceeding the moment of a magnon. A microscopic model based on phonon-magnon coupling accounts for the observations. Furthermore, we identify two types of phononic domains with opposite phonon Zeeman splitting and propose the existence of topologically protected phononic edge modes at domain boundaries. These results demonstrate effective manipulation of chiral phonons with magnetism, and pave the way for engineering chiral phononic domains on the micrometer scale.}, archive = {J_PRL}, author = {Fangliang Wu and Jing Zhou and Song Bao and Liangyue Li and Jinsheng Wen and Yuan Wan and Qi Zhang}, doi = {10.1103/gcgl-9sbb}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236701}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic switching of phonon angular momentum in a ferrimagnetic insulator}, volume = {134}, year = {2025}, }
• (2025). Instanton-induced supersymmetry breaking in topological semimetals. PRL, 134(23), 236602. (www)

  @article{ , abstract = {Supersymmetry (SUSY) proposed as an elementary symmetry for physics beyond the standard model has found important applications in various areas outside high-energy physics. Here, we systematically implement supersymmetric quantum mechanics—exhibiting fundamental SUSY properties in the simple setting of quantum mechanics—into a wide range of topological semimetals, where the broken translational symmetry, e.g., by a magnetic field, is effectively captured by a SUSY potential. We show that the dynamical SUSY breaking via the instanton effect over the SUSY potential valleys works as the underlying mechanism for the gap opening of the topological semimetallic phases, and the magnitude of the instanton effect is proportional to the energy gap. This instanton mechanism provides a simple criterion for determining whether the energy gap has been opened, without resorting to detailed calculations, i.e., a finite energy gap is opened if and only if the SUSY potential has an even number of zeros. Our theory leads to previously unexpected results: even an infinitesimal magnetic field can open a gap in topologically robust Dirac, Weyl, and nodal-line semimetallic phases due to the dynamical SUSY breaking. Overall, the revealed connection between SUSY quantum mechanics and nonuniform topological semimetals can elucidate previously ambiguous phenomena, provide guidance for future investigations, and open a new avenue for exploring topological semimetals.}, archive = {J_PRL}, author = {W. B. Rui and Y. X. Zhao and Z. D. Wang}, doi = {10.1103/hcw4-y356}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236602}, shortjournal = {Phys. Rev. Lett.}, title = {Instanton-induced supersymmetry breaking in topological semimetals}, volume = {134}, year = {2025}, }
• (2025). Bulk-boundary correspondence of fractonic field theories. PRL, 134(23), 236601. (www)

  @article{ , abstract = {We develop a theory of edge excitations of fractonic systems in two dimensions, and elucidate their connections to bulk transport properties and quantum statistics of bulk excitations. The system we consider has immobile point charges, dipoles constrained to move only along lines perpendicular to their moment, and freely mobile quadrupoles and higher multipoles, realizing a bulk fractonic analog of fractional quantum Hall phases. We demonstrate that a quantized braiding phase between two bulk excitations is obtained only in two cases: when a point quadrupole braids around an immobile point charge, or when two non-orthogonal point dipoles braid with one another. The presence of a boundary edge in the system entails two types of gapless edge excitation modes, one that is fractonic with immobile charges and longitudinal dipoles, and a second non-fractonic mode consisting of transverse dipoles. We derive a novel current algebra of the fractonic edge modes. Further, investigating the effect of local edge-to-edge tunneling on these modes, we find that such a process is a relevant perturbation suggesting the possibility of edge deformation.}, archive = {J_PRL}, author = {Bhandaru Phani Parasar and Yuval Gefen and Vijay B. Shenoy}, doi = {10.1103/ggls-zhl8}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236601}, shortjournal = {Phys. Rev. Lett.}, title = {Bulk-boundary correspondence of fractonic field theories}, volume = {134}, year = {2025}, }
• (2025). Nature of spinons in 1D spin chains. PRL, 134(23), 236504. (www)

  @article{ , abstract = {We provide an intuitive understanding of the collective low-energy spin excitation of the one-dimensional spin- antiferromagnetic Heisenberg chain, known as the spinon. To this end, we demonstrate how a single spinon can be excited by adding one extra spin to the ground state. This procedure accurately reproduces all key features of the spinon’s dispersion. These follow from the vanishing norm of the excited state which is triggered by the ground state entanglement. Next, we show that the spinon dispersion can be approximately reproduced if we replace the true ground state with the simplest valence-bond solid. This proves that the spinon of the one-dimensional Heisenberg model can be understood as a single spin flowing through a valence-bond solid.}, archive = {J_PRL}, author = {Teresa Kulka and Miłosz Panfil and Mona Berciu and Krzysztof Wohlfeld}, doi = {10.1103/stvg-lg9h}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236504}, shortjournal = {Phys. Rev. Lett.}, title = {Nature of spinons in 1D spin chains}, volume = {134}, year = {2025}, }
• (2025). Tunable t−t′−U hubbard models in twisted square homobilayers. PRL, 134(23), 236503. (www)

  @article{ , abstract = {Square lattice Hubbard model with tunable hopping ratio t ′ / t is highly promising for realizing a variety of quantum phases, including higher-temperature superconductivity. We show that twisted square lattice homobilayers offer such tunability when the flat bands originate from the corner of the Brillouin zone. An emergent symmetry, generically present at low twist angles, enforces t = 0 for these bands. Breaking it with interlayer displacement field or in-plane magnetic field introduces t and anisotropy, tunable in a wide range for correlated electrons on the moiré square lattice.}, archive = {J_PRL}, author = {P. Myles Eugenio and Zhu-Xi Luo and Ashvin Vishwanath and Pavel A. Volkov}, doi = {10.1103/PhysRevLett.134.236503}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236503}, shortjournal = {Phys. Rev. Lett.}, title = {Tunable t−t′−U hubbard models in twisted square homobilayers}, volume = {134}, year = {2025}, }
• (2025). Non-fermi liquids from subsystem symmetry breaking in van der waals multilayers. PRL, 134(23), 236502. (www)

  @article{ , abstract = {We investigate the spontaneous breaking of subsystem symmetry in a stack of two-dimensional Fermi liquid metals, each maintaining a subsystem number conservation symmetry, driven by interlayer exciton condensation. The resulting Goldstone modes in this broken symmetry phase couple to the quasiparticle current perpendicular to the layers. This coupling, which remains nonzero for small momentum transfers, leads to the emergence of a three-dimensional anisotropic marginal Fermi liquid state when the number of layers is sufficiently large. We propose a possible experimental realization of this phenomenon in two-dimensional multilayer van der Waals heterostructures. Using self-consistent mean-field calculations, we characterize the subsystem symmetry-broken metallic state and examine the effects of fluctuations on its physical properties within the random phase approximation. We find that these fluctuations produce additional logarithmic enhancements to the specific heat at low temperature, specifically .}, archive = {J_PRL}, author = {Archisman Panigrahi and Ajesh Kumar}, doi = {10.1103/v6r7-4ph9}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236502}, shortjournal = {Phys. Rev. Lett.}, title = {Non-fermi liquids from subsystem symmetry breaking in van der waals multilayers}, volume = {134}, year = {2025}, }
• (2025). Magnetic signatures of pressure-induced multicomponent superconductivity in UTe2. PRL, 134(23), 236501. (www)

  @article{ , abstract = {The phase diagram of the heavy fermion compound contains multiple superconducting phases, several of which show characteristics of odd-parity pairing. We have investigated the pressure dependence of the superconducting transition in high-quality crystals of by tracking its signature in the magnetic susceptibility . A single, sharp superconducting transition is observed at low pressures . At higher pressure, a second feature emerges in , which is located at the lower-temperature superconducting phase boundary previously identified in specific heat measurements. This second transition anomaly in can be attributed to a step change in the London penetration depth, providing direct evidence for a change in the superconducting order parameter of . Thermodynamic constraints suggest that the low temperature, high pressure superconducting state is distinct from zero pressure superconductivity as well as from the high pressure, high temperature superconducting state, raising the possibility of multicomponent superconductivity in high pressure .}, archive = {J_PRL}, author = {Zheyu Wu and Jiasheng Chen and Theodore I. Weinberger and Andrej Cabala and Vladimír Sechovský and Michal Vališka and Patricia L. Alireza and Alexander G. Eaton and F. Malte Grosche}, doi = {10.1103/PhysRevLett.134.236501}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236501}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic signatures of pressure-induced multicomponent superconductivity in UTe2}, volume = {134}, year = {2025}, }
• (2025). Nonreciprocal transport in KTaO3-based interface superconductors with parity mixing. PRL, 134(23), 236303. (www)

  @article{ , abstract = {Spin-triplet pairing of superconductivity, drawing huge attention by enabling future technologies in quantum computing, spintronics, and other fields, can host unique transport phenomena. Here, we report gigantically enhanced nonreciprocal transport in the superconducting fluctuation regime of KTaO 3 -based interface superconductors. Notably, the observed nonreciprocity undergoes a sign reversal compared to the normal state. Combining experimental observations with theoretical modeling, we identify its dominant mechanism as the vortex motion and parity mixing of spin-singlet and spin-triplet pairings. We also provide evidence for an attractive spin-triplet pairing interaction. Furthermore, the nonreciprocal response is highly tunable by orders of magnitude using electrostatic gating. These findings shed light on the pairing mechanisms in Rashba superconductors and offer new pathways for developing nonlinear superconducting devices.}, archive = {J_PRL}, author = {Jinfeng Zhai and Taekoo Oh and Hao Liu and Chaoyu Pan and Naoto Nagaosa and Pan He and Jian Shen}, doi = {10.1103/nshl-7b3z}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236303}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal transport in KTaO3-based interface superconductors with parity mixing}, volume = {134}, year = {2025}, }
• (2025). Macroscopic quantum states and universal correlations in a disorder-order interface propagating over a 1D ground state. PRL, 134(23), 236302. (www)

  @article{ , abstract = {We consider translationally invariant quantum spin- 1 2 chains with local interactions and a discrete symmetry that is spontaneously broken at zero temperature. We envision experimenters switching off the couplings between two parts of the system and preparing them in independent equilibrium states. One side of the chain is prepared in a disordered phase, and the other in a symmetry-breaking ground state. When the couplings are switched back on, time evolution ensues. We argue that in integrable systems the front separating the ordered region recedes at the maximal velocity of quasiparticle excitations over the ground state. We infer that, generically, the order parameters should vary on a subdiffusive scale of order t 1 / 3 , where t is time, and their fluctuations should exhibit the same scaling. This interfacial region exhibits full range correlations, indicating that it cannot be decomposed into nearly uncorrelated subsystems. Using the transverse-field Ising chain as a case study, we demonstrate that all order parameters follow the same universal scaling functions. Through an analysis of the skew information, we uncover that the breakdown of cluster decomposition has a quantum contribution: each subsystem within the interfacial region, with extent comparable to the region, exists in a macroscopic quantum state.}, archive = {J_PRL}, author = {Vanja Marić and Florent Ferro and Maurizio Fagotti}, doi = {10.1103/982k-5jmn}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236302}, shortjournal = {Phys. Rev. Lett.}, title = {Macroscopic quantum states and universal correlations in a disorder-order interface propagating over a 1D ground state}, volume = {134}, year = {2025}, }
• (2025). Quasi-1D coulomb drag in the nonlinear regime. PRL, 134(23), 236301. (www)

  @article{ , abstract = {One-dimensional Coulomb drag has been an essential tool to probe the physics of interacting Tomonaga-Luttinger liquids. To date, most experimental work has focused on the linear regime while the predictions for Luttinger liquids beyond the linear response theory remain largely untested. In this Letter, we report measurements of reciprocal momentum transfer induced Coulomb drag between vertically coupled quasi-one-dimensional quantum wires in the nonlinear regime. Measurements were performed at ultralow temperatures between wires only 15 nm apart. Our results reveal a nonlinear dependence of the drag voltage as a function of the drive current superimposed with an oscillatory contribution, in agreement with theoretical predictions for Coulomb drag between Tomonaga-Luttinger liquids. Additionally, the observed current-voltage characteristics exhibit a nonmonotonic temperature dependence, further corroborating the presence of non-Fermi-liquid behavior in our system. These findings are observed both in the single and in the multiple subband regimes and in the presence of disorder, extending the onset of this behavior beyond the clean single channel Tomonaga-Luttinger regime where the predictions were originally formulated.}, archive = {J_PRL}, author = {Mingyang Zheng and Rebika Makaju and Rasul Gazizulin and Alex Levchenko and Sadhvikas J. Addamane and Dominique Laroche}, doi = {10.1103/v3dn-bnrp}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236301}, shortjournal = {Phys. Rev. Lett.}, title = {Quasi-1D coulomb drag in the nonlinear regime}, volume = {134}, year = {2025}, }
• (2025). Layer hall effect without external electric field. PRL, 134(23), 236206. (www)

  @article{ , abstract = {The layer Hall effect is an intriguing phenomenon observed in magnetic topological layered materials, where the Hall response arises from the opposite deflection of electrons on top and bottom layers. To realize the layer Hall effect, space-time symmetry is typically broken by applying an external electric field. In this Letter, we propose a new mechanism to realize the layer Hall effect by introducing inequivalent exchange fields on both surfaces of a topological insulator thin film in the absence of an electric field. This approach yields a distinct Hall response compared to the conventional electric-field-induced layer Hall effect, particularly with respect to the Fermi level. Taking the topological insulator as a concrete example, we demonstrate the feasibility of inducing the layer Hall effect only by coupling the top and bottom surfaces of with different magnetic insulators. Notably, we show that both built-in electric-field-induced and inequivalent exchange-field-induced layer Hall effects can be achieved by tuning the stacking order between and the magnetic layers. Given the well-established experimental techniques for fabricating topological insulator thin films, our work offers a viable pathway for realizing layer Hall effect without external electric field.}, archive = {J_PRL}, author = {Yulei Han and Yunpeng Guo and Zeyu Li and Zhenhua Qiao}, doi = {10.1103/tdx6-gnxz}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236206}, shortjournal = {Phys. Rev. Lett.}, title = {Layer hall effect without external electric field}, volume = {134}, year = {2025}, }
• (2025). Nanoscale conducting and insulating domains on YbB6. PRL, 134(23), 236205. (www)

  @article{ , abstract = {YbB 6 is a predicted topological insulator, with experimental evidence for conducting surface states of yet-unproven origin. However, its lack of a natural cleavage plane, and resultant surface-dependent polarity, has obscured its study. We use scanning tunneling microscopy to image the cleaved surface of YbB 6 , which exhibits several coexisting terminations with distinct atomic structures. Our spectroscopic measurements reveal band bending between the terminations, resulting in both conducting and fully gapped domains. In the conducting domains, we observe spectral peaks that are suggestive of Van Hove singularities arising from Rashba spin-split quantum well states. The insulating domains rule out the possibility that YbB 6 is a strong topological insulator, while the spin-polarized conducting domains suggest possible utility for spintronic devices.}, archive = {J_PRL}, author = {Aaron Coe and Zhi-Huai Zhu and Yang He and Dae-Jeong Kim and Zachary Fisk and Jason D. Hoffman and Jennifer E. Hoffman}, doi = {10.1103/1cft-d9np}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236205}, shortjournal = {Phys. Rev. Lett.}, title = {Nanoscale conducting and insulating domains on YbB6}, volume = {134}, year = {2025}, }
• (2025). Warping effect-induced spin current absorption at various timescales in Fe/Bi2Te3 heterostructures. PRL, 134(23), 236204. (www)

  @article{ , abstract = {The spin pumping in ferromagnet/nonmagnetic materials ( ) heterostructures is an effective technique to inject spin current into NM, which provides the possibility of ultrafast, low-power consumption spintronic devices. Previous work demonstrates that the high order terms in theory can induce a large warping effect, and consequently snowflakelike Fermi contour in topological insulator (TI). Unfortunately, the effect of warped topological surface state (TSS) on pure spin absorption in heterostructures is completely unknown. Here, by considering strength of spin accumulation, we identified a mechanism for the anisotropic absorption of spin current in a heterostructure with a large warping effect. If the density of states (DOS) of TSS dominates at the Fermi surface, the warping effect results in an anisotropic Gilbert damping at nanosecond timescale and almost isotropic ultrafast demagnetization time at femtosecond timescale. The anisotropy of Gilbert damping is found to decrease as bulk state contributions become more significant in thicker films. Our theoretical predictions regarding the warping effect-induced spin current absorption at nanosecond and subpicosecond timescales have been experimentally validated in heterostructures by ferromagnetic resonance and time-resolved magneto-optical Kerr effect (TRMOKE) results, respectively. Our work provides a more intuitional way to understand the spin transfer mechanism, and lays the groundwork for advancing anisotropic spintronics.}, archive = {J_PRL}, author = {Jia-nan Liu and Hao-Pu Xue and Zhuo Deng and Qing-Lin Yang and Xiao-Min Li and Xue-Dong Bai and Xu Yang and Peng-Tao Yang and Yu-Han Gao and Wei He and Xiang-Qun Zhang and Zhao-Hua Cheng}, doi = {10.1103/PhysRevLett.134.236204}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236204}, shortjournal = {Phys. Rev. Lett.}, title = {Warping effect-induced spin current absorption at various timescales in Fe/Bi2Te3 heterostructures}, volume = {134}, year = {2025}, }
• (2025). Site-resolved near-surface cation diffusion in magnetite. PRL, 134(23), 236203. (www)

  @article{ , abstract = {In situ nuclear forward scattering shows a thermally induced cation exchange between a thin-film and a (001) substrate predominantly in the octahedral sublattice for a temperature range between 470 and 710 K. The overall activation barrier in this temperature range is found to be , which is significantly lower than expected from extrapolating a bulk diffusion model. This observation can be attributed to the large out-of-equilibrium cation deficit as determined by surface x-ray diffraction. Despite the relatively low hopping barrier, the diffusion constant is about 5 orders of magnitude lower than expected for magnetite having an equilibrium cation stoichiometry. The results are relevant for applications relying on the near-surface structure and stoichiometry of magnetite, and we argue that the correlation between cation diffusion and stoichiometry may play a role for a wider range of oxide materials.}, archive = {J_PRL}, author = {Steffen Tober and Jan-Christian Schober and Marcus Creutzburg and Esko Erik Beck and Guilherme Dalla Lana Semione and Simon Chung and Leon Jacobse and Björn Arndt and Alina Vlad and René Steinbrügge and Hans-Christian Wille and Ilya Sergueev and Heshmat Noei and Kai Schlage and Olaf Leupold and Vedran Vonk and Andreas Stierle}, doi = {10.1103/PhysRevLett.134.236203}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236203}, shortjournal = {Phys. Rev. Lett.}, title = {Site-resolved near-surface cation diffusion in magnetite}, volume = {134}, year = {2025}, }
• (2025). Real-time 3D coherent X-ray diffraction imaging. PRL, 134(23), 236202. (www)

  @article{ , abstract = {The coherent x-ray diffraction imaging (CXDI) technique offers unique insights into the nanoscale world, enabling the reconstruction of 3D structures with a nanoscale resolution achieved through computational phase reconstruction from measured scattered intensity maps. However, the computational demands of 3D coherent x-ray diffraction imaging limit its real-time application in experimental settings. This Letter presents a carousel phase retrieval algorithm (CPRA) that enables the real-time, high-resolution reconstruction of computationally complex 3D objects. CPRA is based on representing the 3D reconstruction problem as a set of 2D reconstructions of projected images corresponding to different experimentally collected angles via the Fourier slice theorem. The consistency between the 2D reconstructed images is based on an iterative procedure in which each 2D reconstruction accounts for the adjacent 2D reconstructed images in a periodic (carousel) manner. Demonstrations on complex systems, including a lithium-rich layered oxide particle and a biological cell of Staphylococcus aureus , demonstrate that CPRA significantly enhances the reconstruction quality and enables the reconstruction process to be completed in real time during the experiment.}, archive = {J_PRL}, author = {Fangzhou Ai and Oleg Shpyrko and Vitaliy Lomakin}, doi = {10.1103/PhysRevLett.134.236202}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236202}, shortjournal = {Phys. Rev. Lett.}, title = {Real-time 3D coherent X-ray diffraction imaging}, volume = {134}, year = {2025}, }
• (2025). Structure and strain field of surface dislocations on gold determined by surface X-ray diffraction. PRL, 134(23), 236201. (www)

  @article{ , abstract = {Au(111) with its famous surface reconstruction has led to many studies, but its subsurface structure has never been determined. Here, we study the Au(677) surface which is a vicinal of Au(111) with steps and surface reconstruction, showing an array of surface dislocations. By using surface x-ray diffraction and atomistic simulations, we are able to quantitatively determine the complete structure and the strain fields associated with the surface reconstruction described in terms of surface dislocations, especially a stair-rod dislocation lying parallel to the surface step. The stair-rod dislocation strain field adds up to the one due to the step dipole, explaining the extraordinary regularity of the step array. We can also give new insights on the strain field associated with the Au(111) surface discommensuration lines ( reconstruction) and find that it penetrates deeply into the bulk, in contrast with commonly used surface reconstruction models.}, archive = {J_PRL}, author = {Vincent Repain and Julien Durinck and Yves Garreau and Alessandro Coati and Yann Girard and Sylvie Rousset and Christophe Coupeau and Amandine Bellec}, doi = {10.1103/PhysRevLett.134.236201}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236201}, shortjournal = {Phys. Rev. Lett.}, title = {Structure and strain field of surface dislocations on gold determined by surface X-ray diffraction}, volume = {134}, year = {2025}, }
• (2025). Dual view of the z2-gauged XY model in 3D. PRL, 134(23), 236001. (www)

  @article{ , abstract = {The Z 2 -gauged XY model is of long-standing interest both in the context of nematic order, and the study of fractionalization and superconductivity. This Letter presents heuristic arguments that no deconfinement of the XY field occurs in this model and presents results of a large-scale Monte Carlo simulations on a cubic lattice that are consistent with this conclusion. The correlation radius determining the confinement is found to be growing rapidly as a function of the parameters in the phase featuring the nematic order. Thus, mesoscopic properties of the system can mimic deconfinement with high accuracy in some part of the phase diagram.}, archive = {J_PRL}, author = {Piers Coleman and Anatoly Kuklov and Alexei Tsvelik}, doi = {10.1103/nf4j-kbtj}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {236001}, shortjournal = {Phys. Rev. Lett.}, title = {Dual view of the z2-gauged XY model in 3D}, volume = {134}, year = {2025}, }
• (2025). Spatiotemporal energy cascade in three-dimensional magnetohydrodynamic turbulence. PRL, 134(23), 235201. (www)

  @article{ , abstract = {We present a new scale decomposition method to investigate turbulence in wavenumber-frequency space. Using 3D magnetohydrodynamic turbulence simulations, we show that magnetic fluctuations with time scales longer than the nonlinear time exhibit an inverse cascade toward even smaller frequencies. Low frequency magnetic fluctuations support turbulence, acting as an energy reservoir that is converted into plasma kinetic energy, the latter cascading toward large wavenumbers and frequencies, where it is dissipated. Our results shed new light on the spatiotemporal properties of turbulence, potentially explaining the origin and role of low frequency turbulent fluctuations in the solar wind.}, archive = {J_PRL}, author = {Giuseppe Arrò and Hui Li and William H. Matthaeus}, doi = {10.1103/hx6s-8ns8}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {235201}, shortjournal = {Phys. Rev. Lett.}, title = {Spatiotemporal energy cascade in three-dimensional magnetohydrodynamic turbulence}, volume = {134}, year = {2025}, }
• (2025). Physics of edge-core coupling by inward turbulence propagation. PRL, 134(23), 235101. (www)

  @article{ , abstract = {The dynamics of edge-core coupling is critically important to the optimization of magnetically confined fusion plasmas. Since early proposals, there has been persistent speculation that inward propagation of turbulence from the boundary is a possible means to energize the edge-core coupling region. However, the detailed mechanism of this process has remained a mystery until recent experiments observed that regular, intense gradient relaxation events generated blob-void pairs very close to the last closed flux surface. Blobs ( ) propagate outward and detach from the bulk plasma, while voids ( ) propagate inward, and so stir the core plasma. Here, we demonstrate that this heretofore ignored process of void emission can drive a broad turbulent layer of width , for typical parameters. The mechanism is the Cherenkov emission of drift waves from inward-propagating voids. The model shows promise to resolve several questions surrounding the shortfall problem and the strong turbulence in the edge-core coupling region.}, archive = {J_PRL}, author = {Mingyun Cao and P. H. Diamond}, doi = {10.1103/PhysRevLett.134.235101}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {235101}, shortjournal = {Phys. Rev. Lett.}, title = {Physics of edge-core coupling by inward turbulence propagation}, volume = {134}, year = {2025}, }
• (2025). Causality and instability in wave propagation in random time-varying media. PRL, 134(23), 233801. (www)

  @article{ , abstract = {We develop a theoretical model to investigate wave propagation in media with random time-varying properties, where temporal fluctuations lead to complex scattering dynamics. Focusing on the ensemble-averaged field, we derive an exact expression for the average Green’s function in the presence of finite temporal disorder, and extend the analysis to the thermodynamic limit. In contrast to spatial disorder, causality prevents recurrent scattering, allowing us to achieve a nonperturbative solution. We introduce an effective medium description providing a simple analysis of the propagation regimes. Our findings offer new insights into wave dynamics in temporally disordered media, with potential applications in time-varying metamaterials, dynamic sensing, and imaging in turbulent or chaotic environments.}, archive = {J_PRL}, author = {R. Pierrat and J. Rocha and R. Carminati}, doi = {10.1103/td38-f69r}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233801}, shortjournal = {Phys. Rev. Lett.}, title = {Causality and instability in wave propagation in random time-varying media}, volume = {134}, year = {2025}, }
• (2025). Hierarchical verification of non-gaussian coherence in bosonic quantum states. PRL, 134(23), 233604. (www)

  @article{ , abstract = {Non-Gaussianity, a distinctive characteristic of bosonic quantum states, is pivotal in advancing quantum networks, fault-tolerant quantum computing, and high-precision metrology. Verifying the quantum nature of a state, particularly its non-Gaussian features, is essential for ensuring the reliability and performance of these technologies. However, the specific properties required for each application demand tailored validation thresholds. Here, we introduce a hierarchical framework comprising absolute, relative, and qubit-specific thresholds to assess the non-Gaussianity of local coherences. We illustrate this framework using heralded optical non-Gaussian states with the highest purities available in optical platforms. This comprehensive framework presents the first detailed evaluation of number state coherences and can be extended to a wide range of bosonic states.}, archive = {J_PRL}, author = {Beate E. Asenbeck and Lukáš Lachman and Ambroise Boyer and Priyanka Giri and Alban Urvoy and Radim Filip and Julien Laurat}, doi = {10.1103/PhysRevLett.134.233604}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233604}, shortjournal = {Phys. Rev. Lett.}, title = {Hierarchical verification of non-gaussian coherence in bosonic quantum states}, volume = {134}, year = {2025}, }
• (2025). Narrow optical linewidths in stoichiometric layered rare-earth crystals. PRL, 134(23), 233603. (www)

  @article{ , abstract = {Rare-earth emitters in solids are well suited for implementing efficient, long-lived quantum memory coupled to integrated photonics for scalable quantum technologies. They are typically introduced as dopants in a solid-state host, but this introduces disorder and limits the available density of emitters. Stoichiometric materials can offer high densities with narrow optical linewidths. The regular spacing of emitters also opens possibilities for quantum information processing and collective effects. Here, we show narrow optical linewidths in a layered stoichiometric crystalline material, NaEu ( IO 3 ) 4 . We observed an inhomogeneous linewidth of 2.2(1) GHz and a homogeneous linewidth of 120(4) kHz. Using spectral hole-burning techniques, we observe a hyperfine spin lifetime of 1.9(4) s. Furthermore, we demonstrate an atomic frequency comb delay of up to 800 ns.}, archive = {J_PRL}, author = {Donny R. Pearson, Jr and Ashwith Prabhu and Selvin Tobar and Jack D’Amelio and Amy Tram and Zachary W. Riedel and Daniel P. Shoemaker and Elizabeth A. Goldschmidt}, doi = {10.1103/p39m-pnvt}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233603}, shortjournal = {Phys. Rev. Lett.}, title = {Narrow optical linewidths in stoichiometric layered rare-earth crystals}, volume = {134}, year = {2025}, }
• (2025). Chiral dissociation of bound photon pairs for a non-hermitian skin effect. PRL, 134(23), 233602. (www)

  @article{ , abstract = {We theoretically study the bound states of interacting photons propagating in a waveguide chirally coupled to an array of atoms. We demonstrate that the bound photon pairs can concentrate at the edge of the array and link this to the non-Hermitian skin effect. Unlike tight-binding non-Hermitian setups, the bound states in the waveguide-coupled array exhibit infinite radiative lifetimes when the array has an infinite size. However, in a finite array, non-Hermiticity and localization of bound pairs emerge due to their chiral dissociation into scattering states. Counterintuitively, when the photons are preferentially emitted to the right, the bound pairs are localized at the left edge of the array and vice versa.}, archive = {J_PRL}, author = {Jiaming Shi and Alexander N. Poddubny}, doi = {10.1103/q6wr-2rt9}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233602}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral dissociation of bound photon pairs for a non-hermitian skin effect}, volume = {134}, year = {2025}, }
• (2025). Conditional entanglement amplification via non-hermitian superradiant dynamics. PRL, 134(23), 233601. (www)

  @article{ , abstract = {Because of the inherently probabilistic nature of quantum mechanics, each experimental realization of a dynamical quantum system can produce distinct measurement outcomes, particularly when coupled to a dissipative environment. Although quantum trajectories that lead to exotic, highly entangled states are possible in principle, their observation is typically hindered by extremely low probabilities. In this Letter, we present a method to significantly enhance the probability of generating highly entangled states in an ensemble of atoms undergoing collective superradiant decay on timescales much shorter than the individual atomic spontaneous emission rate. By analyzing an effective non-Hermitian Hamiltonian governing the dynamics between photon emission events, we identify the conditions necessary for these rare no-click trajectories to occur with higher likelihood. Crucially, our method relies on initializing the system in a nonclassical state, whose entanglement is amplified via the non-Hermitian superradiant dynamics. This approach provides a new route to creating highly entangled macroscopic states such as atomic Schrödinger cat states, paving the way for advancements in quantum metrology and other quantum technologies.}, archive = {J_PRL}, author = {Christoph Hotter and Arkadiusz Kosior and Helmut Ritsch and Karol Gietka}, doi = {10.1103/w377-f9mx}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233601}, shortjournal = {Phys. Rev. Lett.}, title = {Conditional entanglement amplification via non-hermitian superradiant dynamics}, volume = {134}, year = {2025}, }
• (2025). Observation of jones-roberts solitons in a paraxial quantum fluid of light. PRL, 134(23), 233401. (www)

  @article{ , abstract = {We investigate the formation and dynamics of Jones-Roberts solitons in a smoothly inhomogeneous quantum fluid. To do so, we create a superfluid of light using a paraxial, near-resonant laser beam propagating through a hot rubidium vapor. We excite a bounded vortex-antivortex dipole in the superfluid and observe its transition to a rarefaction pulse and back, in agreement with the seminal predictions of Jones and Roberts. Employing an analogy with ray optics, we calculate the trajectory of the interacting vortices, deriving an effective refractive index from the inhomogeneous fluid density. Finally, we examine analytically and experimentally the superfluid velocity correlations, observing a transfer of coherence from incompressible to compressible velocity of the quantum fluid, a direct signature of the dynamical conversion between vortices and the rarefaction pulse.}, archive = {J_PRL}, author = {Myrann Baker-Rasooli and Tangui Aladjidi and Nils A. Krause and Ashton S. Bradley and Quentin Glorieux}, doi = {10.1103/PhysRevLett.134.233401}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233401}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of jones-roberts solitons in a paraxial quantum fluid of light}, volume = {134}, year = {2025}, }
• (2025). Bose-einstein condensates of microwave-shielded polar molecules. PRL, 134(23), 233003. (www)

  @article{ , abstract = {We investigate the ground-state phases of ultracold gases composed of bosonic microwave-shielded polar molecules (MSPMs). Using a translational symmetry-breaking variational ansatz with Jastrow correlations, we characterize the many-body correlations arising from the large shielding core of the two-body potential in a dense gas. We show that the molecular gases are always stabilized by the shielding potential and support a self-bound gas phase and an expanding gas phase. Furthermore, we find that, analogous to liquid He 4 , the condensate fraction is significantly reduced when the size of the shielding core of the two-body potential becomes comparable to the intermolecular distance. For experimental detection, we also identify a bimodal feature in the momentum distribution. Our work invalidates the application of the Gross-Pitaevskii equation to molecular gases and establishes a universal framework to reveal the many-body correlations in dense molecular gases.}, archive = {J_PRL}, author = {Wei-Jian Jin and Fulin Deng and Su Yi and Tao Shi}, doi = {10.1103/b8y9-yvz9}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233003}, shortjournal = {Phys. Rev. Lett.}, title = {Bose-einstein condensates of microwave-shielded polar molecules}, volume = {134}, year = {2025}, }
• (2025). Nonlinear calcium king plot constrains new bosons and nuclear properties. PRL, 134(23), 233002. (www)

  @article{ , abstract = {Nonlinearities in King plots (KP) of isotope shifts (IS) can reveal the existence of beyond-standard-model (BSM) interactions that couple electrons and neutrons. However, it is crucial to distinguish higher-order standard model (SM) effects from BSM physics. We measure the IS of the transitions in and in with sub-Hz precision as well as the nuclear mass ratios with relative uncertainties below for the five stable, even isotopes of calcium ( ). Combined, these measurements yield a calcium KP nonlinearity with a significance of . Precision calculations show that the nonlinearity cannot be fully accounted for by the expected largest higher-order SM effect, the second-order mass shift, and identify the little-studied nuclear polarization as the only remaining SM contribution that may be large enough to explain it. Despite the observed nonlinearity, we improve existing KP-based constraints on a hypothetical Yukawa interaction for most of the new boson masses between and .}, archive = {J_PRL}, author = {Alexander Wilzewski and Lukas J. Spieß and Malte Wehrheim and Shuying Chen and Steven A. King and Peter Micke and Melina Filzinger and Martin R. Steinel and Nils Huntemann and Erik Benkler and Piet O. Schmidt and Luca I. Huber and Jeremy Flannery and Roland Matt and Martin Stadler and Robin Oswald and Fabian Schmid and Daniel Kienzler and Jonathan Home and Diana P. L. Aude Craik and Menno Door and Sergey Eliseev and Pavel Filianin and Jost Herkenhoff and Kathrin Kromer and Klaus Blaum and Vladimir A. Yerokhin and Igor A. Valuev and Natalia S. Oreshkina and Chunhai Lyu and Sreya Banerjee and Christoph H. Keitel and Zoltán Harman and Julian C. Berengut and Anna Viatkina and Jan Gilles and Andrey Surzhykov and Michael K. Rosner and José R. Crespo López-Urrutia and Jan Richter and Agnese Mariotti and Elina Fuchs}, doi = {10.1103/PhysRevLett.134.233002}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {233002}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear calcium king plot constrains new bosons and nuclear properties}, volume = {134}, year = {2025}, }
• (2025). Precision mass measurements reveal low neutron pairing in tin beyond n=82 and its impact on stellar nucleosynthesis. PRL, 134(23), 232701. (www)

  @article{ , abstract = {We present a study on neutron-rich tin ( Z = 50 ) isotopes beyond the doubly closed shell of N = 82 through high-precision mass measurements, including the first-ever measurements of the masses of Sn 136 , Sn 137 , and Sn 138 isotopes. These measurements enhance our understanding of the nuclear structure and astrophysical nucleosynthesis in this previously unexplored region. The new mass data are used for evaluation of the final abundances of mass numbers A = 135 and 137 in r -process network calculations. Our findings reveal a notable change in the empirical pairing gap for tin isotopes beyond the N = 82 closed shell and a shift in the two-neutron-separation energy slope compared to heavier elements above the shell closure. A new set of ab initio calculations effectively describes these observed trends.}, archive = {J_PRL}, author = {A. Mollaebrahimi and C. Walls and T. Dickel and T. Miyagi and A. Sieverding and C. Andreoiu and J. Ash and B. Ashrafkhani and I. Belosevic and J. Bergman and C. Brown and T. Brunner and J. Cardona and L. Egoriti and G. Gelinas and G. Gwinner and Z. Hockenbery and J. D. Holt and A. Jacobs and S. Kakkar and B. Kootte and J. Lassen and E. M. Lykiardopoulou and S. Malbrunot-Ettenauer and G. Martínez-Pinedo and S. F. Paul and W. R. Plaß and M. P. Reiter and A. Ridley and C. Scheidenberger and R. I. Thompson and Y. Wang and M. E. Wieser and A. A. Kwiatkowski}, doi = {10.1103/ctyj-ls15}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {232701}, shortjournal = {Phys. Rev. Lett.}, title = {Precision mass measurements reveal low neutron pairing in tin beyond n=82 and its impact on stellar nucleosynthesis}, volume = {134}, year = {2025}, }
• (2025). Seniority structure in neutron-rich nucleus ag128: Evidence for robustness of n=82 shell closure in silver isotopes. PRL, 134(23), 232502. (www)

  @article{ , abstract = {The spectroscopic studies of very neutron-rich nucleus have been performed for the first time at the Radioactive Isotope Beam Factory of RIKEN. A new seniority isomer with a half-life of has been identified and is proposed to have a spin-parity of with a maximally aligned configuration comprising three proton holes in the orbital and one neutron hole in the orbital. The new level structure in is quite well described by shell model calculations without invoking excitations across the and shell gaps, and presents a good case of seniority scheme in odd–odd nuclei in the south vicinity of the double-magic nucleus . With a classification of various components of the proton–neutron interaction, the inversion of lowest-lying and states between and its neighboring isotone is found to be dynamically ascribed to the seniority-nonconserving proton–neutron interaction components. The structure above up to the isomer in shows remarkable similarities to seniority structures in the semimagic nuclei and . These spectroscopic features in indicate that the shell closure is still robust in silver isotopes.}, archive = {J_PRL}, author = {D. W. Luo and J. Z. Zhang and Z. H. Li and Y. Y. Cheng and H. Hua and H. Watanabe and G. Lorusso and C. X. Yuan and S. Nishimura and H. Baba and G. Benzoni and F. Browne and K. Y. Chae and Z. Q. Chen and F. C. L. Crespi and P. Doornenbal and N. Fukuda and R. Gernhäuser and G. Gey and C. Y. Guo and N. Inabe and T. Isobe and D. X. Jiang and Y. Jin and H. S. Jung and A. Jungclaus and D. Kameda and G. D. Kim and Y. K. Kim and I. Kojouharov and F. G. Kondev and T. Kubo and N. Kurz and Y. K. Kwon and G. J. Lane and X. Q. Li and J. L. Lou and A. Montaner-Pizá and K. Moschner and F. Naqvi and L. Ni and M. Niikura and H. Nishibata and A. Odahara and R. Orlandi and Z. Patel and Zs. Podolyák and H. Sakurai and H. Schaffner and G. S. Simpson and P.-A. Söderström and K. Steiger and T. Sumikama and H. Suzuki and H. Takeda and J. Taprogge and Zs. Vajta and A. Wendt and H. Y. Wu and J. Wu and C. Xu and Z. Y. Xu and A. Yagi and Y. L. Ye and K. Yoshinaga and S. Q. Zhang and S. Y. Zhang and Z. X. Zhou}, doi = {10.1103/wq9m-trj8}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {232502}, shortjournal = {Phys. Rev. Lett.}, title = {Seniority structure in neutron-rich nucleus ag128: Evidence for robustness of n=82 shell closure in silver isotopes}, volume = {134}, year = {2025}, }
• (2025). Probing the shell effects on fission: The new superheavy nucleus sg257. PRL, 134(23), 232501. (www)

  @article{ , abstract = {Decay properties of the neutron-deficient Sg isotopes were studied at the gas-filled recoil separator TASCA at GSI, Darmstadt by using the reactions. We report on the discovery of the new isotope . Its ground state, tentatively assigned to have [734] configuration, was observed to decay by both spontaneous fission and -particle emission with a half-life of . The alpha decay from this high-spin state was followed by fission of after . In , we observed strong evidence for the occurrence of a -isomeric state for the first time in superheavy nuclei with 106 protons. The current experimental findings, discussed within the experimental systematics and theory, indicate that hitherto unseen features of the shell effect on the fission process may be found in the neutron-deficient superheavy nuclei.}, archive = {J_PRL}, author = {P. Mosat and J. Khuyagbaatar and J. Ballof and R. A. Cantemir and D. Dietzel and Ch. E. Düllmann and K. Hermainski and F. P. Heßberger and E. Jäger and B. Kindler and J. Krier and N. Kurz and B. Lommel and S. Löchner and M. Maiti and T. K. Sato and B. Schausten and J. Uusitalo and P. Wieczorek and A. Yakushev}, doi = {10.1103/s7hr-y7zq}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {232501}, shortjournal = {Phys. Rev. Lett.}, title = {Probing the shell effects on fission: The new superheavy nucleus sg257}, volume = {134}, year = {2025}, }
• (2025). Effective action for relativistic hydrodynamics from the crooks fluctuation theorem. PRL, 134(23), 232302. (www)

  @article{ , abstract = {A new effective theory framework for fluctuating hydrodynamics in the relativistic regime is derived using standard thermodynamical principles and general properties of nonequilibrium stochastic dynamics. For the first time, we establish clear and concise conditions for ensuring that the resulting effective theories are causal, stable, and well-posed within general relativity. These properties are independent of spacetime foliation and are valid in the full nonlinear regime. Out-of-equilibrium fluctuations are constrained by a relativistically covariant version of the Crooks fluctuation theorem, which determines how the entropy production is distributed even when the system is driven by an external force. This leads to an emerging Z 2 symmetry responsible for imposing fluctuation-dissipation relations for n-point correlation functions, which matches the standard constraints for the Schwinger-Keldysh effective action.}, archive = {J_PRL}, author = {Nicki Mullins and Mauricio Hippert and Jorge Noronha}, doi = {10.1103/PhysRevLett.134.232302}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {232302}, shortjournal = {Phys. Rev. Lett.}, title = {Effective action for relativistic hydrodynamics from the crooks fluctuation theorem}, volume = {134}, year = {2025}, }
• (2025). Measurement of in-medium jet modification using direct Photon+Jet and π0+Jet correlations in p+p and central Au+Au collisions at sNN=200 GeV. PRL, 134(23), 232301. (www)

  @article{ , abstract = {The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon ( γ dir ) and neutral-pion ( π 0 ) triggers in p + p and central Au + Au collisions at s N N = 200 GeV over a broad kinematic range, for jet resolution parameters R = 0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for R = 0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The predictions of model calculations incorporating jet quenching are not fully consistent with the observations. These results provide new insight into the physical origins of jet quenching.}, archive = {J_PRL}, author = {STAR Collaboration and B. E. Aboona and J. Adam and L. Adamczyk and I. Aggarwal and M. M. Aggarwal and Z. Ahammed and D. M. Anderson and E. C. Aschenauer and S. Aslam and J. Atchison and V. Bairathi and X. Bao and K. Barish and S. Behera and R. Bellwied and P. Bhagat and A. Bhasin and S. Bhatta and S. R. Bhosale and J. Bielcik and J. Bielcikova and J. D. Brandenburg and C. Broodo and X. Z. Cai and H. Caines and M. Calderón de la Barca Sánchez and D. Cebra and J. Ceska and I. Chakaberia and P. Chaloupka and B. K. Chan and Z. Chang and A. Chatterjee and D. Chen and J. Chen and J. H. Chen and Q. Chen and Z. Chen and J. Cheng and Y. Cheng and W. Christie and X. Chu and S. Corey and H. J. Crawford and M. Csanád and G. Dale-Gau and A. Das and I. M. Deppner and A. Deshpande and A. Dhamija and A. Dimri and P. Dixit and X. Dong and J. L. Drachenberg and E. Duckworth and J. C. Dunlop and J. Engelage and G. Eppley and S. Esumi and O. Evdokimov and O. Eyser and R. Fatemi and S. Fazio and Y. Feng and E. Finch and Y. Fisyak and F. A. Flor and C. Fu and T. Fu and C. A. Gagliardi and T. Galatyuk and T. Gao and F. Geurts and N. Ghimire and A. Gibson and K. Gopal and X. Gou and D. Grosnick and A. Gu and A. Gupta and W. Guryn and A. Hamed and X. Han and S. Harabasz and M. D. Harasty and J. W. Harris and H. Harrison-Smith and L. B. Havener and X. H. He and Y. He and N. Herrmann and L. Holub and C. Hu and Q. Hu and Y. Hu and H. Huang and H. Z. Huang and S. L. Huang and T. Huang and Y. Huang and T. J. Humanic and M. Isshiki and P. M. Jacobs and W. W. Jacobs and A. Jalotra and C. Jena and A. Jentsch and Y. Ji and J. Jia and C. Jin and N. Jindal and X. Ju and E. G. Judd and S. Kabana and D. Kalinkin and K. Kang and D. Kapukchyan and K. Kauder and D. Keane and A. Khanal and Y. V. Khyzhniak and D. P. Kikoła and D. Kincses and I. Kisel and A. Kiselev and A. G. Knospe and H. S. Ko and J. Kołaś and B. Korodi and L. K. Kosarzewski and L. Kumar and M. C. Labonte and R. Lacey and J. M. Landgraf and C. Larson and J. Lauret and A. Lebedev and J. H. Lee and Y. H. Leung and C. Li and D. Li and H-S. Li and H. Li and W. Li and X. Li and Y. Li and Z. Li and X. Liang and Y. Liang and R. Licenik and T. Lin and Y. Lin and M. A. Lisa and C. Liu and G. Liu and H. Liu and L. Liu and X. Liu and Z. Liu and T. Ljubicic and O. Lomicky and R. S. Longacre and E. M. Loyd and T. Lu and J. Luo and X. F. Luo and L. Ma and R. Ma and Y. G. Ma and D. Mallick and R. Manikandhan and S. Margetis and C. Markert and O. Matonoha and O. Mezhanska and K. Mi and S. Mioduszewski and B. Mohanty and B. Mondal and M. M. Mondal and I. Mooney and J. Mrazkova and M. I. Nagy and C. J. Naim and A. S. Nain and J. D. Nam and M. Nasim and H. Nasrulloh and D. Neff and J. M. Nelson and M. Nie and G. Nigmatkulov and T. Niida and T. Nonaka and G. Odyniec and A. Ogawa and S. Oh and K. Okubo and B. S. Page and S. Pal and A. Pandav and A. Panday and A. K. Pandey and T. Pani and A. Paul and S. Paul and D. Pawlowska and C. Perkins and J. Pluta and B. R. Pokhrel and I. D. Ponce Pinto and M. Posik and S. Prodhan and T. L. Protzman and V. Prozorova and N. K. Pruthi and M. Przybycien and J. Putschke and Z. Qin and H. Qiu and S. K. Radhakrishnan and A. Rana and R. L. Ray and R. Reed and C. W. Robertson and M. Robotkova and M. A. Rosales Aguilar and D. Roy and P. Roy Chowdhury and L. Ruan and A. K. Sahoo and N. R. Sahoo and H. Sako and S. Salur and S. S. Sambyal and J. K. Sandhu and S. Sato and B. C. Schaefer and W. B. Schmidke and N. Schmitz and F-J. Seck and J. Seger and R. Seto and P. Seyboth and N. Shah and P. V. Shanmuganathan and T. Shao and M. Sharma and N. Sharma and R. Sharma and S. R. Sharma and A. I. Sheikh and D. Shen and D. Y. Shen and K. Shen and S. Shi and Y. Shi and F. Si and J. Singh and S. Singha and P. Sinha and M. J. Skoby and N. Smirnov and Y. Söhngen and Y. Song and T. D. S. Stanislaus and M. Stefaniak and Y. Su and M. Sumbera and X. Sun and Y. Sun and B. Surrow and M. Svoboda and Z. W. Sweger and A. C. Tamis and A. H. Tang and Z. Tang and T. Tarnowsky and J. H. Thomas and A. R. Timmins and D. Tlusty and T. Todoroki and D. Torres Valladares and S. Trentalange and P. Tribedy and S. K. Tripathy and T. Truhlar and B. A. Trzeciak and O. D. Tsai and C. Y. Tsang and Z. Tu and J. Tyler and T. Ullrich and D. G. Underwood and G. Van Buren and J. Vanek and I. Vassiliev and F. Videbæk and S. A. Voloshin and G. Wang and J. S. Wang and J. Wang and K. Wang and X. Wang and Y. Wang and Z. Wang and A. J. Watroba and J. C. Webb and P. C. Weidenkaff and G. D. Westfall and D. Wielanek and H. Wieman and G. Wilks and S. W. Wissink and R. Witt and J. Wu and X. Wu and B. Xi and Z. G. Xiao and G. Xie and W. Xie and H. Xu and N. Xu and Q. H. Xu and Y. Xu and Z. Xu and G. Yan and Z. Yan and C. Yang and Q. Yang and S. Yang and Y. Yang and Z. Ye and L. Yi and Y. Yu and H. Zbroszczyk and W. Zha and C. Zhang and D. Zhang and J. Zhang and S. Zhang and W. Zhang and X. Zhang and Y. Zhang and Z. Zhang and F. Zhao and J. Zhao and M. Zhao and S. Zhou and Y. Zhou and X. Zhu and M. Zurek and M. Zyzak}, doi = {10.1103/PhysRevLett.134.232301}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {232301}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of in-medium jet modification using direct Photon+Jet and π0+Jet correlations in p+p and central Au+Au collisions at sNN=200 GeV}, volume = {134}, year = {2025}, }
• (2025). Using the w boson as a standard candle to reach the top: Calibrating energy-correlator-based top mass measurements. PRL, 134(23), 231903. (www)

  @article{ , abstract = {The top quark mass is a key parameter of the standard model, yet measuring it precisely at the Large Hadron Collider (LHC) is challenging. Inspired by the use of standard candles in cosmology, we propose a novel energy correlator-based observable, which directly accesses the dimensionless quantity m t / m W . We perform a Monte Carlo study to demonstrate the feasibility of the top mass extraction from Run 2, 3, and High-Luminosity LHC datasets. Our resulting m t can be defined in a well-controlled short-distance mass scheme and exhibits remarkably small uncertainties from nonperturbative effects, as well as insensitivity to parton distribution functions, outlining a roadmap for a record precision measurement at the LHC.}, archive = {J_PRL}, author = {Jack Holguin and Ian Moult and Aditya Pathak and Massimiliano Procura and Robert Schöfbeck and Dennis Schwarz}, doi = {10.1103/j4sp-fcmd}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231903}, shortjournal = {Phys. Rev. Lett.}, title = {Using the w boson as a standard candle to reach the top: Calibrating energy-correlator-based top mass measurements}, volume = {134}, year = {2025}, }
• (2025). New angles on energy correlators. PRL, 134(23), 231902. (www)

  @article{ , abstract = {Energy correlators have recently come to the forefront of jet substructure studies at colliders due to their remarkable properties: they naturally separate physics at different scales, are robust to contamination from soft radiation, and offer a direct connection with quantum field theory. The current parametrization used for energy correlators, however, is based on redundant pairwise angles with complex phase space restrictions. In this Letter, we introduce a new parametrization of energy correlators that features a simpler phase space structure and preserves information about the orientation of jet constituents. Further, our parametrization drastically reduces the computational cost to compute energy correlators on experimental data; whereas the time to compute a traditional projected -point energy correlator scales as on a jet with particles, our new parametrization achieves a scaling of , remarkably independently of . Even for , this improved scaling is particularly important for studies of heavy ion collisions, and higher values of will enable new qualitative understanding of gauge theories. Theoretical calculations for our new energy correlators differ from those of traditional parametrizations only at next-to-next-to-leading logarithmic accuracy and beyond, and we expect that our simpler phase space structure will simplify those calculations. We also discuss how to extend our parametrization to resolved -point energy correlators that encode angular distances between greater numbers of particles, yielding intuitive visualizations of jet substructure that are qualitatively different for different jet samples. We propose two possible generalizations for probing multiprong jets and testing jet scaling behavior.}, archive = {J_PRL}, author = {Samuel Alipour-fard and Ankita Budhraja and Jesse Thaler and Wouter J. Waalewijn}, doi = {10.1103/l6nj-2gsh}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231902}, shortjournal = {Phys. Rev. Lett.}, title = {New angles on energy correlators}, volume = {134}, year = {2025}, }
• (2025). Suppression of spin transfer to Λ hyperon in deep-inelastic scattering. PRL, 134(23), 231901. (www)

  @article{ , abstract = {We investigate production in semi-inclusive deep-inelastic scattering using a polarized lepton beam and find that the spin transfer is significantly suppressed by target fragmentation. As further demonstrated by a model estimation, experimental data can be well described once the target fragmentation is taken into account, which alleviates the tension with calculations solely based on current fragmentation. Our findings suggest that, at the energies of existing fixed-target experiments, the separation of current and target fragmentation regions is not distinct. Spin transfer as well as other spin effects offers a sensitive probe into the origin of the produced hadron.}, archive = {J_PRL}, author = {Xiaoyan Zhao and Zuo-tang Liang and Tianbo Liu and Ya-jin Zhou}, doi = {10.1103/1nd6-9nw9}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231901}, shortjournal = {Phys. Rev. Lett.}, title = {Suppression of spin transfer to Λ hyperon in deep-inelastic scattering}, volume = {134}, year = {2025}, }
• (2025). Observation of collider neutrinos without final state muons with the SND@LHC experiment. PRL, 134(23), 231802. (www)

  @article{ , abstract = {We report the observation of neutrino interactions without final state muons at the LHC, with a significance of 6.4 σ . A dataset of proton-proton collisions at s = 13.6 TeV collected by SND@LHC in 2022 and 2023 is used, corresponding to an integrated luminosity of 68.6 fb − 1 . Neutrino interactions without a reconstructed muon are selected, resulting in an event sample consisting mainly of neutral-current and electron neutrino charged-current interactions in the detector. After selection cuts, 9 neutrino interaction candidate events are observed with an estimated background of 0.32 events.}, archive = {J_PRL}, author = {SND@LHC Collaboration and D. Abbaneo and S. Ahmad and R. Albanese and A. Alexandrov and F. Alicante and K. Androsov and A. Anokhina and T. Asada and C. Asawatangtrakuldee and M. A. Ayala Torres and C. Battilana and A. Bay and A. Bertocco and C. Betancourt and D. Bick and R. Biswas and A. Blanco Castro and V. Boccia and M. Bogomilov and D. Bonacorsi and W. M. Bonivento and P. Bordalo and A. Boyarsky and S. Buontempo and V. Cafaro and M. Campanelli and T. Camporesi and V. Canale and D. Centanni and F. Cerutti and M. Chernyavskiy and K.-Y. Choi and S. Cholak and F. Cindolo and M. Climescu and A. P. Conaboy and A. Crupano and G. M. Dallavalle and D. Davino and P. T. de Bryas and G. De Lellis and M. De Magistris and A. De Roeck and A. De Rújula and M. De Serio and D. De Simone and A. Di Crescenzo and D. Di Ferdinando and C. Dinc and R. Donà and O. Durhan and D. Fasanella and F. Fedotovs and M. Ferrillo and M. Ferro-Luzzi and R. A. Fini and A. Fiorillo and R. Fresa and W. Funk and F. M. Garay Walls and V. Giordano and A. Golovatiuk and A. Golutvin and E. Graverini and A. M. Guler and V. Guliaeva and G. J. Haefeli and C. Hagner and J. C. Helo Herrera and E. van Herwijnen and P. Iengo and S. Ilieva and A. Infantino and A. Iuliano and R. Jacobsson and C. Kamiscioglu and A. M. Kauniskangas and E. Khalikov and S. H. Kim and Y. G. Kim and G. Klioutchnikov and M. Komatsu and N. Konovalova and S. Kuleshov and L. Krzempek and H. M. Lacker and O. Lantwin and F. Lasagni Manghi and A. Lauria and K. Y. Lee and K. S. Lee and V. P. Loschiavo and A. Margiotta and A. Mascellani and F. Mei and A. Miano and A. Mikulenko and M. C. Montesi and F. L. Navarria and W. Nuntiyakul and S. Ogawa and N. Okateva and M. Ovchynnikov and G. Paggi and B. D. Park and A. Pastore and A. Perrotta and D. Podgrudkov and N. Polukhina and F. Primavera and A. Prota and A. Quercia and S. Ramos and A. Reghunath and T. Roganova and F. Ronchetti and T. Rovelli and O. Ruchayskiy and T. Ruf and M. Sabate Gilarte and M. Samoilov and V. Scalera and W. Schmidt-Parzefall and O. Schneider and G. Sekhniaidze and N. Serra and M. Shaposhnikov and V. Shevchenko and T. Shchedrina and L. Shchutska and H. Shibuya and S. Simone and G. Sirri and G. Soares and J. Y. Sohn and O. J. Soto Sandoval and M. Spurio and N. Starkov and J. Steggemann and I. Timiryasov and V. Tioukov and F. Tramontano and C. Trippl and E. Ursov and A. Ustyuzhanin and G. Vankova-Kirilova and G. Vasquez and V. Verguilov and N. Viegas Guerreiro Leonardo and C. Vilela and C. Visone and R. Wanke and E. Yaman and Z. Yang and C. Yazici and C. S. Yoon and E. Zaffaroni and J. Zamora Saa}, doi = {10.1103/r2qy-9hft}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231802}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of collider neutrinos without final state muons with the SND@LHC experiment}, volume = {134}, year = {2025}, }
• (2025). Evidence of coherent elastic neutrino-nucleus scattering with COHERENT’s germanium array. PRL, 134(23), 231801. (www)

  @article{ , abstract = {We report the first detection of coherent elastic neutrino-nucleus scattering (CEvNS) on natural germanium, measured at the Spallation Neutron Source at Oak Ridge National Laboratory. The Ge-Mini detector of the COHERENT collaboration employs large-mass, low-noise, high-purity germanium spectrometers, enabling excellent energy resolution, and an analysis threshold of 1.5 keV electron-equivalent ionization energy. We observe an on-beam excess of 20.6 − 6.3 + 7.1 counts with a total exposure of 10.22 GWhkg, and we reject the no-CEvNS hypothesis with 3.9 σ significance. The result agrees with the predicted standard model of particle physics signal rate within 2 σ .}, archive = {J_PRL}, author = {The COHERENT Collaboration and S. Adamski and M. Ahn and P. S. Barbeau and V. Belov and I. Bernardi and C. Bock and A. Bolozdynya and R. Bouabid and J. Browning and B. Cabrera-Palmer and N. Cedarblade-Jones and A. I. Colón Rivera and E. Conley and V. da Silva and J. Daughhetee and J. Detwiler and K. Ding and M. R. Durand and Y. Efremenko and S. R. Elliott and A. Erlandson and L. Fabris and A. Galindo-Uribarri and M. P. Green and J. Hakenmüller and M. R. Heath and S. Hedges and H. Jeong and B. A. Johnson and T. Johnson and H. Jones and A. Khromov and D. Kim and A. Konovalov and E. Kozlova and A. Kumpan and O. Kyzylova and Y. Lee and G. Li and L. Li and J. M. Link and J. Liu and M. Luxnat and A. Major and K. Mann and D. M. Markoff and J. Mattingly and J. Moye and P. E. Mueller and J. Newby and N. Ogoi and J. O’Reilly and D. S. Parno and D. Pérez-Loureiro and D. Pershey and C. G. Prior and J. Queen and R. Rapp and H. Ray and O. Razuvaeva and D. Reyna and G. C. Rich and D. Rudik and J. Runge and D. J. Salvat and J. Sander and K. Scholberg and A. Shakirov and G. Simakov and W. M. Snow and V. Sosnovtsev and M. Stringer and T. Subedi and B. Suh and B. Sur and R. Tayloe and K. Tellez-Giron-Flores and Y.-T. Tsai and E. E. van Nieuwenhuizen and C. J. Virtue and G. Visser and K. Walkup and E. M. Ward and T. Wongjirad and Y. Yang and J. Yoo and C.-H. Yu and A. Zaalishvili}, doi = {10.1103/PhysRevLett.134.231801}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231801}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence of coherent elastic neutrino-nucleus scattering with COHERENT’s germanium array}, volume = {134}, year = {2025}, }
• (2025). Impediment to torsion from spectral geometry. PRL, 134(23), 231501. (www)

  @article{ , abstract = {Modifications of standard general relativity that bring torsion into the game have a long-standing history. However, no convincing arguments exist for or against its presence in physically acceptable gravity models. In this Letter, we provide an argument based on spectral geometry (using methods of pseudodifferential calculus) that suggests that the torsion shall be excluded from the consideration. We demonstrate that there is no well-defined functional extending to the torsion-full case of the spectral formulation of the Einstein tensor.}, archive = {J_PRL}, author = {Arkadiusz Bochniak and Ludwik Dąbrowski and Andrzej Sitarz and Paweł Zalecki}, doi = {10.1103/drdl-l2mp}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231501}, shortjournal = {Phys. Rev. Lett.}, title = {Impediment to torsion from spectral geometry}, volume = {134}, year = {2025}, }
• (2025). Low energy limit of banks-fischler-shenker-susskind quantum mechanics. PRL, 134(23), 231402. (www)

  @article{ , abstract = {We investigate the low energy regime of BFSS quantum mechanics using its holographic dual. We identify three distinct thermodynamic phases (black holes) and analyze their thermodynamic properties extensively, including phase transitions amongst the several phases. While the properties of the canonical ensemble aligns with existing conjectures on BFSS thermodynamics, we uncover intriguing and unexpected behavior in the microcanonical ensemble. Specifically, for sufficiently low energies, we observe the dominance of the localized phase. Surprisingly, we also identify an energy range where the non-uniform phase becomes dominant. The transition between these phases is mediated by a Kol-type topology-changing phenomenon.}, archive = {J_PRL}, author = {Óscar J. C. Dias and Jorge E. Santos}, doi = {10.1103/wws8-m34w}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231402}, shortjournal = {Phys. Rev. Lett.}, title = {Low energy limit of banks-fischler-shenker-susskind quantum mechanics}, volume = {134}, year = {2025}, }
• (2025). Magnets are weber bar gravitational wave detectors. PRL, 134(23), 231401. (www)

  @article{ , abstract = {When a gravitational wave (GW) passes through a dc magnetic field, it couples to the conducting wires carrying the currents which generate the magnetic field, causing them to oscillate at the GW frequency. The oscillating currents then generate an ac component through which the GW can be detected—thus forming a resonant mass detector or a nagnetic Weber bar. We quantify this claim and demonstrate that magnets can have exceptional sensitivity to GWs over a frequency range demarcated by the mechanical and electromagnetic resonant frequencies of the system; indeed, we outline why a magnetic readout strategy can be considered an optimal Weber bar design. The concept is applicable to a broad class of magnets, but can be particularly well exploited by the powerful magnets being deployed in search of axion dark matter, for example, by DMRadio and ADMX-EFR. Explicitly, we demonstrate that the MRI magnet that is being deployed for ADMX-EFR can achieve a broadband GW strain sensitivity of ∼ 10 − 20 / Hz from a few kHz to about 10 MHz, with a peak sensitivity down to ∼ 10 − 22 / Hz at a kHz exploiting a mechanical resonance.}, archive = {J_PRL}, author = {Valerie Domcke and Sebastian A. R. Ellis and Nicholas L. Rodd}, doi = {10.1103/966v-r5fm}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {231401}, shortjournal = {Phys. Rev. Lett.}, title = {Magnets are weber bar gravitational wave detectors}, volume = {134}, year = {2025}, }
• (2025). Entangling two rydberg superatoms via heralded storage. PRL, 134(23), 230803. (www)

  @article{ , abstract = {Heralded storage of photons is crucial for advancing quantum networks. Previous realizations have primarily relied on single atoms strongly coupled to optical cavities. In this work, we present the experimental realization of heralded storage using a Rydberg superatom, a mesoscopic atomic ensemble operating in the strong blockade regime. In our approach, an input photon is initially stored in the superatom via electromagnetically induced transparency. Subsequently, a second photon is emitted conditioned on the success of the first photon’s storage. Because of the collectively enhanced interaction, both the storage and the emission of the herald photon can be rather efficient in principle. As a demonstration of this technique, we use it to entangle two remote Rydberg superatoms. This method obviates the need for an intermediate node, which is commonly employed in traditional interference-based remote entanglement schemes. Our results showcase the potential of performing cavity-QED-like experiments with Rydberg superatoms. This work opens pathways for numerous applications in quantum networks and linear optical quantum computing.}, archive = {J_PRL}, author = {Zi-Ye An and Bo-Wei Lu and Jun Li and Chao-Wei Yang and Li Li and Xiao-Hui Bao and Jian-Wei Pan}, doi = {10.1103/cmpn-jfqr}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230803}, shortjournal = {Phys. Rev. Lett.}, title = {Entangling two rydberg superatoms via heralded storage}, volume = {134}, year = {2025}, }
• (2025). Enhancing quantum metrology by quantum resonance dynamics. PRL, 134(23), 230802. (www)

  @article{ , abstract = {Quantum effects in metrology can in principle enhance measurement precision from the so-called standard quantum limit to the Heisenberg limit. Further advancements in quantum metrology largely rely on innovative metrology protocols that can avoid a number of known obstacles, including the challenge of preparing entangled states with sufficient fidelity, the readout noise in measuring highly entangled states, and no-go theorems for quantum metrology under noisy environments. In this Letter, exploiting some peculiar but experimentally feasible dynamical features of a collection of spins with all-to-all time-periodic interactions, we propose a metrology protocol that can circumvent all three mentioned obstacles and yet still make good use of time as a resource for metrology. Specifically, by mapping the dynamics of such a periodically driven spin system to that of a paradigm of quantum chaos but tuned to some high-order quantum resonance, it is shown that a simple SU(2) coherent state can, after evolving to highly entangled states in the ensuing dynamics, be dynamically brought back to the same initial coherent state. The associated quantum Fisher information is found to exhibit quadratic scaling with both the number of spins and the duration of the metrology protocol. The achieved Heisenberg scaling can also largely survive in the presence of Markovian noise. Representing a previously unknown strategy for quantum metrology, the protocol proposed here can be tested on available experimental platforms.}, archive = {J_PRL}, author = {Zhixing Zou and Jiangbin Gong and Weitao Chen}, doi = {10.1103/lkrt-lvng}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230802}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing quantum metrology by quantum resonance dynamics}, volume = {134}, year = {2025}, }
• (2025). Ultrabright entanglement based quantum key distribution over a 404 km optical fiber. PRL, 134(23), 230801. (www)

  @article{ , abstract = {Entangled photons are crucial resources for quantum information processing. Here, we present an ultrabright polarization-entangled photon source based on a periodically poled lithium niobate waveguide designed for practical quantum communication networks. Using a 780 nm pump laser, the source achieves a pair generation rate of 2.4 × 10 10 pairs / s / mW . Remarkably, the entangled photons are bright enough to be detected by a power meter, reaching a power of 17.9 nW under a pump power of 3.2 mW. We demonstrate the practicality of the source by conducting quantum key distribution experiments over long-distance fiber links. Wavelength-division multiplexing was employed to enhance the key generation, and nonlocal dispersion compensation was implemented to ensure precise timing coincidence measurements across a broad spectral range. By utilizing nine pairs of wavelength channels, the system achieved the applicable secure key rates of up to 440.80 bits / s over 200 km with a 62 dB loss and extended the maximum secure key generation distance to 404 km. These results demonstrate the potential of wavelength-multiplexed polarization-entangled photon sources for high-speed, long-distance quantum communication, positioning them as key components for future large-scale quantum networks.}, archive = {J_PRL}, author = {Shi-Chang Zhuang and Bo Li and Ming-Yang Zheng and Yi-Xi Zeng and Hui-Nan Wu and Guang-Bing Li and Quan Yao and Xiu-Ping Xie and Yu-Huai Li and Hao Qin and Li-Xing You and Feihu Xu and Juan Yin and Yuan Cao and Qiang Zhang and Cheng-Zhi Peng and Jian-Wei Pan}, doi = {10.1103/PhysRevLett.134.230801}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230801}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrabright entanglement based quantum key distribution over a 404 km optical fiber}, volume = {134}, year = {2025}, }
• (2025). Single-qubit gates with errors at the 10−7 level. PRL, 134(23), 230601. (www)

  @article{ , abstract = {We report the achievement of single-qubit gates with sub-part-per-million error rates, in a trapped-ion hyperfine clock qubit. We explore the speed and fidelity trade-off for gate times , and benchmark a minimum error per Clifford gate of . Calibration errors are suppressed to , leaving qubit decoherence ( ), leakage, and measurement as the dominant error contributions. The ion is held above a microfabricated surface-electrode trap that incorporates a chip-integrated microwave resonator for electronic qubit control; the trap is operated at room temperature without magnetic shielding.}, archive = {J_PRL}, author = {M. C. Smith and A. D. Leu and K. Miyanishi and M. F. Gely and D. M. Lucas}, doi = {10.1103/42w2-6ccy}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230601}, shortjournal = {Phys. Rev. Lett.}, title = {Single-qubit gates with errors at the 10−7 level}, volume = {134}, year = {2025}, }
• (2025). Emergent equilibrium in all-optical single quantum-trajectory ising machines. PRL, 134(23), 230404. (www)

  @article{ , abstract = {We investigate the dynamics of multimode optical systems driven by two-photon processes and subject to nonlocal losses, incorporating quantum noise at the Gaussian level. Our findings show that the statistics retrieved from a single Gaussian quantum trajectory exhibits emergent thermal equilibrium governed by an Ising Hamiltonian, encoded in the dissipative coupling between modes. The system’s effective temperature is set by the driving strength relative to the oscillation threshold. Given the ultrashort timescales typical of all-optical devices, our Letter demonstrates that such multimode optical systems can operate as ultrafast Boltzmann samplers, paving the way toward the realization of efficient hardware for combinatorial optimization, with promising applications in machine learning and beyond.}, archive = {J_PRL}, author = {Jacopo Tosca and Marcello Calvanese Strinati and Claudio Conti and Cristiano Ciuti}, doi = {10.1103/fk9d-k8dc}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230404}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent equilibrium in all-optical single quantum-trajectory ising machines}, volume = {134}, year = {2025}, }
• (2025). Space-time correlations in monitored kinetically constrained discrete-time quantum dynamics. PRL, 134(23), 230403. (www)

  @article{ , abstract = {State-of-the-art quantum simulators permit local temporal control of interactions and midcircuit readout. These capabilities open the way toward the exploration of intriguing nonequilibrium phenomena. We illustrate this with a kinetically constrained many-body quantum system that has a natural implementation on Rydberg quantum simulators. The evolution proceeds in discrete time and is generated by repeatedly entangling the system with an auxiliary environment that is monitored and reset after each time step. Despite featuring an uncorrelated infinite-temperature average stationary state, the dynamics displays coexistence of fast and slow space-time regions in stochastic realizations of the system state. The time record of measurement outcomes on the environment serves as natural probe for such dynamical heterogeneity, which we characterize using tools from large deviation theory. Our Letter establishes the large deviation framework for discrete-time open quantum many-body systems as a means to characterize complex dynamics and collective phenomena in quantum processors and simulators.}, archive = {J_PRL}, author = {Marcel Cech and María Cea and Mari Carmen Bañuls and Igor Lesanovsky and Federico Carollo}, doi = {10.1103/2lxs-wccj}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230403}, shortjournal = {Phys. Rev. Lett.}, title = {Space-time correlations in monitored kinetically constrained discrete-time quantum dynamics}, volume = {134}, year = {2025}, }
• (2025). Entanglement patterns of quantum chaotic hamiltonians with a scalar u(1) charge. PRL, 134(23), 230402. (www)

  @article{ , abstract = {Our current understanding of quantum chaos in many-body quantum systems hinges on the random matrix theory (RMT) behavior of eigenstates and their energy level statistics. Although RMT has been remarkably successful in describing “coarse” features of many-body quantum Hamiltonians in chaotic regimes, such as the Wigner-Dyson level spacing statistics or the volume-law behavior of eigenstate entanglement entropy, it remains a challenge to describe their “finer” features, particularly those arising from spatial locality. Here, we show that we can accurately describe the statistical behavior of eigenstate ensembles in many-body Hamiltonians by using pure random states with physical constraints that capture the essential features of the Hamiltonian, specifically spatial locality and symmetries. We demonstrate our approach on local spin Hamiltonians with a scalar U(1) charge. By constructing ensembles of constrained random states that account for two commuting scalar charges playing the role of energy and magnetization, we describe the patterns of entanglement of midspectrum eigenstates beyond their average volume-law behavior, including corrections and fluctuations, analytically and numerically. When defining the correspondence between quantum chaotic eigenstates in many-body Hamiltonians and RMT ensembles, our work highlights the important role played by spatial locality in describing universal features beyond the volume-law behavior.}, archive = {J_PRL}, author = {Christopher M. Langlett and Joaquin F. Rodriguez-Nieva}, doi = {10.1103/xxlq-d1sw}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230402}, shortjournal = {Phys. Rev. Lett.}, title = {Entanglement patterns of quantum chaotic hamiltonians with a scalar u(1) charge}, volume = {134}, year = {2025}, }
• (2025). Emergence of navier-stokes hydrodynamics in chaotic quantum circuits. PRL, 134(23), 230401. (www)

  @article{ , abstract = {We construct an ensemble of two-dimensional nonintegrable quantum circuits that are chaotic but have a conserved particle current, and thus a finite Drude weight. The long-wavelength hydrodynamics of such systems is given by the incompressible Navier-Stokes equations. By analyzing circuit-to-circuit fluctuations in the ensemble we argue that these are negligible, so the circuit-averaged value of transport coefficients like the viscosity is also (in the long-time limit) the value in a typical circuit. The circuit-averaged transport coefficients can be mapped onto a classical irreversible Markov process. Therefore, remarkably, our construction allows us to efficiently compute the viscosity of a family of strongly interacting chaotic two-dimensional quantum systems.}, archive = {J_PRL}, author = {Hansveer Singh and Ewan McCulloch and Sarang Gopalakrishnan and Romain Vasseur}, doi = {10.1103/z9ym-kqln}, journal = {Physical Review Letters}, month = {6}, number = {23}, pages = {230401}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of navier-stokes hydrodynamics in chaotic quantum circuits}, volume = {134}, year = {2025}, }
• (2025). Erratum: Next-to-next-to-leading-order QCD corrections to pion electromagnetic form factors [Phys. rev. lett. 132, 201901 (2024)]. PRL, 134(22), 229901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 229901 (2025)}, archive = {J_PRL}, author = {L. B. Chen and W. Chen and F. Feng and Y. Jia}, doi = {10.1103/pl5b-blv5}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {229901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Next-to-next-to-leading-order QCD corrections to pion electromagnetic form factors [Phys. rev. lett. 132, 201901 (2024)]}, volume = {134}, year = {2025}, }
• (2025). Mechanics of poking a cyst. PRL, 134(22), 228402. (www)

  @article{ , abstract = {Indentation tests are classical tools to determine material properties. For biological samples such as cysts of cells, however, the observed force-displacement relation cannot be expected to follow predictions for simple materials. Here, by solving the Pogorelov problem of a point force indenting an elastic shell for a purely nonlinear material, we discover that complex material behavior can even give rise to new scaling exponents in this force-displacement relation. In finite-element simulations, we show that these exponents are surprisingly robust, persisting even for thick shells indented with a sphere. By scaling arguments, we generalize our results to pressurized and prestressed shells, uncovering additional new scaling exponents. We find these predicted scaling exponents in the force-displacement relation observed in cyst indentation experiments. Our results thus form the basis for inferring the mechanisms that set the mechanical properties of these biological materials.}, archive = {J_PRL}, author = {Shiheng Zhao (赵世恒 and Pierre A. Haas}, doi = {10.1103/PhysRevLett.134.228402}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {228402}, shortjournal = {Phys. Rev. Lett.}, title = {Mechanics of poking a cyst}, volume = {134}, year = {2025}, }
• (2025). Universal model for ion transport: Bridging the goldman-hodgkin-katz paradigm with reverse electrodialysis. PRL, 134(22), 228401. (www)

  @article{ , abstract = {The Goldman-Hodgkin-Katz (GHK) theory has been the paradigm for ion transport in physiological systems for the past century. However, GHK incorrectly assumes a uniform electrical field, leading to several inconsistencies. We propose a new theory developed using methods from the reverse-electrodialysis (RED) community. Our theory, substantiated by simulations, provides expressions for all the main characteristics of ion transport and connects GHK to RED, providing a remarkably robust framework for (re-)interpreting ion transport experiments in any (living or inanimate) charge-selective system.}, archive = {J_PRL}, author = {Yoav Green}, doi = {10.1103/kf5h-wtlb}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {228401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal model for ion transport: Bridging the goldman-hodgkin-katz paradigm with reverse electrodialysis}, volume = {134}, year = {2025}, }
• (2025). Not-so-glass-like caging and fluctuations of an active matter model. PRL, 134(22), 228301. (www)

  @article{ , abstract = {Simple active models of matter recapitulate complex biological phenomena. The out-of-equilibrium nature of these models, however, often makes them beyond the reach of first-principle descriptions. This limitation is particularly perplexing when attempting to distinguish between different glass-forming mechanisms. We here consider a minimal active system in various spatial dimensions to identify the processes underlying their sluggish dynamics. Activity is found to markedly impact cage escape processes and critical fluctuations associated with exploring lower-dimensional caging features.}, archive = {J_PRL}, author = {Mingyuan Zheng and Dmytro Khomenko and Patrick Charbonneau}, doi = {10.1103/PhysRevLett.134.228301}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {228301}, shortjournal = {Phys. Rev. Lett.}, title = {Not-so-glass-like caging and fluctuations of an active matter model}, volume = {134}, year = {2025}, }
• (2025). Emergence of intermediate range order in jammed packings. PRL, 134(22), 228201. (www)

  @article{ , abstract = {We perform a structural analysis of large scale jammed packings of monodisperse, frictionless and frictional spheres to elucidate structural signatures of the static structure factor in the low-to-intermediate wave number region. We employ discrete element method simulations containing up to 8 × 10 7 particles, in which the particle friction coefficient(s), including sliding, rolling, and twisting interactions, are varied. At intermediate wave number values, corresponding to length scales that lie between that of the nearest neighbor primary peak and the system size, we find the emergence of a prepeak—a signature of intermediate range order—that grows with increasing friction. We correlate the emergence of this peak to real space fluctuations in the local particle coordination number, which exhibits a grainy fluctuating field throughout the packing process that is retained in the final, mechanically stable state. While the formation of the prepeak shows varying degrees of robustness to packing protocol changes, our results suggest that preparation history may be used to construct packings with variable large length scale structural properties.}, archive = {J_PRL}, author = {Joseph M. Monti and Ishan Srivastava and Leonardo E. Silbert and A. P. Santos and Joel T. Clemmer and Jeremy B. Lechman and Gary S. Grest}, doi = {10.1103/PhysRevLett.134.228201}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {228201}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of intermediate range order in jammed packings}, volume = {134}, year = {2025}, }
• (2025). Radiative stabilization of the indenyl cation: Recurrent fluorescence in a closed-shell polycyclic aromatic hydrocarbon. PRL, 134(22), 228002. (www)

  @article{ , abstract = {Several small polycyclic aromatic hydrocarbons (PAHs) with closed-shell electronic structure have been identified in the cold, dark environment Taurus Molecular Cloud 1. We measure efficient radiative cooling through the combination of recurrent fluorescence (RF) and IR emission in the closed-shell indenyl cation ( C 9 H 7 + ), finding good agreement with a master equation model including molecular dynamics trajectories to describe internal-energy-dependent properties for RF. We find that C 9 H 7 + formed with up to E c = 5.85 eV vibrational energy, which is ≈ 2 eV above the dissociation threshold, radiatively cool rather than dissociate. The efficient radiative stabilization dynamics are likely common to other closed-shell PAHs present in space, contributing to their abundance.}, archive = {J_PRL}, author = {James N. Bull and Arun Subramani and Chang Liu and Samuel J. P. Marlton and Eleanor K. Ashworth and Henrik Cederquist and Henning Zettergren and Mark H. Stockett}, doi = {10.1103/PhysRevLett.134.228002}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {228002}, shortjournal = {Phys. Rev. Lett.}, title = {Radiative stabilization of the indenyl cation: Recurrent fluorescence in a closed-shell polycyclic aromatic hydrocarbon}, volume = {134}, year = {2025}, }
• (2025). State-specific density functionals for excited states via a density-driven correlation model. PRL, 134(22), 228001. (www)

  @article{ , abstract = {We present a first principles strategy for developing approximations for excited states through ensemble density functionals. Central to our result is the recognition that density-driven correlations (ddc’s) can be vitally important to address excited states individually through ensembles, yet standard density-functional approximations based on ground state physics miss ddc’s altogether. To model the ddc, we exploit the recently understood low-density limit of electrons in excited states. The theory developments are then combined to produce a proof-of-concept excited state approximation that resolves urgent paradigmatic failures (double excitations, charge transfer excitations, piecewise linearity) of existing state-of-art density-functional approaches, directly from differences in self-consistent field calculations; i.e., Δ SCF . In light of its observed impressive performance, we conclude that the approach represents a major step toward unified and accurate modeling of neutral and charged excitations.}, archive = {J_PRL}, author = {Tim Gould and Stephen G. Dale and Leeor Kronik and Stefano Pittalis}, doi = {10.1103/PhysRevLett.134.228001}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {228001}, shortjournal = {Phys. Rev. Lett.}, title = {State-specific density functionals for excited states via a density-driven correlation model}, volume = {134}, year = {2025}, }
• (2025). Kinetic energy diffusivity and scaling velocity correlation functions. PRL, 134(22), 227103. (www)

  @article{ , abstract = {We propose a Green-Kubo-like relation for kinetic energy diffusivity to investigate the interplay between ergodicity and anomalous diffusion. This approach introduces a fluctuation metric for the time-averaged kinetic energy, which holds for scaling velocity correlation functions. We demonstrate that as stationary diffusive systems transition into an effective ergodic phase, their kinetic energy metric converges to a universal law. This finding provides a robust framework for understanding the dynamics of such systems. Applications to protein folding and single-particle tracking illustrate the practical utility of our approach, offering a clear prescription for extracting key physical parameters, such as the friction constant and relaxation time, from finite experimental datasets. Importantly, this method remains effective even when the underlying processes exhibit weak ergodicity breaking or are bounded. Furthermore, we explore the nonergodic transition associated with the aging velocity correlation function observed in granular gases.}, archive = {J_PRL}, author = {Jing-Dong Bao and Fabio Marchesoni}, doi = {10.1103/fmbw-9j8w}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {227103}, shortjournal = {Phys. Rev. Lett.}, title = {Kinetic energy diffusivity and scaling velocity correlation functions}, volume = {134}, year = {2025}, }
• (2025). Visitation dynamics of d-dimensional fractional brownian motion. PRL, 134(22), 227102. (www)

  @article{ , abstract = {The fractional Brownian motion (fBm) is a paradigmatic strongly non-Markovian process with broad applications in various fields. Despite their importance, the properties of the territory covered by a d -dimensional fBm have remained elusive so far. Here, we study the visitation dynamics of the fBm by considering the time τ n required to visit a site, defined as a unit cell of a d -dimensional lattice, when n sites have been visited. Relying on scaling arguments, we determine all temporal regimes of the probability distribution function of τ n . These results are confirmed by extensive numerical simulations that employ large deviation Monte Carlo algorithms. Besides these theoretical aspects, our results account for the tracking data of telomeres in the nucleus of mammalian cells, microspheres in an agorose gel, and vacuoles in the amoeba, which are experimental realizations of fBm.}, archive = {J_PRL}, author = {Léo Régnier and Maxim Dolgushev and Olivier Bénichou}, doi = {10.1103/PhysRevLett.134.227102}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {227102}, shortjournal = {Phys. Rev. Lett.}, title = {Visitation dynamics of d-dimensional fractional brownian motion}, volume = {134}, year = {2025}, }
• (2025). Experimental realization of an analog of entanglement between two brownian particles. PRL, 134(22), 227101. (www)

  @article{ , abstract = {We experimentally investigate the statistical properties of a classical analog of quantum entanglement between two Brownian particles connected by an elastic force and maintained at different temperatures through separate heat reservoirs. Uncertainty relations between coordinates and coarse-grained velocity can produce a phenomenon similar to quantum entanglement, where temperature plays the role of Planck’s constant. The theoretical analysis matches the experimental results, confirming that the interconnected particles exhibit Brownian quantum-inspired classical correlation entanglement. This effect arises from a coarse-grained description of Brownian motion and vanishes at a finer resolution. The coarsening scale range is measured too.}, archive = {J_PRL}, author = {Theerthagiri L and S. Ciliberto}, doi = {10.1103/PhysRevLett.134.227101}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {227101}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental realization of an analog of entanglement between two brownian particles}, volume = {134}, year = {2025}, }
• (2025). Theory of the photonic joule effect in superconducting circuits. PRL, 134(22), 227001. (www)

  @article{ , abstract = {When a small system is coupled to a bath, it is generally assumed that the state of the bath remains unaffected by the system due to the bath’s large number of degrees of freedom. Here, we show theoretically that this assumption can be easily violated for photonic baths typically used in experiments involving superconducting circuits. We analyze the dynamics of a voltage-biased Josephson junction coupled to a photonic bath, represented as a long Josephson junction chain. Our findings show that the system can reach a nonequilibrium steady state where the photonic degrees of freedom become significantly overheated, leading to a qualitative change in the current-voltage I – V curve. This phenomenon is analogous to the Joule effect observed in electrical conductors, where flowing current can substantially heat up electrons. Recognizing this effect is crucial for the many applications of high-impedance environments in quantum technologies.}, archive = {J_PRL}, author = {Samuel Cailleaux and Quentin Ficheux and Nicolas Roch and Denis M. Basko}, doi = {10.1103/b9hw-b6y6}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {227001}, shortjournal = {Phys. Rev. Lett.}, title = {Theory of the photonic joule effect in superconducting circuits}, volume = {134}, year = {2025}, }
• (2025). Testing the tomographic fermi liquid hypothesis with high-order cyclotron resonance. PRL, 134(22), 226902. (www)

  @article{ , abstract = {The tomographic Fermi liquid (TFL) hypothesis posits starkly different relaxation times for odd and even angular harmonics of electron distribution function in two-dimensional systems, but its experimental verification remains elusive. Traditional electrical transport struggles to discern these lifetimes, as resistivity is largely unaffected by electron scattering. Here, we demonstrate that high-order cyclotron resonance (CR) offers a direct probe: The linewidth of the th CR peak directly reflects the relaxation rate of the corresponding angular harmonic. Combining theory and terahertz photoconductivity measurements in graphene, we show that the third-order CR exhibits a narrower linewidth than the second-order CR, yielding . This hierarchy defies conventional impurity or phonon scattering models, instead aligning with TFL predictions where odd harmonics evade relaxation via head-on collisions. Our results provide definitive evidence for the TFL regime and establish high-order CR as a powerful tool to unravel hydrodynamic transport in quantum materials.}, archive = {J_PRL}, author = {Ilia Moiseenko and Erwin Mönch and Kirill Kapralov and Denis Bandurin and Sergey Ganichev and Dmitry Svintsov}, doi = {10.1103/zq1g-8d4s}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226902}, shortjournal = {Phys. Rev. Lett.}, title = {Testing the tomographic fermi liquid hypothesis with high-order cyclotron resonance}, volume = {134}, year = {2025}, }
• (2025). Silicon plasmonics for enhanced responsivity of silicon photodetectors in deep-ultraviolet region. PRL, 134(22), 226901. (www)

  @article{ , abstract = {We report on the utilization of Si in plasmonics research, specifically targeting deep ultraviolet (DUV) applications. By incorporating periodic submicron gratings on a Si surface, we demonstrate a photoconductive Si detector with significantly enhanced responsivity to DUV light, which is achieved via surface plasmon resonance (SPR). Notably, even without a metal, the detector exhibits improved responsivity only under TM-polarized light, supporting the interpretation that Si excites SPR. Our demonstration not only validates the effectiveness of Si plasmonics for enhancing photodetector performance but also introduces innovative techniques with potential applications in various research fields.}, archive = {J_PRL}, author = {Yu-ichiro Tanaka and Atsushi Ono and Wataru Inami and Yoshimasa Kawata}, doi = {10.1103/PhysRevLett.134.226901}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226901}, shortjournal = {Phys. Rev. Lett.}, title = {Silicon plasmonics for enhanced responsivity of silicon photodetectors in deep-ultraviolet region}, volume = {134}, year = {2025}, }
• (2025). Universal theoretical elucidation of electrobending deformation in piezoelectrics. PRL, 134(22), 226801. (www)

  @article{ , abstract = {The origin of frequently observed ultrahigh electro-induced longitudinal strain, ranging from 1% to 26%, remains an open question. While recent studies have associated this phenomenon with bending deformation, the underlying mechanisms and the pronounced thickness dependence of the nominal strain have yet to be fully elucidated. Here, we demonstrate that the bending in piezoelectrics can be induced by a nonzero gradient of across thickness direction. A scaling law ( ) is derived to quantify the size dependence, thereby resolving longstanding ambiguities surrounding reported “giant” electrostrains. Simulations reveal that in standard perovskite piezoceramics, such as , a 0.69% concentration of oxygen vacancies can induce a variation in by suppressing polarization rotation, being sufficient to produce ultrahigh nominal strain in thin samples. Numerous factors, including gradients in defect concentration, composition, and stress, may lead to sufficient inhomogeneity in the distribution of , suggesting electrobending may be a widespread phenomenon. This Letter presents a unified framework for understanding electrobending deformation, offering deeper insight into the mechanisms behind abnormally giant electrostrain responses in diverse piezoelectric systems and may encourage new engineering applications.}, archive = {J_PRL}, author = {Zhi Tan and Xiang Lv and Laiming Jiang and Xing Huang and Jie Xing and Shaoxiong Xie and Hui Zhang and Jianguo Zhu}, doi = {10.1103/f9y4-lh2m}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226801}, shortjournal = {Phys. Rev. Lett.}, title = {Universal theoretical elucidation of electrobending deformation in piezoelectrics}, volume = {134}, year = {2025}, }
• (2025). Tunable bifurcation of magnetic anisotropy and bi-oriented antiferromagnetic order in kagome metal GdTi3Bi4. PRL, 134(22), 226704. (www)

  @article{ , abstract = {The novel kagome family ( : rare-earth metals) offers a unique platform for exploring distinctive physical phenomena such as anisotropy, spin density wave, and anomalous Hall effect. In particular, the magnetic frustration and behavior of magnetic anisotropy in antiferromagnetic (AFM) kagome materials are of great interest for the fundamental studies and hold promise for next-generation device applications. Here, we report a tunable bifurcation of magnetic anisotropic and bi-oriented AFM order observed in the quasi-1D kagome antiferromagnet . The magnetic domain evolutions during two plateau transition processes are directly visualized, unveiling a pronounced in-plane anisotropy along the axis. Temperature-dependent characterization reveals a bifurcation transition of anisotropy at approximately 2 K, where the -axis anisotropy splits into two special orientations, revealing a hidden bi-oriented in-plane AFM order that deviates from the high-symmetry direction by . More intriguingly, the characteristics of the bifurcated anisotropy are clearly illustrated through vector magnetic field modulation, revealing three distinct in-plane domain phases in the transverse magnetic field phase diagram. Our results not only provide valuable insights into the tunable bifurcation of magnetic anisotropic in , but also pave a novel pathway for AFM spintronics development.}, archive = {J_PRL}, author = {Jianfeng Guo and Shiyu Zhu and Runnong Zhou and Ruwen Wang and Yunhao Wang and Jianping Sun and Zhen Zhao and Xiaoli Dong and Jinguang Cheng and Haitao Yang and Jiang Xiao and Hong-Jun Gao}, doi = {10.1103/mryp-krmp}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226704}, shortjournal = {Phys. Rev. Lett.}, title = {Tunable bifurcation of magnetic anisotropy and bi-oriented antiferromagnetic order in kagome metal GdTi3Bi4}, volume = {134}, year = {2025}, }
• (2025). Multiferroic collinear antiferromagnets with hidden altermagnetic spin splitting. PRL, 134(22), 226703. (www)

  @article{ , abstract = {Altermagnets exhibit nonrelativistic spin splitting due to the breaking of time-reversal symmetry and have been garnering significant attention as promising materials for spintronic applications. In contrast, conventional antiferromagnets without spin splitting seem to not have any symmetry breaking and have drawn less attention. However, we show that conventional antiferromagnets with a nonzero propagation vector ( Q vector) bring about nontrivial symmetry breakings. The incompatibility between the Q vector and nonsymmorphic symmetry leads to macroscopic symmetry breaking without lifting spin degeneracy. Moreover, the hidden altermagnetic spin splitting in the electronic structure gives rise to various emergent responses. To examine our prediction, we perform first-principles calculations for MnS 2 and investigate its multiferroic properties, such as nonlinear transport and optical activity. Our findings reveal unique properties in conventional antiferromagnets, providing another perspective for designing spintronic materials.}, archive = {J_PRL}, author = {Jin Matsuda and Hikaru Watanabe and Ryotaro Arita}, doi = {10.1103/vgcs-bn8g}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226703}, shortjournal = {Phys. Rev. Lett.}, title = {Multiferroic collinear antiferromagnets with hidden altermagnetic spin splitting}, volume = {134}, year = {2025}, }
• (2025). Absence of altermagnetic magnon band splitting in MnF2. PRL, 134(22), 226702. (www)

  @article{ , abstract = {Altermagnets are collinear compensated magnets in which the magnetic sublattices are related by rotation rather than translation or inversion. One of the quintessential properties of altermagnets is the presence of split chiral magnon modes. Recently, such modes have been predicted in MnF 2 . Here, we report inelastic neutron scattering results on an MnF 2 single crystal along high-symmetry Brillouin zone paths for which the magnon splitting is expected. Within the resolution of our measurement, we do not observe the predicted splitting. The inelastic spectrum is well modeled using J 1 , J 2 , J 3 nearest-neighbor exchange interactions with weak uniaxial anisotropy. These interactions have higher symmetry than the crystal lattice, while the interactions predicted to produce the altermagnetic splitting are negligibly small. Therefore, the two magnon modes appear to be degenerate over the entire Brillouin zone and the spin dynamics of MnF 2 is indistinguishable from a classical Néel antiferromagnet. Application of a magnetic field causes a Zeeman splitting of the magnon modes close to the Γ point. Even if chiral magnon modes are allowed by altermagnetic symmetry, the splitting in real materials such as MnF 2 can be negligibly small.}, archive = {J_PRL}, author = {V. C. Morano and Z. Maesen and S. E. Nikitin and J. Lass and D. G. Mazzone and O. Zaharko}, doi = {10.1103/PhysRevLett.134.226702}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226702}, shortjournal = {Phys. Rev. Lett.}, title = {Absence of altermagnetic magnon band splitting in MnF2}, volume = {134}, year = {2025}, }
• (2025). Origin of the hidden energy scale and the f ratio in geometrically frustrated magnets. PRL, 134(22), 226701. (www)

  @article{ , abstract = {Sufficiently clean geometrically frustrated (GF) magnets are the largest class of candidate materials that may host quantum spin liquids (QSLs). Some of them have been shown to exhibit spin-glass freezing, potentially precluding QSLs, at the “hidden energy scale,” which is significantly lower than the microscopic energy scale of spin interactions. Here, we investigate the origin of the hidden energy scale and its relationship to the f ratio, the figure of merit for the degree of frustration in GF magnetic materials. The available experimental and numerical data provide evidence that GF magnets display, universally, two distinct temperature scales in the specific heat, the lowest of which is of the order of the hidden energy scale T * . We argue that this scale is determined by nonmagnetic excitations, similar to spin exchanges in chains of spins. The collective entropy of such excitations matches the entropy of the ground states of the Ising model on the same lattice, which provides a way to verify the proposed scenario in experiment. We demonstrate that in the presence of quenched disorder, a broad class of materials exhibits spin-glass freezing at temperatures of order T * , in accordance with experimental observations. As T * is a property of the clean GF medium, it leads to a constraint on the f ratio.}, archive = {J_PRL}, author = {Phillip Popp and Arthur P. Ramirez and Sergey Syzranov}, doi = {10.1103/PhysRevLett.134.226701}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226701}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of the hidden energy scale and the f ratio in geometrically frustrated magnets}, volume = {134}, year = {2025}, }
• (2025). Topological domain-wall pump with z2 spontaneous symmetry breaking. PRL, 134(22), 226603. (www)

  @article{ , abstract = {A domain-wall pump by an extended cluster model of spins is proposed with local U(1) gauge invariance. In contrast to the conventional pump, the current and the gauge field are defined on sites instead of links. Its snapshot ground state is gapped and doubly degenerated due to invariance, which is broken by an infinitesimal boundary magnetic field. The ground state associated with the spontaneous symmetry breaking is, at the same time, symmetry-protected with additional spatial inversion that is characterized by the Berry phase defined by the twist on the boundary site. We investigate the topological domain-wall pump with and without boundaries. The topological pump associated with the inversion symmetry-breaking path induces a nontrivial Chern number of bulk and a singular behavior of edge states of the domain wall. Generalization to the multispin interaction is also explicitly given. These extended quantum degrees of freedom are prominent qubits that are topologically protected.}, archive = {J_PRL}, author = {Yoshihito Kuno and Yasuhiro Hatsugai}, doi = {10.1103/PhysRevLett.134.226603}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226603}, shortjournal = {Phys. Rev. Lett.}, title = {Topological domain-wall pump with z2 spontaneous symmetry breaking}, volume = {134}, year = {2025}, }
• (2025). Exceptional magic angles in non-hermitian twisted bilayer graphene. PRL, 134(22), 226602. (www)

  @article{ , abstract = {Twisted bilayer graphene (TBG) features strongly correlated and topological phases due to its flat bands emerging near the magic angle. However, the effects of the non-Hermiticity, arising from the coupling to the environment and dissipation, have remained unexplored. We here develop a simple non-Hermitian (NH) version of twisted bilayer graphene (TBG) by considering relative twisting of two NH graphene monolayers with non-Hermiticity encoded in the imbalance of in-plane nearest-neighbor hopping amplitudes. Remarkably, by generalizing the Bistritzer-MacDonald approach to NH systems, we discover exceptional magic angles where the band structure changes from purely real to purely imaginary thus featuring flat bands with infinite lifetime. Between them, the bands remain flattened, and a Hermitian magic angle emerges at which the imaginary part of energy is maximal, and corresponds to the usual magic angle in nondissipative, purely Hermitian TBG. We propose an optical lattice setup with gain and loss where our theoretical predictions can be verified. These results suggest the robustness of the flat bands in open systems, paving the way for the further studies on the interplay of dissipative effects, electronic topology, and interactions in such NH moiré bands.}, archive = {J_PRL}, author = {Juan Pablo Esparza and Vladimir Juričić}, doi = {10.1103/dl59-vl7v}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226602}, shortjournal = {Phys. Rev. Lett.}, title = {Exceptional magic angles in non-hermitian twisted bilayer graphene}, volume = {134}, year = {2025}, }
• (2025). Intrinsic axion statistical topological insulator. PRL, 134(22), 226601. (www)

  @article{ , abstract = {Ensembles that respect symmetries on average exhibit richer topological states than those in pure states with exact symmetries, leading to the concept of average symmetry-protected topological states (ASPTs). The free-fermion counterpart of ASPT is the so-called statistical topological insulator (STI) in disordered ensembles. In this Letter, we demonstrate the existence of an intrinsic STI, which has no clean counterpart. Using a real space construction (topological crystal), we find an axion STI characterized by the average axion angle θ ¯ = π , protected by an average C 4 T symmetry with ( C 4 T ) 4 = 1 . While the exact C 4 T symmetry reverses the sign of θ angle, and hence seems to protect a Z 2 classification of θ = 0 , π , we prove that the θ = π state cannot be realized in the clean limit if ( C 4 T ) 4 = 1 . Therefore, the axion STI lacks band insulator correspondence and is thus intrinsic. To illustrate this state, we construct a lattice model and numerically explore its phase diagram, identifying an axion STI phase separated from both band insulators and trivial Anderson insulators by a metallic phase, revealing the intrinsic nature of the STI. We also argue that the intrinsic STI is robust against electron-electron interactions. Our Letter thus provides the first intrinsic crystalline ASPT and its lattice realization.}, archive = {J_PRL}, author = {Xi Chen and Fa-Jie Wang and Zhen Bi and Zhi-Da Song}, doi = {10.1103/PhysRevLett.134.226601}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226601}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic axion statistical topological insulator}, volume = {134}, year = {2025}, }
• (2025). Dynamical freezing in exactly solvable models of driven chaotic quantum dots. PRL, 134(22), 226501. (www)

  @article{ , abstract = {The late-time equilibrium behavior of generic interacting models is determined by the coupled hydrodynamic equations associated with the globally conserved quantities. In the presence of an external time-dependent drive, nonintegrable systems typically thermalize to an effectively infinite-temperature state, losing all memory of their initial states. However, in the presence of a large time-periodic Floquet drive, there exist special points in phase space where the strongly interacting system develops approximate emergent conservation laws. Here, we present results for an exactly solvable model of two coupled chaotic quantum dots with multiple orbitals interacting via random two- and four-fermion interactions in the presence of a Floquet drive. We analyze the phenomenology of dynamically generated freezing using a combination of exact diagonalization and field-theoretic analysis in the limit of a large number of electronic orbitals. The model displays universal freezing behavior irrespective of whether the theory is averaged over the disorder configurations or not. We present explicit computations for the growth of many-body chaos and entanglement entropy, which demonstrates the long-lived coherence associated with the interacting degrees of freedom even at late times at the dynamically frozen points. We also compute the slow timescale that controls relaxation away from exact freezing in a high-frequency expansion.}, archive = {J_PRL}, author = {Haoyu Guo and Rohit Mukherjee and Debanjan Chowdhury}, doi = {10.1103/ggk3-6cf8}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226501}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical freezing in exactly solvable models of driven chaotic quantum dots}, volume = {134}, year = {2025}, }
• (2025). Distinguishing thermal fluctuations from polaron formation in halide perovskites. PRL, 134(22), 226402. (www)

  @article{ , abstract = {Recent angle-resolved photoelectron spectroscopy (ARPES) measurements of the hole effective mass in CsPbBr 3 revealed an enhancement of ∼ 50 % compared to the bare mass computed from first principles for CsPbBr 3 at T = 0 K . This large enhancement was interpreted as evidence of polaron formation. Employing accurate finite-temperature first-principles calculations, we show that the calculated hole effective mass of CsPbBr 3 at T = 300 K can explain experimental results without invoking polarons. Thermal fluctuations are particularly strong in halide perovskites compared to conventional semiconductors such as Si and GaAs, and cannot be ignored when comparing with experiment. We not only resolve the debate on polaron formation in halide perovskites, but also demonstrate the general importance of including thermal fluctuations in first-principles calculations for strongly anharmonic materials.}, archive = {J_PRL}, author = {Bai-Qing Zhao and Jue-Yi Qi and Xun Xu and Xuan-Yan Chen and Chuan-Nan Li and Jinshan Li and Chris G. Van de Walle and Xie Zhang}, doi = {10.1103/p9h2-l2gh}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226402}, shortjournal = {Phys. Rev. Lett.}, title = {Distinguishing thermal fluctuations from polaron formation in halide perovskites}, volume = {134}, year = {2025}, }
• (2025). Quantification of electronic asymmetry: Chirality and axiality in solids. PRL, 134(22), 226401. (www)

  @article{ , abstract = {Chiral and axial materials offer platforms for intriguing phenomena, such as cross-correlated responses and chirality-induced spin selectivity. However, quantifying the properties of such materials has generally been considered challenging. Here, we demonstrate that the spatial distribution of the electron chirality, represented by with the four-component Dirac field , characterizes the chirality and axiality of materials. Furthermore, we reveal that spin-derived electric polarization can serve as an effective indicator of material polarity. We present quantitative evaluations of electron chirality distribution and spin-derived electric polarization based on first-principles calculations. Additionally, we propose that electron chirality can be directly observed via circular dichroism in photoemission spectroscopy, which measures the difference between right- and left-handed circularly polarized light. Electron chirality and spin-derived electric polarization provide a new framework for quantifying chirality, axiality, and polarity in asymmetric materials, paving the way for the exploration of novel functional materials.}, archive = {J_PRL}, author = {Tatsuya Miki and Hiroaki Ikeda and Michi-To Suzuki and Shintaro Hoshino}, doi = {10.1103/PhysRevLett.134.226401}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantification of electronic asymmetry: Chirality and axiality in solids}, volume = {134}, year = {2025}, }
• (2025). Coupled electron-phonon hydrodynamics in two-dimensional semiconductors. PRL, 134(22), 226301. (www)

  @article{ , abstract = {Electronic and thermal transport properties in two-dimensional (2D) semiconductors have been extensively investigated due to their potential to miniaturize transistors. Microscopically, electron-phonon interactions are considered the dominant momentum relaxation mechanism for electrons that limits carrier mobility beyond cryogenic temperatures. However, when electrons and phonons are considered as a single system, electron-phonon interactions conserve the total momentum and energy, leading to the possibility of low-dissipation transport. In this Letter, we systematically investigate the momentum circulation, in which momentum previously transferred from electrons to phonons (or vice versa) can be pumped back to the original carriers through interactions between nonequilibrium electrons and phonons, and its impact on carrier transport properties in 2D semiconductors with strong electron-phonon interactions. We find that, when strong momentum circulation is taken into account, the total momentum in the coupled electron-phonon system is weakly dissipated, leading to a coupled electron-phonon hydrodynamic transport regime, in which electrons and phonons exhibit a joint drift motion rather than separate diffusive behaviors. In this transport regime, charge transport properties are significantly enhanced. Contrary to previous belief, our results demonstrate that low-dissipation charge transport can occur despite strong electron-phonon interactions when there is effective momentum circulation between electrons and phonons. Our Letter advances fundamental understandings of carrier transport in 2D semiconductors.}, archive = {J_PRL}, author = {Yujie Quan and Bolin Liao}, doi = {10.1103/PhysRevLett.134.226301}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226301}, shortjournal = {Phys. Rev. Lett.}, title = {Coupled electron-phonon hydrodynamics in two-dimensional semiconductors}, volume = {134}, year = {2025}, }
• (2025). Non-markovian effects in quantum rate calculations of hydrogen diffusion with electronic friction. PRL, 134(22), 226201. (www)

  @article{ , abstract = {We address the challenge of incorporating non-Markovian electronic friction effects in quantum-mechanical approximations of dynamical observables. A generalized Langevin equation is formulated for ring-polymer molecular dynamics rate calculations, which combines electronic friction with a description of nuclear quantum effects for adsorbates on metal surfaces. An efficient propagation algorithm is introduced that captures both the spatial dependence of friction strength and non-Markovian frictional memory. This framework is applied to a model of hydrogen diffusing on Cu(111) derived from ab initio density functional theory calculations, revealing significant alterations in rate constants and tunneling crossover temperatures due to non-Markovian effects. Our findings explain why previous classical molecular dynamics simulations with Markovian friction showed unexpectedly good agreement with experiment, highlighting the critical role of non-Markovian effects in first-principles atomistic simulations.}, archive = {J_PRL}, author = {George Trenins and Mariana Rossi}, doi = {10.1103/PhysRevLett.134.226201}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226201}, shortjournal = {Phys. Rev. Lett.}, title = {Non-markovian effects in quantum rate calculations of hydrogen diffusion with electronic friction}, volume = {134}, year = {2025}, }
• (2025). Postavalanche relaxation sheds light on twinning mechanisms. PRL, 134(22), 226101. (www)

  @article{ , abstract = {Avalanches are abundant abrupt events that occur during various physical processes, where the material transitions between equilibrium states through complex dynamics. Relaxation’s dynamics are simpler and milder compared to avalanches, typically following a well-defined kinetic law. Here, we reveal the elemental differences between avalanches and relaxations during deformation twinning in magnesium in terms of their rate and duration. At the same time, we find that each avalanche is followed by relaxation with an almost identical magnitude. An avalanche occurs at the timescale and corresponds to a twin nucleation while relaxation occurs at the ms timescale and corresponds to twin growth. Our results indicate that the local volumes twinned during these two coupled processes are nearly identical. This implies a simple geometrical relation between twin nucleation and subsequent twin growth, shedding light on the basic mechanisms during the early stages of twinning.}, archive = {J_PRL}, author = {Haile Gebrehiwet Seyoum and Emil Bronstein and Eilon Faran and Doron Shilo}, doi = {10.1103/ykym-pn9s}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226101}, shortjournal = {Phys. Rev. Lett.}, title = {Postavalanche relaxation sheds light on twinning mechanisms}, volume = {134}, year = {2025}, }
• (2025). Role of nematic fluctuations on superconductivity in FeSe0.47Te0.53 revealed by nuclear magnetic resonance under pressure. PRL, 134(22), 226002. (www)

  @article{ , abstract = {The relationship between antiferromagnetic (AFM) spin fluctuations (SF), nematic fluctuations, and superconductivity (SC) has been central to understanding the pairing mechanism in iron-based superconductors (IBSCs). Iron chalcogenides, which hold the simplest crystal structure in IBSCs, provide a good platform to investigate the relationship. Here, we report Se 77 and Te 125 nuclear magnetic resonance studies of FeSe 0.47 Te 0.53 , which is located close to a nematic quantum critical point (QCP), under pressures up to 1.35 GPa. Both the superconducting critical temperature and AFMSF were found to be enhanced under pressure, which suggests a correlation between SC and AFMSF in FeSe 0.47 Te 0.53 . However, the contribution of AFMSF to SC in FeSe 0.47 Te 0.53 was found to be much less compared to that in FeSe 1 − x S x , suggesting that nematic fluctuations play a dominant role in the SC in FeSe 1 − x Te x around the nematic QCP.}, archive = {J_PRL}, author = {Qing-Ping Ding and Juan Schmidt and Jose A. Moreno and Sergey L. Bud’ko and Paul C. Canfield and Yuji Furukawa}, doi = {10.1103/kxth-gxvm}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226002}, shortjournal = {Phys. Rev. Lett.}, title = {Role of nematic fluctuations on superconductivity in FeSe0.47Te0.53 revealed by nuclear magnetic resonance under pressure}, volume = {134}, year = {2025}, }
• (2025). Anomalous doppler effect in superfluid and supersolid atomic gases. PRL, 134(22), 226001. (www)

  @article{ , abstract = {By employing the formalism of hydrodynamics, we derive novel analytic predictions for the Doppler effect in superfluids with broken Galilean invariance and hosting persistent currents at zero temperature. We consider two scenarios: when Galilean invariance is broken explicitly (by external potentials) and spontaneously, as it happens in a supersolid. In the former case, the presence of a stationary current affects the propagation of sound via an anomalous Doppler term proportional to the density derivative of the superfluid fraction. In supersolids, where, according to Goldstone theorem, distinct sounds of hybrid superfluid and crystal nature can propagate, the Doppler effect can be very different for each sound. Quantitative estimates of the Doppler shifts are obtained for Bose-Einstein condensed atomic gases, described by Gross-Pitaevskii theory. The estimates are obtained both calculating the thermodynamic parameters entering the hydrodynamic results and from full time-dependent simulations.}, archive = {J_PRL}, author = {Tomasz Zawiślak and Marija Šindik and Sandro Stringari and Alessio Recati}, doi = {10.1103/PhysRevLett.134.226001}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {226001}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous doppler effect in superfluid and supersolid atomic gases}, volume = {134}, year = {2025}, }
• (2025). Transient fluted films behind falling water columns. PRL, 134(22), 224001. (www)

  @article{ , abstract = {When a column of water drains from a vertical tube, it often leaves behind a trailing film that forms intricate, axisymmetric liquid structures. Using high-speed imaging and first-principles modeling, we investigate the formation and breakup of these fluted films and demonstrate that their diverse morphologies arise from the evolving balance of inertia, surface tension, gravity, and viscous forces. By analyzing the characteristic timescales for film emergence, retraction, and rupture, we classify the observed behaviors into distinct regimes and predict the transitions between them. Our theoretical framework captures the transient velocity and thickness of the film at the tube exit and yields regime boundaries that closely match experimental observations. These results not only explain a deceptively simple fluid dynamic system but also provide insight into film stability, merging, and rupture processes relevant to falling film evaporators, coating flows, and capillary-inertial instabilities across soft matter and multiphase systems.}, archive = {J_PRL}, author = {Abhijit K. Kushwaha and Matthew B. Jones and Jesse Belden and Nathan Speirs and Tadd T. Truscott}, doi = {10.1103/PhysRevLett.134.224001}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {224001}, shortjournal = {Phys. Rev. Lett.}, title = {Transient fluted films behind falling water columns}, volume = {134}, year = {2025}, }
• (2025). Chern-protected flatband edge state in metaphotonics. PRL, 134(22), 223806. (www)

  @article{ , abstract = {Two-dimensional Dirac semimetals feature flatband edge states but a zero Chern number, while Chern insulators support one-way edge states associated with a nonzero Chern number. Here, we demonstrate a two-dimensional photonic crystal combining the response of a semimetal and of a Chern insulator, termed a Chern semimetal. This photonic semimetal is characterized by a nonzero Chern number, simultaneously hosting both a flatband edge state and a one-way edge state. We experimentally realize such a photonic Chern semimetal using a gyromagnetic photonic crystal with programmable magnetic bias, tailoring its second-neighbor coupling within each sublattice. We also verify the ability to control over the light speed while preserving topological protection. Our findings open new avenues toward exploring topological phases and their applications across fermionic and bosonic systems, providing an exciting platform for nanophotonic applications and a playground for topological physics discoveries.}, archive = {J_PRL}, author = {Jianfeng Chen and Yidong Zheng and Shuihua Yang and Andrea Alù and Zhi-Yuan Li and Cheng-Wei Qiu}, doi = {10.1103/PhysRevLett.134.223806}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223806}, shortjournal = {Phys. Rev. Lett.}, title = {Chern-protected flatband edge state in metaphotonics}, volume = {134}, year = {2025}, }
• (2025). Fluctuation statistics of nonlinear optical microcanonical systems. PRL, 134(22), 223805. (www)

  @article{ , abstract = {It is by now well known, that at thermal equilibrium, the dynamics of multimoded optical configurations eventually settle into a Rayleigh-Jeans (RJ) distribution in the presence of weak nonlinearities. Yet, in spite of intense research, a general methodology to quantify and predict the complete statistical response of optical microcanonical settings remains elusive. Toward this end, we here develop a universal theory of fluctuation statistics for nonlinear multimode optical systems. Our results reveal a transition from narrow quasi-Lorentzian statistics in the low temperature regime, to an exponential distribution at higher temperatures. We show that this peculiar morphing of the underlying photostatistics is unique to microcanonical systems and has no analog in grand canonical configurations. A comparison between direct phase space integration and numerical simulations shows excellent agreement with our theoretical results, providing a testament to ergodicity even in nonlinear systems with very few modes. Through our formal methodology, we are able to accurately quantify the nonlinear equilibria of small sized configurations, demonstrating a strong deviation from RJ statistics and an equilibrium response that defies equipartition at infinite temperatures.}, archive = {J_PRL}, author = {Do Hyeok Jeon and Georgios G. Pyrialakos and Mahmoud A. Selim and Abraham M. Berman Bradley and Mercedeh Khajavikhan and Demetrios N. Christodoulides}, doi = {10.1103/wpz5-dvpl}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223805}, shortjournal = {Phys. Rev. Lett.}, title = {Fluctuation statistics of nonlinear optical microcanonical systems}, volume = {134}, year = {2025}, }
• (2025). Rewritable binary recording of the photon spin state in chiral liquid crystals. PRL, 134(22), 223804. (www)

  @article{ , abstract = {We experimentally demonstrate that the spin state (up or down) of circularly polarized light can be reliably encoded as a polar structural state (up or down) in chiral liquid crystals, with high selectivity. This enables a spin-driven, nonvolatile binary liquid crystal memory, which can be optically written and electrically erased on demand. The underlying mechanism involves an orientational buckling instability, whose direction depends on whether the handedness of light matches or opposes that of the chiral medium. This optical poling effect arises from a chiral light-matter interaction during the propagation of light through the twisted anisotropic medium.}, archive = {J_PRL}, author = {Nicolas Bruni and Charles Loussert and Mushegh Rafayelyan and Tetiana Orlova and Delphine Coursault and Etienne Brasselet}, doi = {10.1103/pqdp-x2vr}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223804}, shortjournal = {Phys. Rev. Lett.}, title = {Rewritable binary recording of the photon spin state in chiral liquid crystals}, volume = {134}, year = {2025}, }
• (2025). Stochastic dynamics of incoherent branched flows. PRL, 134(22), 223803. (www)

  @article{ , abstract = {Waves propagating through weakly disordered smooth linear media undergo a universal phenomenon called branched flow. Branched flow has been observed and studied experimentally in various systems by considering coherent waves. Recent experiments have reported the observation of optical branched flow by using an incoherent light source, thus revealing the key role of coherent phase-sensitive effects in the development of incoherent branched flow. By considering the paraxial wave equation as a generic representative model, we elaborate a stochastic theory of both coherent and incoherent branched flow. We derive closed-form equations that determine the evolution of the intensity correlation function, as well as the value and the propagation distance of the maximum of the scintillation index, which characterize the dynamical formation of incoherent branched flow. We report accurate numerical simulations that are found in quantitative agreement with the theory without free parameters. Our theory highlights the important impact of coherence and interference on branched flow, thereby providing a framework for exploring branched flow in nonlinear media, in relation to the formation of freak waves in oceans.}, archive = {J_PRL}, author = {Josselin Garnier and Antonio Picozzi and Theo Torres}, doi = {10.1103/PhysRevLett.134.223803}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223803}, shortjournal = {Phys. Rev. Lett.}, title = {Stochastic dynamics of incoherent branched flows}, volume = {134}, year = {2025}, }
• (2025). Dissipative topological dynamics in optical waveguides: Sensitivity versus robustness. PRL, 134(22), 223802. (www)

  @article{ , abstract = {Topological physics has garnered attention across various fields, emphasizing topologically protected modes renowned for their robustness against disorders. Recent advancements have expanded from conservative wave systems to diffusion systems with dissipative interactions. However, the transition region between wave and diffusion dynamics remains scarce, primarily due to the complexities involved in coupling modulation. Here, we develop a universal coupling control scheme via reservoir engineering, achieving conservative, dissipative, and mixed topologies in an optical waveguide array. Contrary to the belief that topological modes are disorder resistant, we found that topological dissipative modes are highly sensitive to initial excitations and noise. This sensitivity is due to their residence within the complex band gap, facilitating the excitation and preservation of bulk modes with lower loss. We also propose a method to control the degree of topological robustness and even stabilize these sensitive topological states by selectively managing dissipative potentials. Our Letter offers new insights into the dissipative dynamics of topological states, paving the way for wave coherent manipulation and diffusion transport on photonic chips.}, archive = {J_PRL}, author = {Zhiyuan Lin and Jian Li and Wange Song and Shanhe Su and Jiacheng Sun and Shengjie Wu and Chunyu Huang and Shining Zhu and Tao Li}, doi = {10.1103/bk7q-6r9d}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223802}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipative topological dynamics in optical waveguides: Sensitivity versus robustness}, volume = {134}, year = {2025}, }
• (2025). Transient symmetry breaking in a pumped crystal via the electric-field-dependent stark effect. PRL, 134(22), 223801. (www)

  @article{ , abstract = {We have investigated the transient properties of a ZnO crystal under a pump pulse (pumped crystal) using a pump-probe methodology. By monitoring the second harmonic of the weak probe pulse generated from the pumped crystal, we observe that the angular distribution of the second-harmonic yield becomes asymmetric compared to that without the pump. Importantly, the asymmetry of the second-harmonic generation (SHG) appears to be retarded by nearly 25 fs relative to the pump pulse, and its scaling shows a highly nonlinear dependence on the pump intensity. In addition, by using a two-color pump pulse, we further demonstrate that the asymmetry of SHG is controllable by adjusting the electric field of the two-color pulse. These phenomena can be attributed to the strong-field-induced electric-field-dependent Stark effect. Unlike the conventional intensity-dependent Stark effect, where only energy levels of the pumped target move, electric-field-dependent Stark effect indicates that the excitation induced by the pump pulse can distort the orbital and plays a vital role on the transient property of the pumped crystal. Our work suggests a new freedom for rationally designing the transient property of crystals by controlling the electric field of the pump pulse, which paves the way for realizing petahertz high-speed signal processing.}, archive = {J_PRL}, author = {Liang Li and Wei He and Shiqi Liang and Pengfei Lan and Peixiang Lu}, doi = {10.1103/PhysRevLett.134.223801}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223801}, shortjournal = {Phys. Rev. Lett.}, title = {Transient symmetry breaking in a pumped crystal via the electric-field-dependent stark effect}, volume = {134}, year = {2025}, }
• (2025). On-chip quantum interference between independent lithium niobate-on-insulator photon-pair sources. PRL, 134(22), 223602. (www)

  @article{ , abstract = {Generating and interfering nonclassical states of light is fundamental to optical quantum information science and technology. Quantum photonic integrated circuits provide one pathway towards scalability by combining nonlinear sources of nonclassical light and programmable circuits in centimeter-scale devices. The key requirements for quantum applications include efficient generation of indistinguishable photon-pairs and high-visibility programmable quantum interference. Here, we demonstrate a lithium niobate-on-insulator (LNOI) integrated photonic circuit that generates a two-photon path-entangled state, and a programmable interferometer for quantum interference. We generate entangled photons with brightness and perform quantum interference experiments on the chip with visibility. LNOI is an emerging photonics technology that has revolutionized high-speed modulators and efficient frequency conversion. Our results provide a path towards large-scale integrated quantum photonics including efficient photon-pair generation and programmable circuits for applications such as boson sampling and quantum communications.}, archive = {J_PRL}, author = {Robert J. Chapman and Tristan Kuttner and Jost Kellner and Alessandra Sabatti and Andreas Maeder and Giovanni Finco and Fabian Kaufmann and Rachel Grange}, doi = {10.1103/n2y3-2bmz}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223602}, shortjournal = {Phys. Rev. Lett.}, title = {On-chip quantum interference between independent lithium niobate-on-insulator photon-pair sources}, volume = {134}, year = {2025}, }
• (2025). Torus bifurcation of a dissipative time crystal. PRL, 134(22), 223601. (www)

  @article{ , abstract = {Using a quantum gas setup consisting of a Bose-Einstein condensate strongly coupled to a high-finesse optical cavity by a transverse pump laser, we experimentally observe an instability of a dissipative continuous time crystal toward a time crystalline state exhibiting two prominent oscillation frequencies. Applying a mean-field approximation model and a Floquet analysis, we theoretically confirm that this transition is a manifestation in a many-body system of a torus bifurcation between a limit cycle (LC) and a limit torus (LT). We theoretically illustrate the LC and LT attractors using the minimal model and experimentally reconstruct them using Takens’ embedding theorem applied to the nondestructively measured intracavity photon dynamics.}, archive = {J_PRL}, author = {Jayson G. Cosme and Phatthamon Kongkhambut and Anton Bölian and Richelle Jade L. Tuquero and Jim Skulte and Ludwig Mathey and Andreas Hemmerich and Hans Keßler}, doi = {10.1103/PhysRevLett.134.223601}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223601}, shortjournal = {Phys. Rev. Lett.}, title = {Torus bifurcation of a dissipative time crystal}, volume = {134}, year = {2025}, }
• (2025). Spin and density modes in a binary fluid of light. PRL, 134(22), 223403. (www)

  @article{ , abstract = {We report the experimental observation of spin and density modes in a binary mixture of superfluids of light. A miscible Bose-Bose mixture with repulsive interactions is realized by propagating the two circular polarization components of a laser through a nonlinear hot atomic vapor in the paraxial limit. By controlling the intensity and phase of both polarizations, we selectively excite the fundamental modes of the mixture. Using a Bragg-like spectroscopy technique, we measure the dispersion relation and identify two distinct branches with different sound velocities, corresponding to the spin and density modes. At high photon density, we observe a crossing of these branches, resulting from higher order nonlinear terms, linked to the saturation of the medium’s nonlinearity.}, archive = {J_PRL}, author = {Clara Piekarski and Nicolas Cherroret and Tangui Aladjidi and Quentin Glorieux}, doi = {10.1103/s58b-3mmx}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223403}, shortjournal = {Phys. Rev. Lett.}, title = {Spin and density modes in a binary fluid of light}, volume = {134}, year = {2025}, }
• (2025). Observation of brownian motion of a bose-einstein condensate. PRL, 134(22), 223402. (www)

  @article{ , abstract = {We report on the experimental observation of classical Brownian motion in momentum space by a Bose-Einstein condensate (BEC) of rubidium atoms prepared in a hexagonal optical lattice. Upon suddenly increasing the effective atomic mass, the BEC as a whole behaves as a classical rigid body with its center of mass receiving random momentum kicks by a Langevin force arising from atom loss and interactions with the surrounding thermal cloud. Physically, this amounts to selective heating of the BEC center-of-mass degree of freedom by a sudden quench, while with regard to the relative coordinates, the BEC is stabilized by repulsive atomic interactions, and its internal dynamics is suppressed by forced evaporative cooling induced by atom loss. A phenomenological theory is developed that well explains the experimental data quantitatively.}, archive = {J_PRL}, author = {Xiao-Qiong Wang and Rui-Lang Zeng and Zi-Yao Zhang and Chushun Tian and Shizhong Zhang and Andreas Hemmerich and Zhi-Fang Xu}, doi = {10.1103/tp71-51gv}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223402}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of brownian motion of a bose-einstein condensate}, volume = {134}, year = {2025}, }
• (2025). High precision spectroscopy of trilobite rydberg molecules. PRL, 134(22), 223401. (www)

  @article{ , abstract = {We perform three-photon photoassociation to obtain high resolution spectra of trilobite dimers for the principal quantum numbers , 24, 25, 26, and 27. The large binding energy of the molecules in combination with a relative spectroscopic resolution of provides a rigorous benchmark for existing theoretical models. A recently developed Green’s function framework, which circumvents the convergence issues that afflicted previous studies, is employed to theoretically reproduce the vibrational spectrum of the molecule with high accuracy. The relatively large molecular binding energy is primarily determined by the low-energy -wave electron-atom scattering length, thereby allowing us to extract the scattering phase shift with unprecedented accuracy, at low-energy regimes inaccessible to free electrons.}, archive = {J_PRL}, author = {Markus Exner and Rohan Srikumar and Richard Blättner and Matthew T. Eiles and Peter Schmelcher and Herwig Ott}, doi = {10.1103/PhysRevLett.134.223401}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223401}, shortjournal = {Phys. Rev. Lett.}, title = {High precision spectroscopy of trilobite rydberg molecules}, volume = {134}, year = {2025}, }
• (2025). Limits on anomalous spin-spin interactions using noble-gas nuclear magnetic resonance. PRL, 134(22), 223201. (www)

  @article{ , abstract = {Numerous theories beyond the standard model of particle physics propose the existence of ultralight hypothetical bosons, which are prominent dark-matter candidates. One of the most promising approaches to search for these bosons is through precision measurements. The basic principle is to measure energy shifts of standard-model particles induced by hypothetical bosons with ultrahigh energy resolution. Here we develop a sensitive magnetometer based on noble-gas nuclear magnetic resonance, achieving an energy resolution of ∼ 10 − 23 eV . Using this magnetometer, we measure the energy shifts of nuclear spins induced by anomalous Z ′ boson-mediated spin-spin interactions. The null results set the most stringent constraints on anomalous neutron-neutron and neutron-proton spin couplings in the Z ′ -boson mass ranges of 6.0–157.4 and < 129.6 μ eV , respectively. Notably, our constraints surpass previous ones by up to 17 orders of magnitude in aforementioned mass ranges. Our experiments further set the most stringent constraints on neutron-proton spin couplings mediated by massless γ ′ paraphotons, surpassing previous constraints by at least 25 orders of magnitude. Our technique paves the way for intriguing future directions in the search for various anomalous spin-spin interactions, including those mediated by axions with projected sensitivity surpassing astrophysical limits.}, archive = {J_PRL}, author = {Haowen Su and Shiju Hu and Yang Ding and Yuanhong Wang and Min Jiang and Xinhua Peng}, doi = {10.1103/PhysRevLett.134.223201}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223201}, shortjournal = {Phys. Rev. Lett.}, title = {Limits on anomalous spin-spin interactions using noble-gas nuclear magnetic resonance}, volume = {134}, year = {2025}, }
• (2025). Ionization energy of metastable he3 (2 s13) and the alpha- and helion-particle charge-radius difference from precision spectroscopy of the np rydberg series. PRL, 134(22), 223001. (www)

  @article{ , abstract = {The current experimental and theoretical values of the ionization energy of metastable He 4 [ ( 1 s ) ( 2 s ) S 3 1 ] differ by 9 σ , which prevents the determination of the alpha-particle charge radius from spectroscopic measurements in He 4 . To help clarify the origin of this discrepancy, we report on a precision measurement of hyperfine-resolved transitions from the ( 1 s ) ( 2 s ) S 3 1 metastable state of He 3 to high n p Rydberg states converging on the F + = 0 , 1 hyperfine levels of the He + 3 ( 1 s ) 2 S 1 / 2 ground state. Rydberg-series extrapolation using multichannel quantum-defect theory (MQDT) enabled the determination of the ionization energy of the ( 1 s ) ( 2 s ) S 3 1 state of He 3 [ E I ( He 3 ) / h = 1 152 788 844.6154 ( 77 ) stat ( 25 ) sys MHz ] and of the corresponding isotopic shift [ ( E I ( He 4 ) − E I ( He 3 ) ) / h = 53 898.093 ( 9 ) MHz ]. The MQDT analysis also permitted the quantification of singlet-triplet mixing in the n p series induced by the hyperfine interaction. From the isotopic shift of the ionization energy of He, the difference δ r 2 between the squared charge radii of the helion and alpha particles is determined to be 1.060 ( 10 ) fm 2 .}, archive = {J_PRL}, author = {Gloria Clausen and Frédéric Merkt}, doi = {10.1103/PhysRevLett.134.223001}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {223001}, shortjournal = {Phys. Rev. Lett.}, title = {Ionization energy of metastable he3 (2 s13) and the alpha- and helion-particle charge-radius difference from precision spectroscopy of the np rydberg series}, volume = {134}, year = {2025}, }
• (2025). Extracting neutron-neutron interaction strength and spatiotemporal dynamics of neutron emission from the two-particle correlation function. PRL, 134(22), 222301. (www)

  @article{ , abstract = {The neutron-neutron ( n n ) correlation function has been measured in 25 MeV / u Sn 124 + Sn 124 reactions. Using the Lednický-Lyuboshitz approach, the n n scattering length and effective range ( f 0 n n , d 0 n n ), as well as the reduced space-time size R ( 0 ) of the neutron emission source are simultaneously extracted as ( 18.9 − 1.2 + 1.3 fm , 1.9 − 1.0 + 1.3 fm ) and 4.12 ± 0.12 fm , respectively. The measured n n scattering length is consistent with the results obtained in the low-energy scattering H 2 ( π − , γ ) 2 n , indicating heavy-ion collisions can serve as an effective approach for measuring n n interactions and further investigating the charge symmetry breaking of nuclear force. The space-time size extracted from momentum-gated correlation functions exhibits clear dependence on the pair momentum, with R ( 0 ) = 2.8 ± 0.1 fm and 4.9 ± 0.2 fm being determined for the high and low momentum neutrons, respectively.}, archive = {J_PRL}, author = {Dawei Si and Sheng Xiao and Zhi Qin and Yuhao Qin and Junhuai Xu and Baiting Tian and Boyuan Zhang and Haojie Zhang and Renjie Zou and Dong Guo and Yijie Wang and Xiaobao Wei and Yibo Hao and Zengxiang Wang and Tianren Zhuo and Chunwang Ma and Yuansheng Yang and Xianglun Wei and Herun Yang and Peng Ma and Limin Duan and Fangfang Duan and Kang Wang and Junbing Ma and Shiwei Xu and Zhen Bai and Guo Yang and Yanyun Yang and Zhigang Xiao}, doi = {10.1103/PhysRevLett.134.222301}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {222301}, shortjournal = {Phys. Rev. Lett.}, title = {Extracting neutron-neutron interaction strength and spatiotemporal dynamics of neutron emission from the two-particle correlation function}, volume = {134}, year = {2025}, }
• (2025). Next-to-next-to-leading-order QCD prediction for the pion form factor. PRL, 134(22), 221901. (www)

  @article{ , abstract = {We accomplish for the first time the two-loop computation of the leading-twist contribution to the pion form factor by employing the effective field theory formalism rigorously. The next-to-next-to-leading-order hard function is determined by evaluating the appropriate five-point QCD amplitude with the modern multiloop technique and by implementing the ultraviolet renormalization and infrared subtractions in the presence of evanescent operators. The yielding two-loop correction to this fundamental quantity turns out to be numerically significant at experimentally accessible momentum transfers. We further demonstrate that the newly computed two-loop QCD correction is highly beneficial for an improved determination of the leading-twist pion distribution amplitude.}, archive = {J_PRL}, author = {Yao Ji and Bo-Xuan Shi and Jian Wang and Ye-Fan Wang and Yu-Ming Wang and Hui-Xin Yu}, doi = {10.1103/yx51-lc3q}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221901}, shortjournal = {Phys. Rev. Lett.}, title = {Next-to-next-to-leading-order QCD prediction for the pion form factor}, volume = {134}, year = {2025}, }
• (2025). Precise extraction of αem(mZ2) at the tera-Z stage of a future circular collider. PRL, 134(22), 221802. (www)

  @article{ , abstract = {The current projected sensitivity on the electromagnetic coupling α em ( m Z 2 ) represents a bottleneck for the precision electroweak program at FCC-ee. We propose a novel methodology to extract this coupling directly from Z -pole data. By comparing the differential distribution of electrons, muons, and positrons in the forward region, the approach achieves a projected statistical sensitivity below the 10 − 5 level, representing a significant improvement over other methods. We assess the impact of leading parametric uncertainties including that of the top quark mass.}, archive = {J_PRL}, author = {Marc Riembau}, doi = {10.1103/PhysRevLett.134.221802}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221802}, shortjournal = {Phys. Rev. Lett.}, title = {Precise extraction of αem(mZ2) at the tera-Z stage of a future circular collider}, volume = {134}, year = {2025}, }
• (2025). Establishing CP violation in b-baryon decays. PRL, 134(22), 221801. (www)

  @article{ , abstract = {It is a long-standing puzzle why the C P violation (CPV) in the baryon system has not yet been definitively established as in the meson one. We demonstrate that individual partial-wave CPV in the Λ b → p π − and p K − decays can exceed 10%, but the destruction between the partial waves (the suppression by the small partial-wave weight) results in a small net direct CPV in the former (the latter) as measured currently. Our finding highlights the different dynamics responsible for CPVs in baryon and meson decays. We propose to probe the CPV observables associated with the angular distributions of the Λ b → p a 1 ( 1260 ) , p K 1 ( 1270 ) decay products, which are large enough for being identified experimentally.}, archive = {J_PRL}, author = {Jia-Jie Han and Ji-Xin Yu and Ya Li and Hsiang-nan Li and Jian-Peng Wang and Zhen-Jun Xiao and Fu-Sheng Yu}, doi = {10.1103/ynnx-f63h}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221801}, shortjournal = {Phys. Rev. Lett.}, title = {Establishing CP violation in b-baryon decays}, volume = {134}, year = {2025}, }
• (2025). Channel capacity of a relativistic string. PRL, 134(22), 221601. (www)

  @article{ , abstract = {I explore the limitations on the capacity of a relativistic channel to transmit power and information that arise because of the finiteness of the transverse speed of light. As a model system, I consider a rope constructed from a fundamental string, for which relativistic invariance is built in. By wiggling one end of the string, both power and information may be transmitted to the other end. I argue that even though an unbounded amount of power and information may be traveling down the string, there is a bound on how much may be transmitted. Further, I conjecture that the two kinds of channel capacity—power and information—interfere with each other, so that the only way to transmit the maximum amount of power is to send no information, and vice versa.}, archive = {J_PRL}, author = {Adam R. Brown}, doi = {10.1103/PhysRevLett.134.221601}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221601}, shortjournal = {Phys. Rev. Lett.}, title = {Channel capacity of a relativistic string}, volume = {134}, year = {2025}, }
• (2025). Black hole supercolliders. PRL, 134(22), 221401. (www)

  @article{ , abstract = {We show that collisions between particles free falling from infinity and a disk of material plunging off the retrograde innermost stable circular orbit of a near-extremal Kerr black hole is the unique astronomically natural way in which to create a gravitational particle accelerator with center of mass energies at the tens to hundreds of teraelectronvolt range; in other words, a supercollider.}, archive = {J_PRL}, author = {Andrew Mummery and Joseph Silk}, doi = {10.1103/PhysRevLett.134.221401}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221401}, shortjournal = {Phys. Rev. Lett.}, title = {Black hole supercolliders}, volume = {134}, year = {2025}, }
• (2025). Partial rate matrix for dark matter scattering. PRL, 134(22), 221003. (www)

  @article{ , abstract = {I present a highly efficient integration method for scattering calculations, and a “partial rate matrix” that encodes the scattering rate as a function of the SO(3) orientation of the detector. This replaces the original multidimensional rate integral with a simple exercise in vector multiplication, speeding up the rate calculation by a factor of around 10 8 . I include a scheme to fully factorize the dark matter particle model, its astrophysical velocity distribution, and the properties of the target material from each other, enabling efficient calculation of the partial rate matrix even in studies comparing large sets of these input functions. This is now the only sensible way to evaluate the dark matter scattering rate in anisotropic detector materials. It is straightforward to generalize this method to other difficult but linear problems.}, archive = {J_PRL}, author = {Benjamin Lillard}, doi = {10.1103/PhysRevLett.134.221003}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221003}, shortjournal = {Phys. Rev. Lett.}, title = {Partial rate matrix for dark matter scattering}, volume = {134}, year = {2025}, }
• (2025). Supernovae time profiles as a probe of new physics at neutrino telescopes. PRL, 134(22), 221002. (www)

  @article{ , abstract = {Neutrino telescopes, including IceCube, can detect galactic supernova events by observing the collective rise in photomultiplier count rates with a subsecond time resolution. Leveraging precise timing, we demonstrate for the first time the ability of neutrino telescopes to explore new weakly coupled states emitted from supernovae and subsequently decaying to neutrinos. Our approach utilizes publicly available packages, asteria and snewpy , for simulating detector responses and parametrizing neutrino fluxes originating from the standard model and new physics. We present results for two beyond-the-standard model scenarios and introduce the tool developed for testing a diverse range of new physics models.}, archive = {J_PRL}, author = {Carlos A. Argüelles and Vedran Brdar and Jeffrey Lazar and Ying-Ying Li}, doi = {10.1103/PhysRevLett.134.221002}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221002}, shortjournal = {Phys. Rev. Lett.}, title = {Supernovae time profiles as a probe of new physics at neutrino telescopes}, volume = {134}, year = {2025}, }
• (2025). Extended δN formalism: Nonspatially flat separate-universe approach. PRL, 134(22), 221001. (www)

  @article{ , abstract = {The δ N formalism is a powerful approach to compute nonlinearly the large-scale evolution of the comoving curvature perturbation ζ . It assumes a set of FLRW patches that evolve independently, but in doing so, all the gradient terms are discarded, which are not negligibly small in models beyond slow roll. In this Letter, we extend the formalism to capture these gradient corrections by encoding them in a homogeneous-spatial-curvature contribution assigned to each FLRW patch. For a concrete example, we apply this formalism to the ultra-slow-roll inflation, and find that it can correctly describe the large-scale evolution of the comoving curvature perturbation from the horizon exit. We also briefly discuss non-Gaussianities in this context.}, archive = {J_PRL}, author = {Danilo Artigas and Shi Pi and Takahiro Tanaka}, doi = {10.1103/PhysRevLett.134.221001}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {221001}, shortjournal = {Phys. Rev. Lett.}, title = {Extended δN formalism: Nonspatially flat separate-universe approach}, volume = {134}, year = {2025}, }
• (2025). Testing the wineland criterion with finite statistics. PRL, 134(22), 220802. (www)

  @article{ , abstract = {The Wineland parameter aims at detecting metrologically useful entangled states, called spin-squeezed states, from expectations and variances of total angular momenta. However, efficient strategies for estimating this parameter in practice have yet to be determined and, in particular, the effects of a finite number of measurements remain insufficiently addressed. We formulate the detection of spin squeezing as a hypothesis-testing problem, where the null hypothesis assumes that the experimental data can be explained by non-spin-squeezed states. Within this framework, we derive upper and lower bounds on the p value to quantify the statistical evidence against the null hypothesis. By applying our statistical test to data obtained in multiple experiments, we are unable to reject the hypothesis that non-spin-squeezed states were measured with a p value of 5% or less in most cases. We also find an explicit non-spin-squeezed state according to the Wineland parameter reproducing most of the observed results with a p value exceeding 5%. More generally, our results provide a rigorous method to establish robust statistical evidence of spin squeezing from the Wineland parameter in future experiments, accounting for finite statistics.}, archive = {J_PRL}, author = {E. S. Carrera and Y. Zhang and J-D. Bancal and N. Sangouard}, doi = {10.1103/5svm-skxk}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {220802}, shortjournal = {Phys. Rev. Lett.}, title = {Testing the wineland criterion with finite statistics}, volume = {134}, year = {2025}, }
• (2025). Exploiting nonlocal correlations for dispersion-resilient quantum communications. PRL, 134(22), 220801. (www)

  @article{ , abstract = {Encoding quantum information via time-bin entangled states has had a profound impact on the development of quantum communications. However, dispersive propagation limits their achievable transmission distances. Here we describe a regime for nonlocal dispersion cancellation where the sum of arrival times of photons undergoing identical dispersion remains highly correlated. We exploit this effect to mitigate dispersive effects in a quantum key distribution fiber link, allowing an increase in the secret key rate by over a factor of 5 after 80 km of optical fiber dispersion.}, archive = {J_PRL}, author = {Hao Yu and Benjamin Crockett and Nicola Montaut and Stefania Sciara and Mario Chemnitz and Sai T. Chu and Brent E. Little and David J. Moss and Zhiming Wang and José Azaña and Roberto Morandotti}, doi = {10.1103/PhysRevLett.134.220801}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {220801}, shortjournal = {Phys. Rev. Lett.}, title = {Exploiting nonlocal correlations for dispersion-resilient quantum communications}, volume = {134}, year = {2025}, }
• (2025). Inhomogeneous quantum quenches of conformal field theory with boundaries. PRL, 134(22), 220404. (www)

  @article{ , abstract = {We develop a method to calculate generic time-dependent correlation functions for inhomogeneous quantum quenches in ( )-dimensional conformal field theory (CFT) induced by sudden Hamiltonian deformations that modulate the energy density inhomogeneously. Our Letter particularly focuses on the effects of spatial boundaries, which have remained unresolved by previous analytical methods. For generic postquench Hamiltonian, we develop a generic method to calculate the correlations by mirroring the system, which otherwise are Euclidean path integrals in complicated spacetime geometries difficult to calculate. On the other hand, for a special class of inhomogeneous postquench Hamiltonians, including the Möbius and sine-square-deformation Hamiltonians, we show that the quantum quenches exhibit simple boundary effects calculable from Euclidean path integrals in a straightforward strip spacetime geometry. Applying our method to the time evolution of entanglement entropy, we find that, for generic cases, the entanglement entropy shows discontinuities (shockwave fronts) propagating from the boundaries. In contrast, such discontinuities are absent in cases with simple boundary effects. We verify that our generic CFT formula matches well with numerical calculations from free-fermion tight-binding models for various quench scenarios.}, archive = {J_PRL}, author = {Xinyu Liu and Alexander McDonald and Tokiro Numasawa and Biao Lian and Shinsei Ryu}, doi = {10.1103/PhysRevLett.134.220404}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {220404}, shortjournal = {Phys. Rev. Lett.}, title = {Inhomogeneous quantum quenches of conformal field theory with boundaries}, volume = {134}, year = {2025}, }
• (2025). Non-markovian quantum mpemba effect. PRL, 134(22), 220403. (www)

  @article{ , abstract = {Since its rediscovery in the twentieth century, the Mpemba effect, where a far-from-equilibrium state may relax faster than a state closer to equilibrium, has been extensively studied in classical systems and has recently received attention in quantum systems. Many theories explaining this counter-intuitive behavior in classical systems rely on memory effects. However, in quantum systems, the relation between the Mpemba effect and memory has remained unexplored. In this Letter, we consider general non-Markovian open quantum systems and reveal new classes of quantum Mpemba effects, with no analog in Markovian quantum dynamics. Generically, open quantum dynamics possess a finite memory time and a unique steady state. Because of non-Markovian dynamics, even if the system is initialized in the steady state it can take a long time to relax back. We find other initial states that reach the steady state much faster. Most notably, we demonstrate that there can be an initial state in which the system reaches the steady state within the finite memory time itself, giving the fastest possible relaxation to stationarity. We verify the effect for quantum dot systems coupled to electronic reservoirs in equilibrium and nonequilibrium setups at weak, intermediate and strong coupling. Our Letter provides new insights into the rich physics underlying accelerated relaxation in quantum systems.}, archive = {J_PRL}, author = {David J. Strachan and Archak Purkayastha and Stephen R. Clark}, doi = {10.1103/PhysRevLett.134.220403}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {220403}, shortjournal = {Phys. Rev. Lett.}, title = {Non-markovian quantum mpemba effect}, volume = {134}, year = {2025}, }
• (2025). Anomalous discharging of quantum batteries: The ergotropic mpemba effect. PRL, 134(22), 220402. (www)

  @article{ , abstract = {Anomalous thermal relaxation is ubiquitous in nonequilibrium statistical mechanics. An emblematic example of this is the Mpemba effect, where an initially “hot” system cools faster than an initially “cooler” one. This effect has recently been studied in a variety of different classical and quantum settings. In this Letter, we find a novel signature of the Mpemba effect in the context of quantum batteries. We identify situations where batteries in higher charge states can discharge faster than less charged states. Specifically, we consider a quantum battery encoded in a single bosonic mode that is charged using unitary Gaussian operations. We show that the ergotropy, used here as a dynamical indicator of the energy stored in the battery, can be recast as a phase space relative entropy between the system’s state and the unitarily connected passive state, at each time. Our formalism allows us to compute the ergotropy analytically under dissipative dynamics and allows us to understand the conditions which give rise to a Mpemba effect. We also find situations where two batteries charged to the same value using different operations can discharge at different rates.}, archive = {J_PRL}, author = {Ivan Medina and Oisín Culhane and Felix C. Binder and Gabriel T. Landi and John Goold}, doi = {10.1103/PhysRevLett.134.220402}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {220402}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous discharging of quantum batteries: The ergotropic mpemba effect}, volume = {134}, year = {2025}, }
• (2025). Decoherence of histories: Chaotic versus integrable systems. PRL, 134(22), 220401. (www)

  @article{ , abstract = {We study the emergence of decoherent histories in isolated systems based on exact numerical integration of the Schrödinger equation for a Heisenberg chain. We reveal that the nature of the system, which we switch from (i) chaotic to (ii) interacting integrable to (iii) noninteracting integrable, strongly impacts decoherence of coarse spin observables. From a finite size scaling law we infer a strong exponential suppression of coherences for (i), a weak exponential suppression for (ii), and no exponential suppression for (iii) on a relevant short (nonequilibrium) timescale. Moreover, for longer times we find stronger decoherence for (i) but the opposite for (ii), hinting even at a possible power-law decay for (ii) at equilibrium timescales. This behavior is encoded in the multitime properties of the quantum histories and it can not be explained by environmentally induced decoherence. Our results suggest that chaoticity plays a crucial role in the emergence of classicality in finite size systems.}, archive = {J_PRL}, author = {Jiaozi Wang and Philipp Strasberg}, doi = {10.1103/m8vq-l449}, journal = {Physical Review Letters}, month = {6}, number = {22}, pages = {220401}, shortjournal = {Phys. Rev. Lett.}, title = {Decoherence of histories: Chaotic versus integrable systems}, volume = {134}, year = {2025}, }
• (2025). Erratum: Three-dimensional reconfigurable optical singularities in bilayer photonic crystals [Phys. rev. lett. 132, 073804 (2024)]. PRL, 134(21), 219901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 219901 (2025)}, archive = {J_PRL}, author = {Xueqi Ni and Yuan Liu and Beicheng Lou and Mingjie Zhang and Evelyn L. Hu and Shanhui Fan and Eric Mazur and Haoning Tang}, doi = {10.1103/PhysRevLett.134.219901}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {219901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Three-dimensional reconfigurable optical singularities in bilayer photonic crystals [Phys. rev. lett. 132, 073804 (2024)]}, volume = {134}, year = {2025}, }
• (2025). Emergence of a hump in the cubic dielectric response of glycerol. PRL, 134(21), 218202. (www)

  @article{ , abstract = {We report a direct determination of the cubic dielectric spectra of a realistic polar molecule, glycerol, from molecular dynamic (MD) simulations. From the liquid state to the mildly supercooled regime, we observed the emergence and growth of a hump in the cubic modulus, traditionally associated with collective effects in the dynamics. Its evolution follows that of dynamical correlations probed by the four-point susceptibility and that of the activation energy of the relaxation time. In particular, its appearance at high temperature coincides with the onset of superactivation. We show that, for this system, the shape of cubic spectra is only weakly affected by dipolar cross-correlations. The good agreement with experimental observations, despite the difference in temperature range, demonstrates the relevance of this approach to help get an insight into the intricate effects probed by nonlinear dielectric spectroscopy.}, archive = {J_PRL}, author = {Marceau Hénot and François Ladieu}, doi = {10.1103/PhysRevLett.134.218202}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {218202}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of a hump in the cubic dielectric response of glycerol}, volume = {134}, year = {2025}, }
• (2025). Diffusive contact between randomly driven colloidal suspensions. PRL, 134(21), 218201. (www)

  @article{ , abstract = {We study the relaxation process of two driven colloidal suspensions in contact, to a joint steady state, similar to the process of thermalization. First, we study a single suspension, subjecting it to random driving forces via holographic optical tweezers, which agitate it to a higher effective temperature. Interestingly, the effective temperature of the suspension, defined by the Einstein relation, exhibits a nonmonotonic dependence on the driving frequency. Next, we follow the flux of particles between two such suspensions in diffusive contact, starting from a uniform density and relaxing to a state with zero net particle flux. At high driving frequencies, we show that the density distribution at steady state is determined by equating the ratio of the chemical potential to the effective temperature in both systems, reminiscent of the thermal equilibrium behavior.}, archive = {J_PRL}, author = {Galor Geva and Tamir Admon and Maayan Levin and Yael Roichman}, doi = {10.1103/PhysRevLett.134.218201}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {218201}, shortjournal = {Phys. Rev. Lett.}, title = {Diffusive contact between randomly driven colloidal suspensions}, volume = {134}, year = {2025}, }
• (2025). Stretching response of a polymer chain with deformable bonds. PRL, 134(21), 218101. (www)

  @article{ , abstract = {The stretching response of polymer chains fundamentally determines the mechanical properties of polymer networks. In this Letter, we develop a statistical mechanics model that incorporates both bond stretching and bond angle deformation, enabling accurate predictions of chain behavior up to large forces. We further propose a semianalytical deformable freely rotating chain (dFRC) model, which represents the chain as a freely rotating chain with effective bond stretch and bond angle that depend on the chain stretch. Using physical parameters without fitting, both the statistical and dFRC models achieve excellent agreement with experimental data for carbon chains across all force regimes. Additionally, the dFRC model provides a direct estimate of the bond force, which is important to predict chain scission. By capturing key bond deformations while remaining computationally efficient, our work lays the foundation for future modeling of polymer network elasticity and failure.}, archive = {J_PRL}, author = {Jie Zhu and Laurence Brassart}, doi = {10.1103/PhysRevLett.134.218101}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {218101}, shortjournal = {Phys. Rev. Lett.}, title = {Stretching response of a polymer chain with deformable bonds}, volume = {134}, year = {2025}, }
• (2025). Two distinct oxidation dispersion mechanisms in Pd−CeO2 mediated by thermodynamic and kinetic behaviors of highly dispersed pd species. PRL, 134(21), 218001. (www)

  @article{ , abstract = {Using environmental scanning transmission electron microscopy and a global optimization algorithm, we unraveled the preoxidation dispersion and direct dispersion mechanisms in Pd − CeO 2 ( 100 ) systems, mediated by the behaviors of highly dispersed Pd species. At lower temperatures, Pd nanoparticles first undergo oxidation, followed by the dispersion of PdO nanoparticles. In contrast, at higher temperatures, Pd nanoparticles directly convert into highly distributed cationic Pd species. These distinct dispersion mechanisms are driven by the thermodynamic and kinetic differences of environment-dependent Pd1-2O and Pd1-4O species, providing a fundamental basis for precisely controlling catalyst dispersion states.}, archive = {J_PRL}, author = {Chen Zou and Wen Liu and Shiyuan Chen and Yuanjie Xu and Yu Tang and Songda Li and Fangwen Yang and Linjiang Yu and Chaobin Zeng and Yue-Yu Zhang and Xiaojuan Hu and Liang Wang and Zhong-Kang Han and Ying Jiang and Wentao Yuan and Hangsheng Yang and Yong Wang}, doi = {10.1103/PhysRevLett.134.218001}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {218001}, shortjournal = {Phys. Rev. Lett.}, title = {Two distinct oxidation dispersion mechanisms in Pd−CeO2 mediated by thermodynamic and kinetic behaviors of highly dispersed pd species}, volume = {134}, year = {2025}, }
• (2025). Critical demand in a stochastic model of flows in supply networks. PRL, 134(21), 217401. (www)

  @article{ , abstract = {Supply networks are essential for modern production, yet their critical properties remain understudied. We present a stochastic model with random production capacities to analyze material flow to a root node, focusing on topology and buffer stocks. The critical demand, where unsatisfied demand diverges, is examined mostly through numerical simulations. Without stocks, minimal production dictates behavior, making topology irrelevant. With stocks, memory effects arise, making topology crucial. Increased local connectivity is beneficial: firms should favor broad, short supply chains over long, narrow ones.}, archive = {J_PRL}, author = {Yannick Feld and Marc Barthelemy}, doi = {10.1103/PhysRevLett.134.217401}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {217401}, shortjournal = {Phys. Rev. Lett.}, title = {Critical demand in a stochastic model of flows in supply networks}, volume = {134}, year = {2025}, }
• (2025). Landau theory description of autferroicity. PRL, 134(21), 216801. (www)

  @article{ , abstract = {Autferroics, recently proposed as a sister branch of multiferroics, exhibit strong intrinsic magnetoelectricity, but ferroelectricity and magnetism are mutually exclusive rather than coexisting. Here, a general model is considered based on the Landau theory, to clarify the distinction between multiferroics and autferroics by qualitative change-rotation in a Landau free energy landscape and in particular phase mapping. The TiGeSe 3 exemplifies a factual material, whose first-principles computed Landau coefficients predict its autferroicity. Our investigation paves the way for an alternative avenue in the pursuit of intrinsically strong magnetoelectrics.}, archive = {J_PRL}, author = {Jun-Jie Zhang and Boris I. Yakobson and Shuai Dong}, doi = {10.1103/PhysRevLett.134.216801}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216801}, shortjournal = {Phys. Rev. Lett.}, title = {Landau theory description of autferroicity}, volume = {134}, year = {2025}, }
• (2025). Unravelling the surface local spin dynamics in magnetic nanoparticles by means of NMR relaxometry. PRL, 134(21), 216703. (www)

  @article{ , abstract = {We singled out the surface and bulk spin dynamics in magnetic hollow nanoparticles by means of nuclear magnetic resonance relaxometry. Experimental -dispersion curves (NMR-D), measured across a wide frequency range ( ), show the presence of a high-frequency contribution to the longitudinal relaxation rate, evidenced for the first time and ascribed to the surface spin dynamics. The nuclear longitudinal relaxation rates were successfully analyzed by means of a phenomenological model accounting for the two spin populations, i.e., surface and core spins. The fit of the longitudinal NMR-D data by means of this model allowed for the estimation of the hyperfine coupling constant of the surface spins, and of the superparamagnetic and surface-paramagnetic-like spin-spin correlation frequency, the last one being larger by more than 1 order of magnitude. These experimental results provide a substantial contribution to the basic knowledge of spin dynamics in nanoscale systems.}, archive = {J_PRL}, author = {M. Basini and M. Mariani and Q. L. Vuong and Y. Gossuin and S. Slimani and G. Singh and D. Peddis and A. Lascialfari}, doi = {10.1103/PhysRevLett.134.216703}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216703}, shortjournal = {Phys. Rev. Lett.}, title = {Unravelling the surface local spin dynamics in magnetic nanoparticles by means of NMR relaxometry}, volume = {134}, year = {2025}, }
• (2025). Magnetoelectric decoupling in bismuth ferrite. PRL, 134(21), 216702. (www)

  @article{ , abstract = {It is still an open question if magnetoelectric coupling occurs at the atomic scale in multiferroic BiFeO 3 . Nuclear solid-state techniques monitor local fields at the atomic scale. Using such an approach, we show that, contrary to our own expectation, ferroelectric and magnetic ordering in bismuth ferrite ( BiFeO 3 or BFO) decouple at the unit-cell level. Time differential perturbed angular correlation (TDPAC) data at temperatures below, close, and above the magnetic Néel temperature show that the coupling of the ferroelectric order to magnetization is completely absent at the bismuth site. It is common understanding that the antiferromagnetic order and the cycloidal ordering due to the Dzyaloshinskii-Moriya interaction generate a net zero magnetization of the sample canceling out any magnetoelectric effect at the macroscopic level. Our previous data show that a very large coupling of magnetic moment and electrical distortions arises on the magnetic sublattice (Fe site). The oxygen octahedra around the iron site experience a large tilt due to the onset of magnetic ordering. Nevertheless, the Bi-containing complementary sublattice carrying the largest part of ferroelectric order is practically unaffected by this large structural change in its direct vicinity. The magnetoelectric coupling thus vanishes already at the unit cell level. These experimental results agree well with an ab initio density functional theory (DFT) calculation.}, archive = {J_PRL}, author = {Thien Thanh Dang and Juliana Heiniger-Schell and Astita Dubey and João Nuno Gonçalves and Marianela Escobar Castillo and Daniil Lewin and Ian Chang Jie Yap and Adeleh Mokhles Gerami and Sobhan Mohammadi Fathabad and Dmitry Zyabkin and Doru Constantin Lupascu}, doi = {10.1103/PhysRevLett.134.216702}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216702}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetoelectric decoupling in bismuth ferrite}, volume = {134}, year = {2025}, }
• (2025). Atacamite Cu2Cl(OH)3 in high magnetic fields: Quantum criticality and dimensional reduction of a sawtooth-chain compound. PRL, 134(21), 216701. (www)

  @article{ , abstract = {We report an extensive high-field study of atacamite , a material realization of quantum sawtooth chains with weak interchain couplings, in continuous and pulsed magnetic fields up to 58 T. In particular, we have mapped the entropy landscape for fields as high as 35 T and have identified a field-induced quantum critical point at 21.9(1) T for axis. The quantum critical point separates field regions with and without magnetic order, evidenced by our thermodynamic study and nuclear magnetic resonance spectroscopy, but lies far below full saturation of the magnetization. Corroborated by numerical results using density-matrix renormalization group calculations, we find this behavior associated with a dimensional reduction of the spin system: the sawtooth chain effectively decouples into an antiferromagnetic spin- chain (backbone of the sawtooth chain) in the presence of an exchange field produced by the remaining field-polarized spins.}, archive = {J_PRL}, author = {L. Heinze and T. Kotte and R. Rausch and A. Demuer and S. Luther and R. Feyerherm and E. L. Q. N. Ammerlaan and U. Zeitler and D. I. Gorbunov and M. Uhlarz and K. C. Rule and A. U. B. Wolter and H. Kühne and J. Wosnitza and C. Karrasch and S. Süllow}, doi = {10.1103/PhysRevLett.134.216701}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216701}, shortjournal = {Phys. Rev. Lett.}, title = {Atacamite Cu2Cl(OH)3 in high magnetic fields: Quantum criticality and dimensional reduction of a sawtooth-chain compound}, volume = {134}, year = {2025}, }
• (2025). Three-dimensional valley hall phases in phononic crystals. PRL, 134(21), 216601. (www)

  @article{ , abstract = {Valley Hall phases (VHPs) in electronic and classical wave systems have been extensively explored and brought fruitful wave manipulations and associated applications. However, the concept of VHPs is so far restricted to two-dimensional (2D) systems. VHPs in 3D platforms remain an open question, which is not a straightforward extension of theirs 2D counterparts. In this work, we generalize the 2D VHPs into the 3D case in phononic crystals, which are derived from a nodal-line semimetal. The variation of geometric parameters gives rise to band inversion and generates two distinct VHPs possessing a pair of valleys with opposite Berry curvature distributions in the Brillouin zone. Topological surface states protected by the 3-tuple valley Chern numbers emerge at the interface between two different VHPs. Thanks to the configuration of the equal-frequency contour, some intriguing surface wave propagations have been observed experimentally. At the corner surrounded by two VHPs, interestingly, circular propagation of the surface wave exhibits negative refraction to form a closed loop around the corner. Furthermore, 3D partition is demonstrated in a four-channel structure. The 3D VHPs will stimulate other exotic transports, such as 3D collimation and wave guiding, and provide new means for designing 3D acoustic devices.}, archive = {J_PRL}, author = {Riyi Zheng and Jialuo Liang and Junpeng Wu and Jiuyang Lu and Weiyin Deng and Xueqin Huang and Manzhu Ke and Zhengyou Liu}, doi = {10.1103/PhysRevLett.134.216601}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216601}, shortjournal = {Phys. Rev. Lett.}, title = {Three-dimensional valley hall phases in phononic crystals}, volume = {134}, year = {2025}, }
• (2025). Machine learning small polaron dynamics. PRL, 134(21), 216301. (www)

  @article{ , abstract = {Polarons are crucial for charge transport in semiconductors, significantly impacting material properties and device performance. The dynamics of small polarons can be investigated using first-principles molecular dynamics. However, the limited timescale of these simulations presents a challenge for adequately sampling infrequent polaron hopping events. Here, we introduce a message-passing neural network combined with first-principles molecular dynamics within the Born-Oppenheimer approximation that learns the polaronic potential energy surface by encoding the polaronic state, allowing for simulations of polaron hopping dynamics at the nanosecond scale. By leveraging the statistical significance of the long timescale, our framework can accurately estimate polaron (anisotropic) mobilities and activation barriers in prototypical polaronic oxides across different scenarios (hole polarons in rocksalt MgO and electron polarons in pristine and F-doped rutile ) within experimentally measured ranges.}, archive = {J_PRL}, author = {Viktor C. Birschitzky and Luca Leoni and Michele Reticcioli and Cesare Franchini}, doi = {10.1103/PhysRevLett.134.216301}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216301}, shortjournal = {Phys. Rev. Lett.}, title = {Machine learning small polaron dynamics}, volume = {134}, year = {2025}, }
• (2025). Discovering high-entropy oxides with a machine-learning interatomic potential. PRL, 134(21), 216101. (www)

  @article{ , abstract = {High-entropy materials shift the traditional materials discovery paradigm to one that leverages disorder, enabling access to unique chemistries unreachable through enthalpy alone. We present a self-consistent approach integrating computation and experiment to understand and explore single-phase rocksalt high-entropy oxides. By leveraging a machine-learning interatomic potential, we rapidly and accurately map high-entropy composition space using our two descriptors: bond length distribution and mixing enthalpy. The single-phase stabilities for all experimentally stabilized rocksalt compositions are correctly resolved, with dozens more compositions awaiting discovery.}, archive = {J_PRL}, author = {Jacob T. Sivak and Saeed S. I. Almishal and Mary Kathleen Caucci and Yueze Tan and Dhiya Srikanth and Joseph Petruska and Matthew Furst and Long-Qing Chen and Christina M. Rost and Jon-Paul Maria and Susan B. Sinnott}, doi = {10.1103/PhysRevLett.134.216101}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216101}, shortjournal = {Phys. Rev. Lett.}, title = {Discovering high-entropy oxides with a machine-learning interatomic potential}, volume = {134}, year = {2025}, }
• (2025). Universal scaling relations in electron-phonon superconductors. PRL, 134(21), 216002. (www)

  @article{ , abstract = {We study linear scaling relations in electron-phonon superconductors. By combining numerical and analytical techniques, we find linear Homes scaling relations between the zero-temperature superfluid density and the normal-state dc conductivity. This phenomenon arises via either a large impurity scattering rate or inelastic scattering of electrons and Einstein phonons at large electron-phonon coupling. Thus, our Letter shows that Homes scaling is more universal than either cuprate or BCS-like physics and is, instead, a fundamental result in a wide class of superconductors.}, archive = {J_PRL}, author = {Joshuah T. Heath and Rufus Boyack}, doi = {10.1103/PhysRevLett.134.216002}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216002}, shortjournal = {Phys. Rev. Lett.}, title = {Universal scaling relations in electron-phonon superconductors}, volume = {134}, year = {2025}, }
• (2025). Large tunable kinetic inductance in a twisted graphene superconductor. PRL, 134(21), 216001. (www)

  @article{ , abstract = {Twisted graphene based moiré heterostructures host a flat band at the magic angles where the kinetic energy of the charge carriers is quenched and interaction effects dominate. This results in emergent phases such as superconductors and correlated insulators that are electrostatically tunable. We investigate superconductivity in twisted trilayer graphene by integrating it as the weak link in a superconducting quantum interference device. The measured current phase relation yields a large and tunable kinetic inductance, up to 150 nH per square, of the electron and hole-type intrinsic superconductors. We further show that the specific kinetic inductance and the critical current density are universally related via the superconducting coherence length, and extract an upper bound of for the coherence length. We discuss the implications of a large coherence length in twisted graphene superconductors.}, archive = {J_PRL}, author = {Rounak Jha and Martin Endres and Kenji Watanabe and Takashi Taniguchi and Mitali Banerjee and Christian Schönenberger and Paritosh Karnatak}, doi = {10.1103/PhysRevLett.134.216001}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {216001}, shortjournal = {Phys. Rev. Lett.}, title = {Large tunable kinetic inductance in a twisted graphene superconductor}, volume = {134}, year = {2025}, }
• (2025). Electron heating by parallel electric fields in magnetotail reconnection. PRL, 134(21), 215201. (www)

  @article{ , abstract = {We investigate electron heating by magnetic-field-aligned electric fields ( ) during antiparallel magnetic reconnection in the Earth’s magnetotail. Using a statistical sample of 140 reconnection outflows, we infer the acceleration potential associated with from the shape of the electron velocity distribution functions. We show that heating by in the reconnection outflow can reach up to 10 times the inflow electron temperature. We demonstrate that the magnitude of the acceleration potential scales with the inflow Alfvén and electron thermal speeds to maintain quasineutrality in the reconnection region. Our results suggest that, as the inflow plasma parameter increases, becomes increasingly important to the ion-to-electron energy partition associated with magnetic reconnection.}, archive = {J_PRL}, author = {Louis Richard and Yuri V. Khotyaintsev and Cecilia Norgren and Konrad Steinvall and Daniel B. Graham and Jan Egedal and Andris Vaivads and Rumi Nakamura}, doi = {10.1103/PhysRevLett.134.215201}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {215201}, shortjournal = {Phys. Rev. Lett.}, title = {Electron heating by parallel electric fields in magnetotail reconnection}, volume = {134}, year = {2025}, }
• (2025). Precursors of thin film rupture: Similarity solution of surfactant-driven, inertial capillary waves. PRL, 134(21), 214002. (www)

  @article{ , abstract = {The thinning of liquid sheets and the resulting capillary waves due to surfactant deposition are relevant to understanding how bubbles burst, with implications for the environment, health, and industry. Here, a similarity solution is obtained, which describes the sheet thinning and capillary waves. The final rupture mechanism of a bubble is explored, suggesting that insoluble surfactant deposition alone does not cause finite-time rupture; instead, sufficient thinning may allow other physical mechanisms to do so. Comparisons to an existing experiment and suggestions for measurements are given.}, archive = {J_PRL}, author = {Jun Eshima and Howard A. Stone and Luc Deike}, doi = {10.1103/PhysRevLett.134.214002}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {214002}, shortjournal = {Phys. Rev. Lett.}, title = {Precursors of thin film rupture: Similarity solution of surfactant-driven, inertial capillary waves}, volume = {134}, year = {2025}, }
• (2025). Jet size prediction in compound multiphase bubble bursting. PRL, 134(21), 214001. (www)

  @article{ , abstract = {The Worthington jets from bursting bubbles at a gas-liquid interface can break up into small droplets, aerosolizing chemical and biological substances into the atmosphere and impacting both global climate and public health. Despite their importance in contaminant transport, the influence of adsorbed contaminants on bubble-bursting jet dynamics remains poorly understood. Here, we document how an immiscible compound contaminant layer impacts the jet radius, which deviates from the expected jetting dynamics produced by clean bubble bursting. We rationalize the deviation of the jet radius by characterizing the propagation of the capillary waves at the air-oil-water interface. We develop a linearized wave damping model based on the oil thickness profile and the wave dispersion, and we propose a revised Ohnesorge number with a scaling relation that captures the experimental results reasonably well. Our work not only advances the fundamental understanding of bubble bursting jets but also offers valuable insights for predicting bubble-mediated aerosol size distributions and transport of airborne contaminants in realistic environmental scenarios.}, archive = {J_PRL}, author = {Zhengyu Yang and Yang Liu and Jie Feng}, doi = {10.1103/PhysRevLett.134.214001}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {214001}, shortjournal = {Phys. Rev. Lett.}, title = {Jet size prediction in compound multiphase bubble bursting}, volume = {134}, year = {2025}, }
• (2025). Simple yet accurate stochastic approach to the quantum phase noise of nanolasers. PRL, 134(21), 213804. (www)

  @article{ , abstract = {Nanolasers operating at low power levels are strongly affected by intrinsic quantum noise, influencing both intensity fluctuations and laser coherence. Starting from semiclassical rate equations and making a simple hypothesis for the phase of the laser field, a simple stochastic model for the laser quantum noise is suggested. The model is shown to agree quantitatively with quantum master equations for microscopic lasers with a small number of emitters and with classical Langevin equations for macroscopic systems. In contrast, neither quantum master equations nor classical Langevin equations adequately address the mesoscopic regime. The stochastic approach is used to calculate the linewidth throughout the transition to lasing, where the linewidth changes from being dominated by the particlelike nature of photons below threshold to the wavelike nature above threshold, where it is strongly influenced by index fluctuations enhancing the linewidth.}, archive = {J_PRL}, author = {Matias Bundgaard-Nielsen and Marco Saldutti and Benjamin Falkenberg Gøtzsche and Emil Grovn and Jesper Mørk}, doi = {10.1103/PhysRevLett.134.213804}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213804}, shortjournal = {Phys. Rev. Lett.}, title = {Simple yet accurate stochastic approach to the quantum phase noise of nanolasers}, volume = {134}, year = {2025}, }
• (2025). Polarization symmetry breaking of GHz dissipative solitons. PRL, 134(21), 213803. (www)

  @article{ , abstract = {Spontaneous symmetry breaking (SSB) is a significant topic in particle physics, condensed matter physics, fluid dynamics, etc. In nonlinear optics, polarization is a crucial degree of freedom that enables novel SSB dynamics in coherently pumped Kerr platforms, yet to be explored in laser systems with self-organized localized structure—dissipative soliton. In this study, a special kind of SSB—polarization symmetry breaking (PSB) of GHz dissipative solitons is demonstrated in a mini fiber laser. First, we establish a bidirectional model of the Fabry-Pérot (FP) mini fiber laser with orthogonally polarized counterpropagating light fields. This bidirectional model theoretically predicts the onset of PSB by merely increasing the soliton energy, which manifests as a Hopf bifurcation. Then, experimental validation is performed by implementing a FP mini fiber laser operating at a GHz repetition rate. An abrupt change of the polarization dynamics from the fixed-point attractor to the limit cycle is observed as the soliton energy increases. To verify these findings in real time, specialized polarization-resolved ultrafast techniques are developed for the analysis of high-repetition-rate vectorial signals. The measurements, including the full-Stokes characterization, not only confirm the presence of PSB but also elucidate the underlying physical mechanism associated with the polarization rotation of vector solitons. Our results suggest that the mini fiber laser can potentially become a promising platform for studying the physics of SSB by exploring the nonlinear dynamics of dissipative optical solitons.}, archive = {J_PRL}, author = {Yang Yang and Xuewen Chen and Wei Lin and Xu Hu and Haijiao Xu and Yuncong Ma and Zhaoheng Liang and Lin Ling and Zhijin Xiong and Yuankai Guo and Tao Liu and Xiaoming Wei and Zhongmin Yang}, doi = {10.1103/x3sy-gf7l}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213803}, shortjournal = {Phys. Rev. Lett.}, title = {Polarization symmetry breaking of GHz dissipative solitons}, volume = {134}, year = {2025}, }
• (2025). Tunable coherence laser interferometry: Demonstrating 40 dB of stray light suppression and compatibility with resonant optical cavities. PRL, 134(21), 213802. (www)

  @article{ , abstract = {A major limitation of laser interferometers using continuous wave lasers are parasitic light fields, such as ghost beams, scattered or stray light, that can cause nonlinear noise. This is especially relevant for laser interferometric ground-based gravitational wave detectors. Increasing their sensitivity, particularly at frequencies below 10 Hz, is threatened by the influence of parasitic photons. These can up-convert low-frequency disturbances into phase and amplitude noise inside the relevant measurement band. By artificially tuning the coherence of the lasers, using pseudo-random-noise (PRN) phase modulations, this influence of parasitic fields can be suppressed. As it relies on these fields traveling different paths, it does not sacrifice the coherence for the intentional interference. We demonstrate the feasibility of this technique experimentally, achieving noise suppression levels of 40 dB in a Michelson interferometer with an artificial coherence length below 30 cm. We probe how the suppression depends on the delay mismatch and length of the PRN sequence. We also prove that optical resonators can be operated in the presence of PRN modulation by measuring the behavior of a linear cavity with and without such a modulation. By matching the resonators round-trip length and the PRN sequence repetition length, the classic response is recovered.}, archive = {J_PRL}, author = {Daniel Voigt and Leonie Eggers and Katharina-Sophie Isleif and Sina M. Koehlenbeck and Melanie Ast and Oliver Gerberding}, doi = {10.1103/PhysRevLett.134.213802}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213802}, shortjournal = {Phys. Rev. Lett.}, title = {Tunable coherence laser interferometry: Demonstrating 40 dB of stray light suppression and compatibility with resonant optical cavities}, volume = {134}, year = {2025}, }
• (2025). Efficient transverse multiwave interactions up to six-wave mixing in a high-Q lithium niobate microresonator. PRL, 134(21), 213801. (www)

  @article{ , abstract = {High-order nonlinear optical processes beyond four-wave mixing ( ) are crucial for advancing ultraviolet (UV) light sources and quantum technologies, yet their practical implementation remains challenging due to inherently weak high-order nonlinear susceptibilities and stringent broadband phase-matching requirements—limitations that persist even in state-of-the-art high-Q microresonators. A breakthrough transverse multiwave mixing scheme is proposed in a high-Q lithium niobate microresonator, only under a single continuous-wave (cw) laser pump. Our approach leverages self-organized subwavelength photorefractive gratings (SPGs) generated through a bidirectional stimulated Raman scattering (SRS) process in the microresonator, without using two external counterpropagating lasers. Under single-wavelength pumping (1546 nm), bidirectional SRS (1713 nm) spontaneously generates dynamic SPGs that enable dual-function control: (1) broadband momentum compensation ( , period) to resolve broadband phase-matching challenges in high-order nonlinear interactions and (2) preservation of ultrahigh-quality factor ( ) for enhanced nonlinear conversion. Moreover, unlike conventional longitudinal configurations requiring more rigid multiwavelength resonance alignment, our transverse architecture decouples nonlinear processes from cavity-mode constraints through SPG-mediated momentum engineering, enabling simultaneous support for sum-frequency generation to six-wave mixing processes across 500-nm bandwidth with high conversion efficiencies. Furthermore, the cascaded SRS process is simultaneously activated to generate a light signal for subsequent nonlinear interactions. Consequently, this novel approach enables the first demonstration of single-pump phase-matched transverse SFG with record conversion efficiency ( ), and transverse multiwave mixing processes from (four-wave) to (six-wave) processes are achieved for the first time using only the single cw pump, leading to efficient visible and UV light generation, representing a notable advance in nonlinear integration.}, archive = {J_PRL}, author = {Chuntao Li and Ni Yao and Huakang Yu and Jintian Lin and Renhong Gao and Jiale Deng and Jianglin Guan and Lingling Qiao and Ya Cheng}, doi = {10.1103/PhysRevLett.134.213801}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213801}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient transverse multiwave interactions up to six-wave mixing in a high-Q lithium niobate microresonator}, volume = {134}, year = {2025}, }
• (2025). Local vs nonlocal dynamics in cavity-coupled rydberg atom arrays. PRL, 134(21), 213604. (www)

  @article{ , abstract = {Locality is a transversal principle that governs quantum dynamics of many-body systems. However, for cavity-embedded systems, such a fundamental notion is hindered by the presence of nonlocal cavity modes, leaving space for new possible dynamical behavior. Here, we investigate the real-time dynamics of low-energy excitations in one-dimensional Rydberg atom arrays coupled to a global cavity mode. We derive an effective description in terms of a Tavis-Cummings–Ising model, whose phase diagram features ordered and disordered phases. The nonlocal nature of the cavity mode drastically affects the emergent meson and string dynamics. Mesons hybridize coherently with the cavity photons, leading to composite meson-polariton excitations. Strings, differently from local interacting theories, acquire a finite kinetic energy thanks to nonlocal cavity-mediated interactions between the underlying domain walls. We then conclude by presenting a new concrete experimental blueprint for a cavity QED Rydberg atom array simulator where the physics outlined in this Letter can be realized.}, archive = {J_PRL}, author = {Zeno Bacciconi and Hernan B. Xavier and Matteo Marinelli and Devendra Singh Bhakuni and Marcello Dalmonte}, doi = {10.1103/PhysRevLett.134.213604}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213604}, shortjournal = {Phys. Rev. Lett.}, title = {Local vs nonlocal dynamics in cavity-coupled rydberg atom arrays}, volume = {134}, year = {2025}, }
• (2025). Deterministic generation of photonic entangled states using decoherence-free subspaces. PRL, 134(21), 213603. (www)

  @article{ , abstract = {We propose the use of collective states of matter as a resource for the deterministic generation of quantum states of light, which are fundamental for quantum information technologies. Our minimal model consists of three emitters coupled to a half-waveguide, i.e., a one-dimensional waveguide terminated by a mirror. Photon-mediated interactions between the emitters result in the emergence of bright and dark states. The dark states form a decoherence-free subspace, protected from dissipation. Local driving of the emitters and control of their resonance frequencies allows us to perform arbitrary quantum gates within the decoherence-free subspace. Coupling to bright states facilitates photon emission, thereby enabling the realization of quantum gates between light and matter. We demonstrate that sequential application of these gates leads to the generation of photonic entangled states, such as Greenberger-Horne-Zeilinger and one- and two-dimensional cluster states.}, archive = {J_PRL}, author = {Oriol Rubies-Bigorda and Stuart J. Masson and Susanne F. Yelin and Ana Asenjo-Garcia}, doi = {10.1103/PhysRevLett.134.213603}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213603}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic generation of photonic entangled states using decoherence-free subspaces}, volume = {134}, year = {2025}, }
• (2025). Leveraging collective effects for thermometry in waveguide quantum electrodynamics. PRL, 134(21), 213602. (www)

  @article{ , abstract = {We report a proof-of-principle experiment for a new method of temperature measurements in waveguide quantum electrodynamics experiments, allowing one to measure separately the temperature of global and local baths. The method takes advantage of collective states of two transmons located in the center of a waveguide. The Hilbert space of such a system forms two separate subspaces (bright and dark) that are coupled differently to external noise sources. Measuring transmission through the waveguide allows one to extract separately the temperatures of the baths responsible for global and local excitations in the system. Such a system would allow for building a new type of primary temperature sensor capable of addressing both local and global baths.}, archive = {J_PRL}, author = {Aleksei Sharafiev and Mathieu Juan and Marco Cattaneo and Gerhard Kirchmair}, doi = {10.1103/PhysRevLett.134.213602}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213602}, shortjournal = {Phys. Rev. Lett.}, title = {Leveraging collective effects for thermometry in waveguide quantum electrodynamics}, volume = {134}, year = {2025}, }
• (2025). Deterministic quantum state generators and stabilizers from nonlinear photonic filter cavities. PRL, 134(21), 213601. (www)

  @article{ , abstract = {Quantum states of light, particularly at optical frequencies, are considered necessary to realize a host of important quantum technologies and applications, spanning Heisenberg-limited metrology, continuous-variable quantum computing, and quantum communications. Nevertheless, a wide variety of important quantum light states are currently challenging to deterministically generate at optical frequencies. In part, this is due to a relatively small number of schemes that prepare target quantum states given nonlinear interactions. Here, we present an especially simple concept for deterministically generating and stabilizing important quantum states of light, using only third-order optical nonlinearities and engineered dissipation. We show how, by considering either a nonlinear cavity with frequency-dependent outcoupling or a chain of nonlinear waveguides, one can induce high loss for all but some desired light intensities. Specifically, we find that the stabilized intensities can correspond to an evenly spaced pattern of stablilized photon numbers. This is shown to produce important quantum states with coherent superpositions between various photon numbers. As examples of this phenomenon, we show cavities which can stabilize squeezed states, as well as produce “photon-number-comb” states. Moreover, in these types of filter cavities, Glauber coherent states will deterministically evolve into Schrodinger cat states of a desired order. We discuss potential realizations in quantum nonlinear optics. More broadly, we expect that combining the techniques introduced here with additional “phase-sensitive” nonlinearities (such as second-order nonlinearity) should enable passive stabilization and generation of a wider variety of states than shown here.}, archive = {J_PRL}, author = {Sean Chen and Nicholas Rivera and Jamison Sloan and Marin Soljačić}, doi = {10.1103/PhysRevLett.134.213601}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213601}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic quantum state generators and stabilizers from nonlinear photonic filter cavities}, volume = {134}, year = {2025}, }
• (2025). Unveiling under-the-barrier electron dynamics in strong field tunneling. PRL, 134(21), 213201. (www)

  @article{ , abstract = {Ever since the advent of quantum mechanics, tunneling has been an intriguing topic and consequently extensively studied and utilized. Investigating both theoretically and experimentally the nonadiabatic tunneling in strong-field ionization across a wide range of laser intensities, we unravel under-the-barrier-recollision dynamics leading to Freeman resonances (FR). The under-the-barrier-recollision model, which goes beyond the traditional direct multiphoton transition description, predicts distinct features of FR phenomena that cannot be explained by the existing direct multiphoton transition scenario. Specifically, it predicts (i) the dominance of high-order FR over above-threshold ionization in the photoelectron energy spectra and (ii) the flat dependence of the FR signal on the laser intensity, both in the nonadiabatic tunneling regime. This Letter experimentally demonstrates these features, corroborating the under-the-barrier-recollision model, and provides intuition into this dynamics, expanding our insights into the control of tunneling dynamics in laser spectroscopy and attosecond physics.}, archive = {J_PRL}, author = {Tsendsuren Khurelbaatar and Michael Klaiber and Suren Sukiasyan and Karen Z. Hatsagortsyan and Christoph H. Keitel and Dong Eon Kim}, doi = {10.1103/PhysRevLett.134.213201}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {213201}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling under-the-barrier electron dynamics in strong field tunneling}, volume = {134}, year = {2025}, }
• (2025). Experimental test of the ratio method for nuclear-reaction analysis. PRL, 134(21), 212501. (www)

  @article{ , abstract = {Nuclear halos are exotic quantal structures observed far from stability. They are mostly studied through reactions. The ratio of angular cross sections for breakup and scattering is predicted to be independent of the reaction process and to be very sensitive to the halo structure. We test this new observable experimentally for the first time on the collision of on C at and using existing data on Pb at . The theoretical predictions are verified, which offers the possibility of developing a new spectroscopic tool to study nuclear structure far from stability.}, archive = {J_PRL}, author = {S. Ota and P. Capel and G. Christian and V. Durant and K. Hagel and E. Harris and R. C. Johnson and Z. Luo and F. M. Nunes and M. Roosa and A. Saastamoinen and D. P. Scriven}, doi = {10.1103/PhysRevLett.134.212501}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {212501}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental test of the ratio method for nuclear-reaction analysis}, volume = {134}, year = {2025}, }
• (2025). Resonant forbidden CP asymmetry from soft leptons. PRL, 134(21), 211802. (www)

  @article{ , abstract = {To explain the baryon asymmetry in the early universe via leptogenesis, quantum corrections to new particles are commonly invoked to generate the necessary asymmetry. We demonstrate, however, that a large asymmetry can already arise from standard model leptons. The mechanism relies on resummation of soft leptons at finite temperatures. The asymmetry, which is kinematically forbidden in vacuum, can be resonantly enhanced from thermally resummed leptons by seven orders of magnitude. Contrary to the resonance from exotic particles, we show that the resonant enhancement from soft leptons is protected by controlled widths under finite-temperature perturbation theory. We quantify such asymmetries in leptogenesis with secluded flavor effects and comment on the significance and application. The mechanism exploits the maximal role of leptons themselves, featuring low-scale leptogenesis, minimal model buildings, and dark matter cogenesis.}, archive = {J_PRL}, author = {Shinya Kanemura and Shao-Ping Li}, doi = {10.1103/PhysRevLett.134.211802}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211802}, shortjournal = {Phys. Rev. Lett.}, title = {Resonant forbidden CP asymmetry from soft leptons}, volume = {134}, year = {2025}, }
• (2025). First measurement of the muon neutrino interaction cross section and flux as a function of energy at the LHC with FASER. PRL, 134(21), 211801. (www)

  @article{ , abstract = {This Letter presents the measurement of the energy-dependent neutrino-nucleon cross section in tungsten and the differential flux of muon neutrinos and antineutrinos. The analysis is performed using proton-proton collision data at a center-of-mass energy of 13.6 TeV and corresponding to an integrated luminosity of . Using the active electronic components of the FASER detector, charged current muon neutrino interaction events are identified, with backgrounds from other processes subtracted. We unfold the neutrino events into a fiducial volume corresponding to the sensitive regions of the FASER detector and interpret the results in two ways: (i) we use the expected neutrino flux to measure the cross section, and (ii) we use the predicted cross section to measure the neutrino flux. Both results are presented in six bins of neutrino energy, achieving the first differential measurement in the TeV range. The observed distributions align with standard model predictions. Using this differential data, we extract the contributions of neutrinos from pion and kaon decays.}, archive = {J_PRL}, author = {FASER Collaboration and Roshan Mammen Abraham and Xiaocong Ai and John Anders and Claire Antel and Akitaka Ariga and Tomoko Ariga and Jeremy Atkinson and Florian U. Bernlochner and Tobias Boeckh and Jamie Boyd and Lydia Brenner and Angela Burger and Franck Cadoux and Roberto Cardella and David W. Casper and Charlotte Cavanagh and Xin Chen and Dhruv Chouhan and Andrea Coccaro and Stephane Débieux and Monica D’Onofrio and Ansh Desai and Sergey Dmitrievsky and Radu Dobre and Sinead Eley and Yannick Favre and Deion Fellers and Jonathan L. Feng and Carlo Alberto Fenoglio and Didier Ferrere and Max Fieg and Wissal Filali and Elena Firu and Edward Galantay and Ali Garabaglu and Stephen Gibson and Sergio Gonzalez-Sevilla and Yuri Gornushkin and Carl Gwilliam and Daiki Hayakawa and Michael Holzbock and Shih-Chieh Hsu and Zhen Hu and Giuseppe Iacobucci and Tomohiro Inada and Luca Iodice and Sune Jakobsen and Hans Joos and Enrique Kajomovitz and Hiroaki Kawahara and Alex Keyken and Felix Kling and Daniela Köck and Pantelis Kontaxakis and Umut Kose and Rafaella Kotitsa and Susanne Kuehn and Thanushan Kugathasan and Lorne Levinson and Ke Li and Jinfeng Liu and Yi Liu and Margaret S. Lutz and Jack MacDonald and Chiara Magliocca and Toni Mäkelä and Lawson McCoy and Josh McFayden and Andrea Pizarro Medina and Matteo Milanesio and Théo Moretti and Mitsuhiro Nakamura and Toshiyuki Nakano and Laurie Nevay and Ken Ohashi and Hidetoshi Otono and Hao Pang and Lorenzo Paolozzi and Pawan Pawan and Brian Petersen and Titi Preda and Markus Prim and Michaela Queitsch-Maitland and Hiroki Rokujo and André Rubbia and Jorge Sabater-Iglesias and Osamu Sato and Paola Scampoli and Kristof Schmieden and Matthias Schott and Anna Sfyrla and Davide Sgalaberna and Mansoora Shamim and Savannah Shively and Yosuke Takubo and Noshin Tarannum and Ondrej Theiner and Eric Torrence and Oscar Ivan Valdes Martinez and Svetlana Vasina and Benedikt Vormwald and Di Wang and Yuxiao Wang and Eli Welch and Monika Wielers and Yue Xu and Samuel Zahorec and Stefano Zambito and Shunliang Zhang}, doi = {10.1103/PhysRevLett.134.211801}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211801}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of the muon neutrino interaction cross section and flux as a function of energy at the LHC with FASER}, volume = {134}, year = {2025}, }
• (2025). Thermal bootstrap for the critical O(N) model. PRL, 134(21), 211604. (www)

  @article{ , abstract = {We propose a numerical method to estimate one-point functions and the free-energy density of conformal field theories at finite temperature by solving the Kubo-Martin-Schwinger condition for the two-point functions of identical scalars. We apply the method for the critical model for , 2, 3 in . We find agreement with known results from Monte Carlo simulations and previous results for the 3D Ising model, and we provide new predictions for , 3.}, archive = {J_PRL}, author = {Julien Barrat and Enrico Marchetto and Alessio Miscioscia and Elli Pomoni}, doi = {10.1103/PhysRevLett.134.211604}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211604}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal bootstrap for the critical O(N) model}, volume = {134}, year = {2025}, }
• (2025). Hydrodynamic and rayleigh-plateau instabilities of q strings. PRL, 134(21), 211603. (www)

  @article{ , abstract = {As analogues of compact objects, solitons have attracted significant attention. We reveal that cylindrical Q strings exhibit a dynamical instability to perturbations with wavelengths exceeding a threshold . This instability can destroy the invariance in the cylindrical direction, as a generation mechanism for Q balls, similar to the formation of droplets. As the interface of Q strings approaches a thin wall, this long-wavelength instability degenerates into the Rayleigh-Plateau instability with a threshold related only to the geometric radius . Such results indicate that Q strings, like black strings, resemble low-viscosity fluids with surface tension.}, archive = {J_PRL}, author = {Qian Chen}, doi = {10.1103/PhysRevLett.134.211603}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211603}, shortjournal = {Phys. Rev. Lett.}, title = {Hydrodynamic and rayleigh-plateau instabilities of q strings}, volume = {134}, year = {2025}, }
• (2025). Batalin-vilkovisky formulation of n=1 supergravity in ten dimensions. PRL, 134(21), 211602. (www)

  @article{ , abstract = {We present a full Batalin-Vilkovisky action in the component field formalism for supergravity in ten dimensions coupled to Yang-Mills multiplets.}, archive = {J_PRL}, author = {Julian Kupka and Charles Strickland-Constable and Fridrich Valach}, doi = {10.1103/PhysRevLett.134.211602}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211602}, shortjournal = {Phys. Rev. Lett.}, title = {Batalin-vilkovisky formulation of n=1 supergravity in ten dimensions}, volume = {134}, year = {2025}, }
• (2025). Inequivalence between the euclidean and lorentzian versions of the type IIB matrix model from lefschetz thimble calculations. PRL, 134(21), 211601. (www)

  @article{ , abstract = {The type IIB matrix model is conjectured to describe superstring theory nonperturbatively in terms of ten bosonic traceless Hermitian matrices ( ), whose eigenvalues correspond to ( )-dimensional space-time. Quite often, this model has been investigated in its Euclidean version, which is well defined although the Lorentz symmetry of the original model is replaced by the rotational symmetry. Recently, a well-defined model respecting the Lorentz symmetry has been proposed by “gauge-fixing” the Lorentz symmetry nonperturbatively using the Faddeev-Popov procedure. Here we investigate the two models by Monte Carlo simulations overcoming the severe sign problem by the Lefschetz thimble method, in the case of matrix size omitting fermionic contributions. We add a quadratic term in the action and calculate the expectation values of rotationally symmetric (or Lorentz symmetric) observables as a function of the coefficient . Our results exhibit striking differences between the two models around and in the region associated with the appearance of different saddle points, clearly demonstrating their inequivalence against naive expectations from quantum field theory.}, archive = {J_PRL}, author = {Chien-Yu Chou and Jun Nishimura and Ashutosh Tripathi}, doi = {10.1103/PhysRevLett.134.211601}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211601}, shortjournal = {Phys. Rev. Lett.}, title = {Inequivalence between the euclidean and lorentzian versions of the type IIB matrix model from lefschetz thimble calculations}, volume = {134}, year = {2025}, }
• (2025). Jet from binary neutron star merger with prompt black hole formation. PRL, 134(21), 211407. (www)

  @article{ , abstract = {We performed the longest numerical-relativity neutrino-radiation magnetohydrodynamics simulation for a binary neutron star merger that extends to after the merger. We consider the binary model that undergoes the prompt collapse to a black hole after the merger with asymmetric mass and and SFHo equation of state. We find the Poynting flux-driven collimated outflow as well as the gravitational wave emission, neutrino emission, dynamical mass ejection, and postmerger mass ejection facilitated by magnetorotational instability-driven turbulent viscosity in a single self-consistent binary neutron star merger simulation. A magnetosphere dominated by the aligned global magnetic field penetrating the black hole develops along the black-hole spin axis after the turbulence in the remnant disk is enhanced. A jet with the Poynting flux with isotropic-equivalent luminosity of is launched, and the duration of the high luminosity is expected to be .}, archive = {J_PRL}, author = {Kota Hayashi and Kenta Kiuchi and Koutarou Kyutoku and Yuichiro Sekiguchi and Masaru Shibata}, doi = {10.1103/PhysRevLett.134.211407}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211407}, shortjournal = {Phys. Rev. Lett.}, title = {Jet from binary neutron star merger with prompt black hole formation}, volume = {134}, year = {2025}, }
• (2025). Thermal origin of the attractor-to-general-relativity in scalar-tensor gravity. PRL, 134(21), 211406. (www)

  @article{ , abstract = {The convergence of scalar-tensor gravity to general relativity, or the departure from it, is described in a new analogy with heat dissipation in a viscous fluid. This new thermal picture is applied to cosmology, shedding light on whether gravity deviates from general relativity early on and approaches it later in the cosmic history.}, archive = {J_PRL}, author = {Valerio Faraoni and Andrea Giusti}, doi = {10.1103/22w4-v2xn}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211406}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal origin of the attractor-to-general-relativity in scalar-tensor gravity}, volume = {134}, year = {2025}, }
• (2025). Charged static AdS black hole binaries. PRL, 134(21), 211405. (www)

  @article{ , abstract = {We construct the first binary black hole solutions of Einstein-Maxwell theory in asymptotically anti–de Sitter space. The attractive force between the two black holes is balanced by the addition of a background electric field, sourced at the conformal boundary. There is a continuous family of bulk solutions for a given boundary profile and temperature, suggesting there is continuous nonuniqueness. We investigate the charges of the solutions and numerically verify that they satisfy a first law of black hole mechanics relation.}, archive = {J_PRL}, author = {William D. Biggs and Jorge E. Santos}, doi = {10.1103/PhysRevLett.134.211405}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211405}, shortjournal = {Phys. Rev. Lett.}, title = {Charged static AdS black hole binaries}, volume = {134}, year = {2025}, }
• (2025). Quadratic mode couplings in rotating black holes and their detectability. PRL, 134(21), 211404. (www)

  @article{ , abstract = {Quadratic quasinormal modes encode fundamental properties of black hole spacetimes. They are also one of the key ingredients of nonlinearities of general relativity in the ringdown stage of binary black hole coalescence. In this Letter, we classify all possible quadratic coupling channels of quasinormal modes for a generic Kerr black hole and use a frequency-domain pseudospectral code with hyperboloidal slicing to calculate these couplings. After accounting for all the channels in systems with reflection symmetry, our results become consistent with those extracted from numerical simulations and time-domain fits. This agreement provides a compelling example demonstrating the success of black hole second-order perturbation theory. We also explore potential applications of our calculations in future ringdown data analysis by carrying out a detectability survey for various quadratic modes. We find that a few of them are observationally relevant for third-generation ground-based detectors like Cosmic Explorer, as well as the spaceborne Laser Interferometer Space Antenna.}, archive = {J_PRL}, author = {Neev Khera and Sizheng Ma and Huan Yang}, doi = {10.1103/PhysRevLett.134.211404}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211404}, shortjournal = {Phys. Rev. Lett.}, title = {Quadratic mode couplings in rotating black holes and their detectability}, volume = {134}, year = {2025}, }
• (2025). Environmental effects in extreme-mass-ratio inspirals: Perturbations to the environment in kerr spacetimes. PRL, 134(21), 211403. (www)

  @article{ , abstract = {Future gravitational wave observatories open a unique avenue to study the environments surrounding black holes. Intermediate or extreme mass ratio inspirals will spend thousands to millions of cycles in the sensitivity range of detectors, allowing subtle environmental effects to accumulate in the gravitational waveform. Working in Lorenz gauge and considering equatorial circular orbits, we present the first self-consistent, fully relativistic calculation of a perturbation to a black hole environment due to an inspiraling secondary in the Kerr geometry. As an example case, we consider the environment to be that of a superradiantly grown scalar cloud, though our framework is generalizable to other scenarios. We demonstrate that the scalar field develops a rich wake structure induced by the secondary and compute scalar fluxes emitted to infinity and through the horizon. Relative differences in the fluxes compared to Schwarzschild are tens of percent on large intervals of parameter space, underscoring the importance of modeling in Kerr.}, archive = {J_PRL}, author = {Conor Dyson and Thomas F. M. Spieksma and Richard Brito and Maarten van de Meent and Sam Dolan}, doi = {10.1103/PhysRevLett.134.211403}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211403}, shortjournal = {Phys. Rev. Lett.}, title = {Environmental effects in extreme-mass-ratio inspirals: Perturbations to the environment in kerr spacetimes}, volume = {134}, year = {2025}, }
• (2025). Dynamical lensing tomography of black hole ringdowns. PRL, 134(21), 211402. (www)

  @article{ , abstract = {Strong gravitational lensing occurs when photons pass through the vicinity of a black hole. We investigate this phenomenon in the context of a gravitational-wave event, specifically when a black hole is settling into its final state. The deflection angle of photons mimics the ringdown pattern of the gravitational wave at intermediate times. At late times it has an inverse cubic dependence on observation time. The deviation angle increases exponentially as photons approach the photon ring orbit, reflecting its unstable nature. Our findings are directly applicable to imaging scenarios involving stars against the background of compact binaries or circumbinary accretion disks, particularly during the merger of two black holes.}, archive = {J_PRL}, author = {Zhen Zhong and Vitor Cardoso and Yifan Chen}, doi = {10.1103/PhysRevLett.134.211402}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211402}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical lensing tomography of black hole ringdowns}, volume = {134}, year = {2025}, }
• (2025). Data driven approach for extracting tidal information from neutron star binary mergers observed with the einstein telescope. PRL, 134(21), 211401. (www)

  @article{ , abstract = {The recent breakthroughs regarding the detection of compact binary mergers via gravitational waves opened up a new window to the Universe. Gravitational-wave models have been essential to this success since they are necessary to infer the properties of the compact binary system from the observational data. Next-generation detectors, such as the Einstein Telescope, will allow for more observations of binary neutron star mergers with higher precision, making accurate waveform models crucial in describing these systems. In this Letter, we propose a novel approach for constructing phenomenological waveform models informed by observational data. Using mock data representing a one-year operation of the Einstein telescope as our baseline, we demonstrate how the results improve as more events are included in the calibration. This method offers a new and complementary approach for developing sophisticated gravitational-wave models compared to classical techniques that employ analytical computations and numerical-relativity simulations. Improved waveform models will then yield more accurate parameter estimation.}, archive = {J_PRL}, author = {Adrian Abac and Anna Puecher and Jonathan Gair and Tim Dietrich}, doi = {10.1103/PhysRevLett.134.211401}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211401}, shortjournal = {Phys. Rev. Lett.}, title = {Data driven approach for extracting tidal information from neutron star binary mergers observed with the einstein telescope}, volume = {134}, year = {2025}, }
• (2025). Collective flavor conversions are interactions of neutrinos with quantized flavor waves. PRL, 134(21), 211003. (www)

  @article{ , abstract = {Collective oscillations in dense neutrino gases (flavor waves) are notable for their instabilities that cause fast flavor conversion. We develop a quantum theory of interacting neutrinos and flavor wave quanta, which are analogous to plasmons but also carry flavor. The emission or absorption of such flavor plasmons 𝜓 , or “flavomons,” changes the neutrino flavor. When an angular crossing occurs, the process 𝜈 𝜇 → 𝜈 𝑒 + 𝜓 is more rapid than its inverse along the direction of the crossing, triggering stimulated 𝜓 emission and fast instability. Calculating the rate via Feynman diagrams matches the fast instability growth rate. Our novel 𝜈 and 𝜓 kinetic equations, corresponding to quasilinear theory, describe instability evolution without resolving the small scales of the flavomon wavelength, potentially overcoming the main challenge of fast flavor evolution.}, archive = {J_PRL}, author = {Damiano F. G. Fiorillo and Georg G. Raffelt}, doi = {10.1103/PhysRevLett.134.211003}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211003}, shortjournal = {Phys. Rev. Lett.}, title = {Collective flavor conversions are interactions of neutrinos with quantized flavor waves}, volume = {134}, year = {2025}, }
• (2025). Detectable and defect-free dark photon dark matter. PRL, 134(21), 211002. (www)

  @article{ , abstract = {Ultralight dark photons are compelling dark matter candidates, but their allowed kinetic mixing with the standard model photon is severely constrained by requiring that the dark photons do not collapse into a cosmic string network in the early Universe. Direct detection in minimal production scenarios for dark photon dark matter is strongly limited, if not entirely excluded; discovery of sub-meV dark photon dark matter would therefore point to a nonminimal dark sector. We describe a model that evades such constraints, capable of producing cold dark photons in any parameter space accessible to future direct detection experiments. The associated production dynamics yield additional signatures in cosmology and small-scale structure, allowing for possible positive identification of this particular class of production mechanisms.}, archive = {J_PRL}, author = {David Cyncynates and Zachary J. Weiner}, doi = {10.1103/PhysRevLett.134.211002}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211002}, shortjournal = {Phys. Rev. Lett.}, title = {Detectable and defect-free dark photon dark matter}, volume = {134}, year = {2025}, }
• (2025). Pole inflation from broken noncompact isometry in weyl gravity. PRL, 134(21), 211001. (www)

  @article{ , abstract = {We propose the microscopic origin of the pole inflation from the scalar fields of broken noncompact isometry in Weyl gravity. We show that the isometry in the field space in combination with the Weyl symmetry relates the form of the nonminimal couplings to the one of the potential in the Jordan frame. In the presence of an explicit breaking of the symmetry in the coefficient of the potential, we realize the pole inflation near the pole of the inflaton kinetic term. Applying our results to the Higgs or Peccei-Quinn (PQ) inflation models, we find that there is one parameter family of the solutions for the pole inflation, depending on the overall coefficient of the Weyl covariant derivatives for scalar fields. The same coefficient not only makes the predictions of the pole inflation varying, being compatible with the Planck data, but also determines the mass of the Weyl gauge field. We also show that the isocurvature perturbations of the axion can be suppressed sufficiently during the PQ pole inflation, and the massive Weyl gauge field produced during reheating serves as a dark matter candidate.}, archive = {J_PRL}, author = {Hyun Min Lee}, doi = {10.1103/skhx-yc43}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {211001}, shortjournal = {Phys. Rev. Lett.}, title = {Pole inflation from broken noncompact isometry in weyl gravity}, volume = {134}, year = {2025}, }
• (2025). Spin grouping in ring cavity and its protection on entangled states transfer. PRL, 134(21), 210803. (www)

  @article{ , abstract = {Long-range interactions are essential for large-scale quantum computation and quantum interconnections. Cavities provide a promising avenue to achieve long-range interaction by enhancing the coupling of remote qubits through shared cavity modes. In this Letter, we investigate a spin array coupled to a ring cavity supporting two counterpropagating modes, focusing on the system’s eigenstates and spin dynamics in the low-excitation regime. We show that, under specific spatial configurations, the spins naturally self-organize into two groups, within which exciton transport is confined. This spin-grouping mechanism preserves coherence between spins across the two groups, and is leveraged to deterministically transfer entangled states between remote spin pairs with additional dynamical addressing. We further propose feasible implementations using atomic qubits or solid-state platforms. Our scheme enables entangling remote spins within a cavity, highlighting potential applications in scalable quantum information processing.}, archive = {J_PRL}, author = {Chang Li}, doi = {10.1103/s7j9-z7f8}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210803}, shortjournal = {Phys. Rev. Lett.}, title = {Spin grouping in ring cavity and its protection on entangled states transfer}, volume = {134}, year = {2025}, }
• (2025). Quantum entanglement enables single-shot trajectory sensing for weakly interacting particles. PRL, 134(21), 210802. (www)

  @article{ , abstract = {Sensors for mapping the trajectory of an incoming particle find important utility in experimental high energy physics and searches for dark matter. For a quantum sensing protocol that uses projective measurements on a multiqubit sensor array to infer the trajectory of an incident particle, we establish that entanglement can dramatically reduce the particle-qubit interaction strength required for perfect trajectory discrimination. Within an interval of above this reduced threshold, any unentangled sensor requires repetitions of the protocol to estimate a previously unknown particle trajectory with error probability, whereas an entangled sensor can succeed with zero error in a single shot. Furthermore, entanglement can enhance trajectory sensing in realistic scenarios where varies continuously over the sensor qubits, exemplified by a Gaussian-profile laser pulse propagating through an array of atoms.}, archive = {J_PRL}, author = {Zachary E. Chin and David R. Leibrandt and Isaac L. Chuang}, doi = {10.1103/PhysRevLett.134.210802}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210802}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum entanglement enables single-shot trajectory sensing for weakly interacting particles}, volume = {134}, year = {2025}, }
• (2025). Experimental single-photon quantum key distribution surpassing the fundamental weak coherent-state rate limit. PRL, 134(21), 210801. (www)

  @article{ , abstract = {Quantum key distribution (QKD) offers a secure means of communication based on the laws of quantum physics. Despite its remarkable advancements, the current reliance of QKD on attenuated coherent (laser) light sources has imposed a fundamental limit on the secure key rate (SKR) per channel use. This constraint stems from the scarcity of single-photon components within coherent light, inherently bounded by a maximum of . Here, we report comprehensive demonstrations of single-photon-source-based high-rate QKD, surpassing the fundamental SKR limit imposed by the weak coherent light. By employing an on-demand, bright single-photon source with an efficiency of 0.71(2), coupled with narrow-bandwidth filtering and random polarization modulation, we demonstrated a field QKD trial over a 14.6(1.1) dB-loss free-space urban channel, achieving a SKR of per pulse. This SKR surpasses the practical limit of weak coherent-light-based QKD by 79%. These findings unequivocally demonstrate the superior performance of single-photon sources over weak coherent light for QKD applications, marking a pivotal stride towards realizing a global quantum internet.}, archive = {J_PRL}, author = {Yang Zhang and Xing Ding and Yang Li and Likang Zhang and Yong-Peng Guo and Gao-Qiang Wang and Zhen Ning and Mo-Chi Xu and Run-Ze Liu and Jun-Yi Zhao and Geng-Yan Zou and Hui Wang and Yuan Cao and Yu-Ming He and Cheng-Zhi Peng and Yong-Heng Huo and Sheng-Kai Liao and Chao-Yang Lu and Feihu Xu and Jian-Wei Pan}, doi = {10.1103/PhysRevLett.134.210801}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210801}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental single-photon quantum key distribution surpassing the fundamental weak coherent-state rate limit}, volume = {134}, year = {2025}, }
• (2025). How much entanglement is needed for quantum error correction?. PRL, 134(21), 210602. (www)

  @article{ , abstract = {It is commonly believed that logical states of quantum error-correcting codes have to be highly entangled such that codes capable of correcting more errors require more entanglement to encode a qubit. Here, we show that the validity of this belief depends on the specific code and the choice of entanglement measure. To this end, we characterize a tradeoff between the code distance quantifying the number of correctable errors, and the geometric entanglement measure of logical states quantifying their maximal overlap with product states or more general “topologically trivial” states. The maximum overlap is shown to be exponentially small in for three families of codes: (1) low-density parity check codes with commuting check operators, (2) stabilizer codes, and (3) codes with a constant encoding rate. Equivalently, the geometric entanglement of any logical state of these codes grows at least linearly with . On the opposite side, we also show that this distance-entanglement tradeoff does not hold in general. For any constant and (number of logical qubits), we show there exists a family of codes such that the geometric entanglement of some logical states approaches zero in the limit of large code length.}, archive = {J_PRL}, author = {Sergey Bravyi and Dongjin Lee and Zhi Li and Beni Yoshida}, doi = {10.1103/PhysRevLett.134.210602}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210602}, shortjournal = {Phys. Rev. Lett.}, title = {How much entanglement is needed for quantum error correction?}, volume = {134}, year = {2025}, }
• (2025). Quantum random access memory with transmon-controlled phonon routing. PRL, 134(21), 210601. (www)

  @article{ , abstract = {Quantum random access memory (QRAM) promises simultaneous data queries at multiple memory locations, with data retrieved in coherent superpositions, essential for achieving quantum speedup in many quantum algorithms. We introduce a transmon-controlled phonon router and propose a QRAM implementation by connecting these routers in a treelike architecture. The router controls the motion of itinerant surface acoustic wave phonons based on the state of the control transmon, implementing the core functionality of conditional routing for QRAM. Our QRAM design is compact, supports fast routing operations, and avoids frequency crowding. Additionally, we propose a hybrid dual-rail encoding method to detect dominant loss errors without additional hardware, a versatile approach applicable to other QRAM platforms. Our estimates indicate that the proposed QRAM platform can achieve high heralding rates using current device parameters, with heralding fidelity primarily limited by transmon dephasing.}, archive = {J_PRL}, author = {Zhaoyou Wang and Hong Qiao and Andrew N. Cleland and Liang Jiang}, doi = {10.1103/PhysRevLett.134.210601}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210601}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum random access memory with transmon-controlled phonon routing}, volume = {134}, year = {2025}, }
• (2025). Exact volume-law entangled zero-energy eigenstates in a large class of spin models. PRL, 134(21), 210403. (www)

  @article{ , abstract = {Exact solutions for excited states in nonintegrable quantum Hamiltonians have revealed novel dynamical phenomena that can occur in quantum many-body systems. This work proposes a method to analytically construct a specific set of volume-law entangled zero-energy exact excited eigenstates in a large class of spin Hamiltonians. In particular, we show that all spin chains that satisfy a simple set of conditions host exact volume law entangled zero-energy eigenstates in the middle of their spectra. Examples of physically relevant spin chains of this type include the transverse-field Ising model, PXP model, spin- model, and spin- Kitaev chain. Although these eigenstates are highly atypical in their structure, they are thermal with respect to local observables. Our framework also unifies many recent constructions of volume-law entangled eigenstates in the literature. Finally, we show that a similar construction also generalizes to spin models on graphs in arbitrary dimensions.}, archive = {J_PRL}, author = {Sashikanta Mohapatra and Sanjay Moudgalya and Ajit C. Balram}, doi = {10.1103/PhysRevLett.134.210403}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210403}, shortjournal = {Phys. Rev. Lett.}, title = {Exact volume-law entangled zero-energy eigenstates in a large class of spin models}, volume = {134}, year = {2025}, }
• (2025). Entanglement oscillations from many-body quantum scars. PRL, 134(21), 210402. (www)

  @article{ , abstract = {Quantum scars are nonthermal eigenstates that prevent thermalization of initial states with weight on the scars. When the scar states are equally spaced in energy, superpositions of scars show oscillating local observables that can be detected in experiments. However, we note that scarred models in the literature show fundamentally different scar entanglement dynamics: some show entanglement oscillations while others are completely frozen. We explain this freezing through a no-go theorem which we apply to more than a dozen scarred models in the literature. We also discuss a method for evading the no-go theorem by deforming the scarred models with frozen scar entanglement dynamics.}, archive = {J_PRL}, author = {Nicholas O’Dea and Adithya Sriram}, doi = {10.1103/PhysRevLett.134.210402}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210402}, shortjournal = {Phys. Rev. Lett.}, title = {Entanglement oscillations from many-body quantum scars}, volume = {134}, year = {2025}, }
• (2025). Quantum decoherence from complex saddle points. PRL, 134(21), 210401. (www)

  @article{ , abstract = {Quantum decoherence is the effect that bridges quantum physics to well-understood classical physics. As such, it plays a crucial role in understanding the mysterious nature of quantum physics. Quantum decoherence is also a source of quantum noise that has to be well under control in quantum computing and in various experiments based on quantum technologies. Here we point out that quantum decoherence can be captured by complex saddle points in the Feynman path integral in much the same way as quantum tunneling can be captured by instantons. In particular, we present some first-principle calculations in the Caldeira–Leggett model, which reproduce the predicted scaling behavior of quantum decoherence with respect to the parameters of the environment such as the temperature and the coupling to the system of interest. We also discuss how to extend our approach to general models by Monte Carlo calculations using a recently developed method to overcome the sign problem.}, archive = {J_PRL}, author = {Jun Nishimura and Hiromasa Watanabe}, doi = {10.1103/PhysRevLett.134.210401}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum decoherence from complex saddle points}, volume = {134}, year = {2025}, }
• (2025). Device-independent full network nonlocality for arbitrary-party and unbounded-input scenario. PRL, 134(21), 210203. (www)

  @article{ , abstract = {The nonlocality arising in a multiparty network involving multiple independent sources radically differs from the standard multipartite Bell nonlocality involving a single source. The notion of the full network nonlocality (FNN) [A. Pozas-Kerstjens et al. , Full network nonlocality, Phys. Rev. Lett. 128 , 010403 (2022) ] characterizes the quantum correlations that cannot be reproduced by a local-nonlocal model featuring one local source and the rest of nonlocal no-signaling sources. However, the demonstration of FNN was limited to bilocal and trilocal star-shaped network scenarios involving three or two dichotomic measurements for edge parties. In this Letter, we first demonstrate that a large class of prevailing network inequalities does not exhibit FNN. We then introduce an elegant set of arbitrary-party and unbounded-input network inequalities in star-shaped and linear-chain networks whose optimal quantum violation exhibits FNN, certifying that the nonlocality is genuinely distributed to the entire network. Contrasting to existing demonstrations of FNN that inevitably require fixed-input and four-output elegant joint measurements for the central party, our generalized inequalities are more experimentally friendly, requiring only two output measurements. Moreover, our derivation of optimal quantum violation is fully analytic and devoid of assuming the dimension of the quantum system, thereby showcasing its potential for device-independent self-testing.}, archive = {J_PRL}, author = {Sneha Munshi and A. K. Pan}, doi = {10.1103/PhysRevLett.134.210203}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210203}, shortjournal = {Phys. Rev. Lett.}, title = {Device-independent full network nonlocality for arbitrary-party and unbounded-input scenario}, volume = {134}, year = {2025}, }
• (2025). Experimental certification of high-dimensional entanglement with randomized measurements. PRL, 134(21), 210202. (www)

  @article{ , abstract = {High-dimensional entangled states offer higher information capacity and stronger resilience to noise compared with two-dimensional systems. However, the large number of modes and sensitivity to random rotations complicate experimental entanglement certification. Here, we experimentally certify three-dimensional entanglement in a five-dimensional two-photon state using 800 Haar-random measurements implemented via a ten-plane programmable light converter. We further demonstrate the robustness of this approach against random rotations, certifying high-dimensional entanglement despite arbitrary phase randomization of the optical modes. This method, which requires no common reference frame between parties, opens the door for high-dimensional entanglement distribution through long-range random links.}, archive = {J_PRL}, author = {Ohad Lib and Shuheng Liu and Ronen Shekel and Qiongyi He and Marcus Huber and Yaron Bromberg and Giuseppe Vitagliano}, doi = {10.1103/PhysRevLett.134.210202}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210202}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental certification of high-dimensional entanglement with randomized measurements}, volume = {134}, year = {2025}, }
• (2025). Experimental realization of genuine three-copy collective measurements for optimal information extraction. PRL, 134(21), 210201. (www)

  @article{ , abstract = {Nonclassical phenomena tied to entangled states are the focus of foundational studies and powerful resources in many applications. By contrast, the counterparts on quantum measurements are still poorly understood. Notably, genuine multipartite nonclassicality is barely discussed, let alone its experimental realization. Here we experimentally demonstrate the power of genuine tripartite nonclassicality in quantum measurements based on a simple estimation problem. To this end we realize an optimal genuine three-copy collective measurement via a nine-step two-dimensional photonic quantum walk with 30 elaborately designed coin operators. Then we realize an optimal estimation protocol and achieve an unprecedented high estimation fidelity, which can beat all strategies based on restricted collective measurements by more than 11 standard deviations. These results clearly demonstrate that genuine collective measurements can extract more information than local measurements and restricted collective measurements. Our Letter opens the door for exploring genuine multipartite nonclassical measurements and their power in quantum information processing.}, archive = {J_PRL}, author = {Kai Zhou and Changhao Yi and Wen-Zhe Yan and Zhibo Hou and Huangjun Zhu and Guo-Yong Xiang and Chuan-Feng Li and Guang-Can Guo}, doi = {10.1103/PhysRevLett.134.210201}, journal = {Physical Review Letters}, month = {5}, number = {21}, pages = {210201}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental realization of genuine three-copy collective measurements for optimal information extraction}, volume = {134}, year = {2025}, }
• (2025). Universal relationship between linear viscoelasticity and nonlinear yielding in soft materials. PRL, 134(20), 208202. (www)

  @article{ , abstract = {The nonlinear response of yield stress fluids remains difficult to predict and control. Here, we show that the height of the overshoot in the loss modulus , a key characteristic of yielding, depends only on linear viscoelastic properties. Furthermore, the position of this overshoot depends on linear viscoelastic and flow properties, demonstrating the important and enduring role of elasticity in yielding. The physics governing linear viscoelasticity is therefore not only preserved during yielding but also controls two commonly reported yielding metrics.}, archive = {J_PRL}, author = {Daniel P. Keane and Elnaz Nikoumanesh and Krutarth M. Kamani and Simon A. Rogers and Ryan Poling-Skutvik}, doi = {10.1103/PhysRevLett.134.208202}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {208202}, shortjournal = {Phys. Rev. Lett.}, title = {Universal relationship between linear viscoelasticity and nonlinear yielding in soft materials}, volume = {134}, year = {2025}, }
• (2025). Morphogenesis of cheese flowers through scraping. PRL, 134(20), 208201. (www)

  @article{ , abstract = {The “Tête de Moine” Swiss cheese is generally served by scraping the surface of a cylindrical loaf with a sharp tool. This produces thin sheets of cheese that are strongly wrinkled at the edge, resembling frilly flowers and enhancing the tasting experience. In this Letter we unveil the physical mechanisms at play in this scraping-induced morphogenesis. We measure the deformation of the cheese during scraping and show that plastic deformation occurs everywhere, but find a larger plastic contraction in the inner part of the flower, causing its buckling into shape. We show that it surprisingly derives from the lower friction coefficient evidenced on the cheese close to its crust. Our analysis provides the tools for a better control of flower chip morphogenesis through plasticity in the shaping of other delicacies, but also in metal cutting.}, archive = {J_PRL}, author = {J. Zhang and A. Ibarra and B. Roman and M. Ciccotti}, doi = {10.1103/PhysRevLett.134.208201}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {208201}, shortjournal = {Phys. Rev. Lett.}, title = {Morphogenesis of cheese flowers through scraping}, volume = {134}, year = {2025}, }
• (2025). Ensemble inequivalence and phase transitions in unlabeled networks. PRL, 134(20), 207401. (www)

  @article{ , abstract = {We discover a first-order phase transition in the canonical ensemble of random unlabeled networks with a prescribed average number of links. The transition is caused by the nonconcavity of microcanonical entropy. Above the critical point coinciding with the graph symmetry phase transition, the canonical and microcanonical ensembles are equivalent and have a well-behaved thermodynamic limit. Below the critical point, the ensemble equivalence is broken, and the canonical ensemble is a mixture of phases: empty networks and networks with average degrees diverging logarithmically with the network size. As a consequence, networks with bounded average degrees do not survive in the thermodynamic limit, decaying into the empty phase. The celebrated percolation transition in labeled networks is thus absent in unlabeled networks. In view of these differences between labeled and unlabeled ensembles, the question of which one should be used as a null model of different real-world networks cannot be ignored.}, archive = {J_PRL}, author = {Oleg Evnin and Dmitri Krioukov}, doi = {10.1103/PhysRevLett.134.207401}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {207401}, shortjournal = {Phys. Rev. Lett.}, title = {Ensemble inequivalence and phase transitions in unlabeled networks}, volume = {134}, year = {2025}, }
• (2025). Unified interface model for dissipative transport of bosons and fermions. PRL, 134(20), 207102. (www)

  @article{ , abstract = {We study the directed transport of bosons along a one dimensional lattice in a dissipative setting, where the hopping is only facilitated by coupling to a Markovian reservoir. By combining numerical simulations with a field-theoretic analysis, we investigate the current fluctuations for this process and determine its asymptotic behavior. These findings demonstrate that dissipative bosonic transport belongs to the Kardar-Parisi-Zhang universality class and therefore, in spite of the drastic difference in the underlying particle statistics, it features the same coarse-grained behavior as the corresponding asymmetric simple exclusion process for fermions. However, crucial differences between the two processes emerge when focusing on the full counting statistics of current fluctuations. By mapping both models to the physics of fluctuating interfaces, we find that dissipative transport of bosons and fermions can be understood as surface growth and erosion processes, respectively. Within this unified description, both the similarities and discrepancies between the full counting statistics of the transport are reconciled. Beyond purely theoretical interest, these findings are relevant for experiments with cold atoms or long-lived quasiparticles in nanophotonic lattices, where such transport scenarios can be realized.}, archive = {J_PRL}, author = {Y. Minoguchi and J. Huber and L. Garbe and A. Gambassi and P. Rabl}, doi = {10.1103/PhysRevLett.134.207102}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {207102}, shortjournal = {Phys. Rev. Lett.}, title = {Unified interface model for dissipative transport of bosons and fermions}, volume = {134}, year = {2025}, }
• (2025). Hydrodynamically consistent many-body harada-sasa relation. PRL, 134(20), 207101. (www)

  @article{ , abstract = {The effect of hydrodynamic interactions on the nonequilibrium stochastic dynamics of particles—arising from the conservation of momentum in the fluid medium—is examined in the context of the relationship between fluctuations, response functions, and the entropy production rate. The multiplicative nature of the hydrodynamic interactions is shown to introduce subtleties that preclude a straightforward extension of the Harada-Sasa relation. A generalization of the definitions involved in the framework is used to propose a new form of the relation applicable to systems with hydrodynamic interactions. The resulting framework will enable characterization of the nonequilibrium properties of living and active matter systems, which are predominantly in suspensions.}, archive = {J_PRL}, author = {Ramin Golestanian}, doi = {10.1103/PhysRevLett.134.207101}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {207101}, shortjournal = {Phys. Rev. Lett.}, title = {Hydrodynamically consistent many-body harada-sasa relation}, volume = {134}, year = {2025}, }
• (2025). Picocavity-enhanced raman spectroscopy of physisorbed h2 and d2 molecules. PRL, 134(20), 206901. (www)

  @article{ , abstract = {We report on tip-enhanced Raman spectroscopy of H 2 and D 2 molecules physisorbed within a plasmonic picocavity at 10 K. The intense Raman peaks resulting from the rotational and vibrational transitions are observed at subnanometer gap distances of the junction formed by an Ag tip and an Ag(111) surface, where a picocavity-enhanced field plays a crucial role. A significant redshift of the H-H stretch frequency is observed as the gap distance decreases, while the D-D stretch frequency is unaffected. Density functional theory, path-integral molecular dynamics, and quantum anharmonic vibrational energy calculations suggest that this unexpected isotope effect is explained by a different molecular density between H 2 and D 2 on the surface.}, archive = {J_PRL}, author = {Akitoshi Shiotari and Shuyi Liu and George Trenins and Toshiki Sugimoto and Martin Wolf and Mariana Rossi and Takashi Kumagai}, doi = {10.1103/PhysRevLett.134.206901}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206901}, shortjournal = {Phys. Rev. Lett.}, title = {Picocavity-enhanced raman spectroscopy of physisorbed h2 and d2 molecules}, volume = {134}, year = {2025}, }
• (2025). Nonreciprocal phonons in PT-symmetric antiferromagnets. PRL, 134(20), 206701. (www)

  @article{ , abstract = {Phonon nonreciprocity, indicating different transport properties along opposite directions, has been observed in experiments under a magnetic field. We show that nonreciprocal acoustic phonons can also exist without a magnetic field or net magnetization. We identify crucial contributions in phenomenological elastic theory. In symmetric antiferromagnets, we find two terms, dubbed flexo viscosity and flexo torque, that induce phonon nonreciprocity. The microscopic origin of these terms is attributed to the derivatives of molecular Berry curvature, manifested as emergent nonlocal magnetic fields on phonons. The symmetry breaking that originated from spin order is transferred to the phonon system through spin-orbit coupling, where the orbital degree of freedom affects the lattice dynamics directly. By electrically breaking inversion symmetry and modifying the spin-orbit coupling, we find extra contributions and show that both the phonon nonreciprocity and helicity can be controlled and enhanced. Importantly, the phonon nonreciprocity is an odd function of the Néel vector, serving as an indicator of the order parameter.}, archive = {J_PRL}, author = {Yafei Ren and Daniyar Saparov and Qian Niu}, doi = {10.1103/PhysRevLett.134.206701}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206701}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal phonons in PT-symmetric antiferromagnets}, volume = {134}, year = {2025}, }
• (2025). Unconventional topological edge states in one-dimensional non-hermitian gapless systems stemming from nonisolated hypersurface singularities. PRL, 134(20), 206603. (www)

  @article{ , abstract = {Topologically protected edge states have been extensively studied in systems characterized by the topological invariants in band gaps (also called line gaps). In this study, we unveil a whole new form of edge states supported by non-Hermitian systems that transcends the established paradigms of band-gap topology. In contrast to the traditional stable edge states in topological insulators with specific band gaps, the one-dimensional systems we investigate are inherently gapless with the Brillouin zones being mapped to the loops encircling hypersurface singularities in a higher-dimensional space with parity-time symmetry. These hypersurface singularities are nonisolated degeneracies embedded entirely on exceptional surfaces, rendering the energy gaps in our systems inevitably closed at the intersections of the Brillouin zone loop and the exceptional surfaces. Unexpectedly, such gapless systems still afford topologically protected edge states at system boundaries, challenging the conventional understanding based on band gaps. To elucidate the existence of these edge states in the absence of a band-gap-based invariant, we propose a theoretical framework based on eigenframe rotation and deformation that incorporates non-Bloch band theory. Finally, we experimentally demonstrate this new form of topological edge states with nonreciprocal circuits for the first time. Our work extends topological edge states from gapped phases to gapless phases, offering new insights into topological phenomena.}, archive = {J_PRL}, author = {Hongwei Jia and Jing Hu and Ruo-Yang Zhang and Yixin Xiao and Dongyang Wang and Mudi Wang and Shaojie Ma and Xiaoping Ouyang and Yifei Zhu and C. T. Chan}, doi = {10.1103/PhysRevLett.134.206603}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206603}, shortjournal = {Phys. Rev. Lett.}, title = {Unconventional topological edge states in one-dimensional non-hermitian gapless systems stemming from nonisolated hypersurface singularities}, volume = {134}, year = {2025}, }
• (2025). Fractionalized superconductivity mediated by majorana fermions in the kitaev-kondo lattice. PRL, 134(20), 206602. (www)

  @article{ , abstract = {Superconductivity usually emerges from a metallic normal state which follows the Fermi-liquid paradigm. If, in contrast, the normal state is a fractionalized non-Fermi liquid, then pairing may either eliminate fractionalization via a Higgs-type mechanism leading to a conventional superconducting state, or pairing can occur in the presence of fractionalization. Here, we discuss a simple model for the latter case: using a combination of perturbation theory and functional renormalization group, we show that the Kitaev-Kondo lattice model displays a fractionalized superconducting phase at weak Kondo coupling. This phase is characterized by Cooper pairing of conventional electronic quasiparticles, coexisting with a spin-liquid background and topological order. Depending on the sign of the Kitaev coupling, we find the pairing to be either of chiral -wave or -wave type for extended doping regions around the van Hove filling. We discuss applications and extensions.}, archive = {J_PRL}, author = {Matthew Bunney and Urban F. P. Seifert and Stephan Rachel and Matthias Vojta}, doi = {10.1103/PhysRevLett.134.206602}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206602}, shortjournal = {Phys. Rev. Lett.}, title = {Fractionalized superconductivity mediated by majorana fermions in the kitaev-kondo lattice}, volume = {134}, year = {2025}, }
• (2025). Observation of extreme anisotropic sensitivity at topological bound states in the continuum. PRL, 134(20), 206601. (www)

  @article{ , abstract = {Bound states in the continuum (BICs) are exceptional resonances with extremely high sensitivity and thus inherently fragile. Introducing topological concepts can fortify BICs against perturbations; however, existing topological BICs (TBICs) often rely on intricate strategies. Here, we explore the universality of TBICs governed by symmetry. Different symmetries naturally segregate wave states into uncoupled Hilbert subspaces, enabling independent topological band structure engineering in each subspace. This results in rich topological features, including TBICs, topological Fano resonance, and even exotic TBICs (eTBICs). Intriguingly, eTBICs inherit core attributes from both topological states and BICs, thereby exhibiting counterintuitive behavior—both strong immunity and high sensitivity. We conceptually and experimentally demonstrate this using an acoustic monolayer topological waveguide, uncovering exotic behavior in the transmission spectrum where the bulk is “muted” and the eTBIC is identified with extreme anisotropic sensitivity. Our findings may enrich the research implications of both topological physics and BICs.}, archive = {J_PRL}, author = {Ruizhi Dong and Yihuan Zhu and Dongxing Mao and Xu Wang and Yong Li}, doi = {10.1103/PhysRevLett.134.206601}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of extreme anisotropic sensitivity at topological bound states in the continuum}, volume = {134}, year = {2025}, }
• (2025). Band-selective spin-charge separation across the charge density wave transition in quasi-1D NbSe3. PRL, 134(20), 206402. (www)

  @article{ , abstract = {Non-Fermi liquid (non-FL) phase is a pivotal enigma in understanding intriguing quantum phases in strongly correlated systems, such as high-temperature superconductivity. Tomonaga-Luttinger liquid (TLL) theory, designed for one-dimensional (1D) systems, serves as one of the microscopic frameworks that elucidates non-FL behavior. Despite its theoretical concreteness, comprehensive experimental verification has remained incomplete. In particular, addressing the persistence of the TLL nature within ordered phases, such as charge density wave (CDW), has posed a significant challenge. We report the observation of TLL characteristics across the CDW transitions in a quasi-1D material using angle-resolved photoemission spectroscopy. Spin-charge separation, a disentanglement of spin and charge degrees of freedom of electrons, is clearly observed within the band, accompanied by the suppression of spectral weight following a power-law behavior with anticipated temperature scaling. Surprisingly, the spin-charge separation persists even below the CDW transition temperatures, indicating the validity of the TLL nature in the CDW phase. Our findings offer a unique opportunity to explore the interplay between the TLL and ordered phases, which could be connected to the interplay between non-FL and ordered phases in strongly correlated systems.}, archive = {J_PRL}, author = {Jounghoon Hyun and Yeonghoon Lee and Chan-young Lim and Gyubin Lee and Jaehun Cha and Yeojin Ahn and Mingi Jho and Seonggeon Gim and Minkyu Park and Makoto Hashimoto and Donghui Lu and Yeongkwan Kim and Sunghun Kim}, doi = {10.1103/PhysRevLett.134.206402}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206402}, shortjournal = {Phys. Rev. Lett.}, title = {Band-selective spin-charge separation across the charge density wave transition in quasi-1D NbSe3}, volume = {134}, year = {2025}, }
• (2025). Advancing natural orbital functional calculations through deep learning-inspired techniques for large-scale strongly correlated electron systems. PRL, 134(20), 206401. (www)

  @article{ , abstract = {Natural orbital functional (NOF) theory provides a valuable framework for studying strongly correlated systems at an affordable computational cost, with an accuracy comparable to highly demanding wave-function-based methods. However, its widespread adoption in cases involving a large number of correlated electrons has been limited by the extensive iterations required for convergence. In this Letter, we present an approach that integrates the techniques used for optimization in deep learning into NOF calculations, enabling a substantial expansion in the scale of accessible systems. The proposed procedure employs an adaptive momentum-based technique for orbital optimization, alternated with the optimization of occupation numbers, significantly improving the computational feasibility of challenging calculations. We illustrate the capabilities of our approach through three challenging test cases: (i) the symmetric dissociation of a large hydrogen cluster with 1000 electrons, (ii) an analysis of occupancy distributions in fullerenes, and (iii) a study of the singlet-triplet energy gap in linear acenes. These examples demonstrate the method’s applicability to large-scale systems and strongly correlated electron phenomena, extending the reach of NOF theory to increasingly complex systems.}, archive = {J_PRL}, author = {Juan Felipe Huan Lew-Yee and Jorge M. del Campo and Mario Piris}, doi = {10.1103/PhysRevLett.134.206401}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206401}, shortjournal = {Phys. Rev. Lett.}, title = {Advancing natural orbital functional calculations through deep learning-inspired techniques for large-scale strongly correlated electron systems}, volume = {134}, year = {2025}, }
• (2025). Quantum monte carlo study of hydrodynamics in systems with particle-hole symmetry. PRL, 134(20), 206303. (www)

  @article{ , abstract = {The emergence of hydrodynamic behavior in electronic flow within clean, particle-hole-symmetric systems at half filling is a nontrivial problem. Navier-Stokes (NS) equations describe the momentum flow, while experimental measurements typically capture the current flow profiles. However, in particle-hole-symmetric systems, electric current and momentum flow are entirely decoupled, because electrons and holes move in opposite directions with equal distribution functions. This makes it challenging to link NS equations to observed flow patterns. In this Letter, we demonstrate that the hydrodynamic behavior of the charge current at half filling can emerge despite the absence of momentum flow. By combining Boltzmann transport theory with numerically exact quantum Monte Carlo simulations of clean graphene samples, we show that NS-type equations can be derived directly for the charge current, eliminating the need for any additional mechanism coupling the velocity field and charge current in explaining the experimentally observed hydrodynamic flow profiles in graphene at half filling. We show that a new transport quantity—the current diffusion coefficient—replaces viscosity and expect this description to be valid for any particle-hole-symmetric system. Our results provide new insights into the interpretation of experimental data and demonstrate how quantum Monte Carlo calculations can serve as an alternative to experiments in transport measurements to verify the kinetic theory results.}, archive = {J_PRL}, author = {Adrien Reingruber and Kitinan Pongsangangan and Fakher Assaad and Maksim Ulybyshev}, doi = {10.1103/PhysRevLett.134.206303}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206303}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum monte carlo study of hydrodynamics in systems with particle-hole symmetry}, volume = {134}, year = {2025}, }
• (2025). Caroli–de Gennes–Matricon analogs in full-shell hybrid nanowires. PRL, 134(20), 206302. (www)

  @article{ , abstract = {We report tunneling spectroscopy of Andreev subgap states in hybrid nanowires with a thin superconducting full shell surrounding a semiconducting core. The combination of the quantized fluxoid of the shell and the Andreev reflection at the superconductor-semiconductor interface gives rise to analogs of Caroli–de Gennes–Matricon states found in Abrikosov vortices in type-II superconductors. Unlike in metallic superconductors, Caroli–de Gennes–Matricon analogs in full-shell hybrid nanowires manifest as one-dimensional Van Hove singularities with energy spacings comparable to the superconducting gap and independent of the Fermi energy, making them readily observable. Evolution of these analogs with axial magnetic field, skewed within the Little-Parks lobe structure, is consistent with theory and yields information about the radial distribution and angular momenta of the corresponding subbands.}, archive = {J_PRL}, author = {M. T. Deng and Carlos Payá and Pablo San-Jose and Elsa Prada and C. M. Marcus and S. Vaitiekėnas}, doi = {10.1103/PhysRevLett.134.206302}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206302}, shortjournal = {Phys. Rev. Lett.}, title = {Caroli–de Gennes–Matricon analogs in full-shell hybrid nanowires}, volume = {134}, year = {2025}, }
• (2025). Universal charge conductance at Abelian–Non-abelian quantum hall interfaces. PRL, 134(20), 206301. (www)

  @article{ , abstract = {Multiple topologically distinct quantum Hall phases can occur at the same Landau level filling factor. It is a major challenge to distinguish between these phases as they only differ by the neutral modes, which do not affect the charge conductance in conventional geometries. We show that the neutral sector can be determined with coherent charge conductance in a π -shaped geometry that interfaces three different filling factors. Specifically, non-Abelian paired states at a half-filled Landau level and the anti-Read-Rezayi state can be identified. Interestingly, for interfaces between paired states and Jain states, the electric current in the π geometry behaves as if pairs of neutral Majorana edge modes were charge modes of Jain states.}, archive = {J_PRL}, author = {Misha Yutushui and Ady Stern and David F. Mross}, doi = {10.1103/PhysRevLett.134.206301}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206301}, shortjournal = {Phys. Rev. Lett.}, title = {Universal charge conductance at Abelian–Non-abelian quantum hall interfaces}, volume = {134}, year = {2025}, }
• (2025). Superconductivity and charge density wave in the holstein model on the penrose lattice. PRL, 134(20), 206001. (www)

  @article{ , abstract = {The exotic quantum states emerging in the quasicrystal (QC) have attracted extensive interest because of various properties absent in the crystal. In this Letter, we systematically study the Holstein model at half filling on a prototypical structure of QC, namely rhombic Penrose lattice, aiming at investigating the superconductivity (SC) and other intertwined ordering arising from the interplay between quasiperiodicity and electron-phonon interaction. Through unbiased sign-problem-free determinant quantum Monte Carlo simulations, we reveal the salient features of the ground state phase diagram. Distinct from the results on bipartite periodic lattices at half filling, SC is dominant in a large parameter regime of the electron-phonon coupling (EPC) strength on the Penrose lattice. The strongest SC emerges in the intermediate EPC strength regime, where it coexists with the charge density wave. The charge density wave dominates the SC only in the sufficiently strong EPC regime. Our results also reveal pronounced pairing fluctuation above the transition temperature of the SC. The strong pairing and its fluctuation originate from the cooperative effects of the QC structure without translational symmetry and the macroscopically degenerate confined states at the Fermi energy, which uniquely exist on the Penrose lattice. Our unbiased numerical results suggest that the Penrose lattice is a potential platform to realize strong SC pairing, providing a promising avenue to discover relatively high- SC predominantly induced by the EPC.}, archive = {J_PRL}, author = {Lu Liu and Zi-Xiang Li and Fan Yang}, doi = {10.1103/PhysRevLett.134.206001}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {206001}, shortjournal = {Phys. Rev. Lett.}, title = {Superconductivity and charge density wave in the holstein model on the penrose lattice}, volume = {134}, year = {2025}, }
• (2025). Drift-energy replacement effect in multi-ion magnetized plasma. PRL, 134(20), 205101. (www)

  @article{ , abstract = {Fast rotation can improve the stability and confinement of fusion plasmas. However, to maintain a rapidly rotating fusion plasma in steady state, significant energy must be invested in spinning up each incoming fuel ion. We show here that, under the right circumstances, collisional cross-field radial fueling can directly transfer drift energy between outgoing and incoming ions without the need for external power recirculation, thereby reducing the energy costs of maintaining the rotation.}, archive = {J_PRL}, author = {M. E. Mlodik and E. J. Kolmes and N. J. Fisch}, doi = {10.1103/PhysRevLett.134.205101}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {205101}, shortjournal = {Phys. Rev. Lett.}, title = {Drift-energy replacement effect in multi-ion magnetized plasma}, volume = {134}, year = {2025}, }
• (2025). Intense X-ray vortices generation via wavefront shaping in high-gain free-electron lasers. PRL, 134(20), 205001. (www)

  @article{ , abstract = {The x-ray vortex optical beam, distinguished by its topological charge and orbital angular momentum, offers new insights in probing complex electronic structures, enhancing material characterization, and advancing high-resolution imaging techniques. Here we propose a novel and reliable method to generate intense x-ray vortices with tunable wavelengths in high-gain free-electron lasers (FELs). By simply adjusting the wavefront tilt of the radiation pulse during the FEL gain process, high-quality vortex beam can be amplified until saturation. Compared with existing methods for FEL vortex generation, the proposed technique offers broader wavelength tunability and can be easily implemented in high-gain FEL facilities, regardless of the operating modes.}, archive = {J_PRL}, author = {Zhikai Zhou and Yin Kang and Weishi Wan and Chao Feng}, doi = {10.1103/PhysRevLett.134.205001}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {205001}, shortjournal = {Phys. Rev. Lett.}, title = {Intense X-ray vortices generation via wavefront shaping in high-gain free-electron lasers}, volume = {134}, year = {2025}, }
• (2025). Structural heterogeneity of MgSiO3 liquid and its connection with dynamical properties. PRL, 134(20), 204101. (www)

  @article{ , abstract = {Silicate melts not only govern key processes in the Earth’s early evolution, but also significantly influence its interior dynamics today. , a primary component of silicate melts, undergoes significant structural changes and exhibits complex macroscopic properties from the Earth’s surface to the core-mantle boundary. Despite extensive studies, the atomic structure, densification mechanisms, and their connection to dynamics remain unclear. In this Letter, using molecular dynamics simulations with a deep neural network potential, we investigate the atomic structure of liquid. Our results reveal significant structural heterogeneity in liquid, with distinct Mg- and Si-enriched regions present throughout the entire mantle pressure range. This heterogeneity offers a new perspective on understanding the densification mechanism, and explains the atomic origin of the viscosity anomaly, as the lifetime of structural heterogeneity aligns well with the Maxwell relaxation time. Our findings provide new insights into the behavior of silicate melts under extreme conditions.}, archive = {J_PRL}, author = {Shiwei Zhang and Junwei Hu and Xuecheng Sun and Jie Deng and Haiyang Niu}, doi = {10.1103/PhysRevLett.134.204101}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {204101}, shortjournal = {Phys. Rev. Lett.}, title = {Structural heterogeneity of MgSiO3 liquid and its connection with dynamical properties}, volume = {134}, year = {2025}, }
• (2025). Out-of-equilibrium fluxes shape the self-organization of locally interacting turbulence. PRL, 134(20), 204001. (www)

  @article{ , abstract = {We study the self-organization of turbulence in a geophysically motivated two-dimensional fluid with local interactions. Using simulations and theory, we show that the out-of-equilibrium flux to small scales imposes a constraint on the large-scale emergent flow. Consequently, a rich phase diagram of large-scale configurations emerges, replacing the unique state found in flows with energy injection below the interaction scale. We explain what sets the boundaries between the different phases and the occurrence of spontaneous symmetry breaking. This letter demonstrates that the selection mechanism of large-scale structures in quasigeostrophic flows can be dramatically altered by forcing above the interaction scale.}, archive = {J_PRL}, author = {Anton Svirsky and Anna Frishman}, doi = {10.1103/PhysRevLett.134.204001}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {204001}, shortjournal = {Phys. Rev. Lett.}, title = {Out-of-equilibrium fluxes shape the self-organization of locally interacting turbulence}, volume = {134}, year = {2025}, }
• (2025). One-way valley-robust transport in edge-tailored photonic crystals. PRL, 134(20), 203803. (www)

  @article{ , abstract = {Valley photonics, with its rapid advancements and immense potential, lays one pivotal cornerstone toward next-generation topological photonic devices. It enables valley-polarized topological states, whose valleys are intrinsically locked up with transmission directivity. However, these states are prone to defects in photonic structures, and backscattering may easily induce valley flipping. Hence, achieving a one-way valley-robust photonic crystal, immune to perturbations, remains elusive. Here, we demonstrate a one-way, valley-polarized state in an edge-tailored photonic crystal that is robust against defects. Such crystal possesses a Chern band gap and is achieved without using an interface between two crystals with opposite Berry curvatures. We show -valley-robust transport in a defective crystal and demonstrate perfect conversion between the and valleys in a hybridized crystal while backscattering is greatly suppressed. Our results offer a promising approach for unidirectional control of the valley degrees of freedom in light.}, archive = {J_PRL}, author = {Jianfeng Chen and Yidong Zheng and Shuihua Yang and Fulong Shi and Zhi-Yuan Li and Cheng-Wei Qiu}, doi = {10.1103/PhysRevLett.134.203803}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203803}, shortjournal = {Phys. Rev. Lett.}, title = {One-way valley-robust transport in edge-tailored photonic crystals}, volume = {134}, year = {2025}, }
• (2025). Light-based chromatic aberration correction of ultrafast electron microscopes. PRL, 134(20), 203802. (www)

  @article{ , abstract = {We propose and theoretically demonstrate a technique that allows one to compensate for chromatic aberrations of traditional electron lenses in ultrafast electron microscopes. The technique is based on space- and time-dependent phase modulation of a pulsed electron beam using interaction with a shaped pulsed ponderomotive lens. The energy-selective focal distance is reached by combining the electron temporal chirp with the time-dependent size of the effective potential, with which the electrons interact. As a result, chromatic aberration can be reduced by up to a factor of 7. This approach paves the way for advanced transverse and longitudinal wave front shaping of electrons in free space.}, archive = {J_PRL}, author = {Marius Constantin Chirita Mihaila and Neli Laštovičková Streshkova and Martin Kozák}, doi = {10.1103/PhysRevLett.134.203802}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203802}, shortjournal = {Phys. Rev. Lett.}, title = {Light-based chromatic aberration correction of ultrafast electron microscopes}, volume = {134}, year = {2025}, }
• (2025). Encoding arbitrary ising hamiltonians on spatial photonic ising machines. PRL, 134(20), 203801. (www)

  @article{ , abstract = {Photonic Ising machines constitute an emergent new paradigm of computation geared toward tackling combinatorial optimization problems that can be reduced to the problem of finding the ground state of an Ising model. Spatial photonic Ising machines (SPIMs) have proven advantageous for simulating fully connected large-scale spin systems. Fine control of a general interaction matrix has been accomplished so far only through matrix decomposition methods. We introduce and experimentally validate a SPIM instance that enables direct control over the full interaction matrix, allowing the encoding of Ising Hamiltonians with arbitrary couplings and connectivity. We demonstrate the conformity of the experimentally measured Ising energy with the theoretically expected value and then proceed to solve both the unweighted and weighted graph partitioning problems, showcasing a systematic convergence to an optimal solution via simulated annealing. Our approach significantly expands the applicability of SPIMs for real-world applications, as it is more efficient than matrix decomposition methods in the case of sparse problems. It paves the way to encoding the full range of NP problems that are known to be equivalent to Ising models on SPIM devices.}, archive = {J_PRL}, author = {Jason Sakellariou and Alexis Askitopoulos and Georgios Pastras and Symeon I. Tsintzos}, doi = {10.1103/PhysRevLett.134.203801}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203801}, shortjournal = {Phys. Rev. Lett.}, title = {Encoding arbitrary ising hamiltonians on spatial photonic ising machines}, volume = {134}, year = {2025}, }
• (2025). Spatial mapping of intrinsic and readout nonlinearities in a strongly driven micromechanical membrane. PRL, 134(20), 203604. (www)

  @article{ , abstract = {Recently, it was shown that strongly driven micromechanical resonators show mode shapes that strongly differ from the eigenmodes [F. Yang et al. , Spatial modulation of nonlinear flexural vibrations of membrane resonators, Phys. Rev. Lett. 122 , 154301 (2019) ]. This raises the question of the origin of this nonlinear behavior. We measure the spatial dependence of the nonlinearities of high-stress micromechanical membranes. The mechanical nonlinearity is determined from the frequency response and is found to be independent of the probing location. It is the phase of the response that is instrumental in extracting that intrinsic nonlinearity. Our interferometric readout results in high-harmonics generation. These harmonics have a clear spatial profile that shows ringlike patterns resembling previous reports. These patterns are reproduced by a model of the displacement-dependent reflection signal in combination with motion amplitudes of the same order as the probing wavelength.}, archive = {J_PRL}, author = {Timo Sommer and Agnes Zinth and Aditya and Menno Poot}, doi = {10.1103/PhysRevLett.134.203604}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203604}, shortjournal = {Phys. Rev. Lett.}, title = {Spatial mapping of intrinsic and readout nonlinearities in a strongly driven micromechanical membrane}, volume = {134}, year = {2025}, }
• (2025). Modular variable laser cooling for efficient entropy extraction. PRL, 134(20), 203603. (www)

  @article{ , abstract = {We propose and experimentally demonstrate a method for laser cooling an oscillator, using a two-level ancillary spin, based on sequences of spin-state-dependent displacements, followed by spin repumping. For a thermal state with mean occupation n ¯ ≫ 1 , the method attains a reduction to 0.632 of the initial thermal oscillator occupation for two repumps of the spin state. This is within a factor of 2.53 of the optimum that is expected due to the reduction of the oscillator entropy by 2ln(2). We show that the method, which is based on encoding the value of the modular variable of the oscillator into the spin, has a simple semiclassical description in terms of a Bayesian update. We demonstrate the method experimentally using the internal and motional states of a single trapped ion.}, archive = {J_PRL}, author = {B. de Neeve and T.-L. Nguyen and A. Ferk and T. Behrle and F. Lancellotti and M. Simoni and S. Welte and J. P. Home}, doi = {10.1103/PhysRevLett.134.203603}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203603}, shortjournal = {Phys. Rev. Lett.}, title = {Modular variable laser cooling for efficient entropy extraction}, volume = {134}, year = {2025}, }
• (2025). Coherent control of photon correlations in trapped ion crystals. PRL, 134(20), 203602. (www)

  @article{ , abstract = {While the spontaneous emission from independent emitters provides spatially uncorrelated photons—a typical manifestation of quantum randomness, the interference of the coherent scattering leads to a well-defined intensity pattern—a feature described by linear optics. We here demonstrate experimentally how the interplay between the two mechanisms in large systems of quantum emitters leads to spatial variations of photon correlations. The implementation with trapped ion crystals in free space allows us to observe the anticorrelation between photon rates and variance of the photon number distributions in chains of up to 18 ions. For smaller crystals of four ions, the transition from antibunching to bunching and super-Poissonian statistics of the scattered light is reported. For higher numbers of scatterers, the photon statistics still display a strong deviation from the fully incoherent scattering case. Our results illustrate how the interference of coherent scattering, combined with spontaneous emission, provides a control mechanism for the light statistics.}, archive = {J_PRL}, author = {K. Singh and A. Cidrim and A. Kovalenko and T. M. Pham and O. Číp and L. Slodička and R. Bachelard}, doi = {10.1103/PhysRevLett.134.203602}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203602}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent control of photon correlations in trapped ion crystals}, volume = {134}, year = {2025}, }
• (2025). Conservation of angular momentum on a single-photon level. PRL, 134(20), 203601. (www)

  @article{ , abstract = {Identifying conservation laws is central to every subfield of physics, as they illuminate the underlying symmetries and fundamental principles. A prime example can be found in quantum optics: the conservation of orbital angular momentum (OAM) during spontaneous parametric down-conversion (SPDC) enables the generation of a photon pair with entangled OAM. In this Letter, we report on the observation of OAM conservation in SPDC pumped on the single-photon level by a preceding SPDC process. We implement this cascaded down-conversion scheme in free space, without waveguide confinement, and thereby set the stage for experiments on the direct generation of multiphoton high-dimensional entanglement using all degrees of freedom of light.}, archive = {J_PRL}, author = {L. Kopf and R. Barros and S. Prabhakar and E. Giese and R. Fickler}, doi = {10.1103/PhysRevLett.134.203601}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203601}, shortjournal = {Phys. Rev. Lett.}, title = {Conservation of angular momentum on a single-photon level}, volume = {134}, year = {2025}, }
• (2025). Quantum-state controlled formation of cosmically relevant metallic molecular ions. PRL, 134(20), 203401. (www)

  @article{ , abstract = {Metal-containing molecular ions are fundamentally important in both terrestrial and interstellar chemistry, yet their formation mechanisms have been largely unexplored experimentally. To address this lack of fundamental understanding of how these ions are created in space, we conducted an experimental study of a quantum-state-controlled reaction between Ca + and C 2 H 2 to investigate a potential unifying mechanism for the formation of metallic molecules. By tuning the quantum-state populations of laser-cooled Ca + , we demonstrate precise control over reactivity. Our results reveal a single ionic product, CaCCH + , providing valuable insights into the mechanisms underlying the formation of metal-containing ions in space.}, archive = {J_PRL}, author = {G. S. Kocheril and C. Zagorec-Marks and H. J. Lewandowski}, doi = {10.1103/PhysRevLett.134.203401}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-state controlled formation of cosmically relevant metallic molecular ions}, volume = {134}, year = {2025}, }
• (2025). Phase-resolved attoclock. PRL, 134(20), 203201. (www)

  @article{ , abstract = {How long an electron spends under the barrier during strong field tunneling ionization is still a controversial issue in attosecond science. We develop a new attoclock technique to address this problem. It exploits the carrier-envelope-phase dependence of angular streaking to extrapolate from elliptically polarized light measurements, for the first time, the deflection angles for circularly polarized light. Thus, we can avoid the ambiguity inherent to the modeling of the conventional elliptical attoclock. Our results show that the deflection angles are solely sensitive to the ionization potentials of targets and tunneling delay is a minor effect.}, archive = {J_PRL}, author = {Emmanuel Orunesajo and Sulaiman Abubakar and Blessed Oguh and Yasashri Ranathunga and Jonathan Dubois and Leonardo Rico and Richard Taïeb and Suk Kyoung Lee and Wen Li}, doi = {10.1103/PhysRevLett.134.203201}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {203201}, shortjournal = {Phys. Rev. Lett.}, title = {Phase-resolved attoclock}, volume = {134}, year = {2025}, }
• (2025). O16 electroweak response functions from first principles. PRL, 134(20), 202501. (www)

  @article{ , abstract = {We present calculations of various electroweak response functions for the nucleus obtained using coupled-cluster theory in conjunction with the Lorentz integral transform method. We employ nuclear forces derived at next-to-leading order and next-to-next-to-leading order in chiral effective field theory and perform a Bayesian analysis to assess uncertainties. Our results are in good agreement with available electron-scattering data at . Additionally, we provide several predictions for the weak response functions in the quasielastic peak region at and , which are critical for long-baseline neutrino experiments.}, archive = {J_PRL}, author = {Bijaya Acharya and Joanna E. Sobczyk and Sonia Bacca and Gaute Hagen and Weiguang Jiang}, doi = {10.1103/PhysRevLett.134.202501}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {202501}, shortjournal = {Phys. Rev. Lett.}, title = {O16 electroweak response functions from first principles}, volume = {134}, year = {2025}, }
• (2025). QCD equation of state with nf=3 flavors up to the electroweak scale. PRL, 134(20), 201904. (www)

  @article{ , abstract = {The equation of state of quantum chromodynamics with flavors is determined nonperturbatively in the range of temperatures between 3 and 165 GeV with a precision of about 0.5%–1.0%. The calculation is carried out by numerical simulations of lattice gauge theory discretized à la Wilson with shifted boundary conditions in the compact direction. At each given temperature the entropy density is computed at several lattice spacings in order to extrapolate the results to the continuum limit. Taken at face value, data point straight to the Stefan-Boltzmann value by following a linear behavior in the strong coupling constant squared. They are also compatible with the known perturbative formula supplemented by higher order terms in the coupling constant, a parametrization which describes well our data together with those present in the literature down to 500 MeV.}, archive = {J_PRL}, author = {Matteo Bresciani and Mattia Dalla Brida and Leonardo Giusti and Michele Pepe}, doi = {10.1103/PhysRevLett.134.201904}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201904}, shortjournal = {Phys. Rev. Lett.}, title = {QCD equation of state with nf=3 flavors up to the electroweak scale}, volume = {134}, year = {2025}, }
• (2025). First measurement of near-threshold and subthreshold j/ψ photoproduction off nuclei. PRL, 134(20), 201903. (www)

  @article{ , abstract = {We report on the first measurement of 𝐽 / 𝜓 photoproduction from nuclei in the photon energy range of 7 to 10.8 GeV, extending above and below the photoproduction threshold in the free proton of ∼ 8 . 2 G e V . The experiment used a tagged photon beam incident on deuterium, helium, and carbon, and the GlueX detector at Jefferson Lab to measure the semi-inclusive 𝐴 ⁡ ( 𝛾 , 𝑒 + ⁢ 𝑒 − ⁢ 𝑝 ) reaction with a dilepton invariant mass 𝑀 ⁡ ( 𝑒 + ⁢ 𝑒 − ) ∼ 𝑚 𝐽 / 𝜓 = 3 . 1 G e V . The incoherent 𝐽 / 𝜓 photoproduction cross sections in the measured nuclei are extracted as a function of the incident photon energy, momentum transfer, and proton-reconstructed missing light-cone momentum fraction. Comparisons with theoretical predictions assuming a dipole form factor allow for extracting a gluonic radius for bound protons of √ ⟨ 𝑟 2 ⟩ = 0 . 8 5 ± 0 . 1 4 f m . The data also suggest an excess of the measured cross section for subthreshold production and for interactions with high missing light-cone momentum fraction protons. The measured enhancement can be explained by modified gluon structure for high-virtuality bound protons.}, archive = {J_PRL}, author = {J. R. Pybus and L. Ehinger and T. Kolar and B. Devkota and P. Sharp and B. Yu and M. M. Dalton and D. Dutta and H. Gao and O. Hen and E. Piasetzky and S. N. Santiesteban and A. Schmidt and A. Somov and H. Szumila-Vance and S. Adhikari and A. Asaturyan and A. Austregesilo and C. Ayerbe Gayoso and J. Barlow and V. V. Berdnikov and H. D. Bhatt and D. Bhetuwal and T. Black and W. J. Briscoe and G. Chung and P. L. Cole and A. Deur and R. Dotel and H. Egiyan and P. Eugenio and C. Fanelli and L. Gan and A. Gasparian and J. Guo and K. Hernandez and D. W. Higinbotham and P. Hurck and I. Jaegle and R. T. Jones and V. Kakoyan and A. Karki and H. Li and W. B. Li and G. R. Linera and V. Lyubovitskij and H. Marukyan and M. D. McCaughan and M. McCracken and K. Mizutani and D. Nguyen and S. Oresic and A. I. Ostrovidov and Z. Papandreou and C. Paudel and K. Peters and J. Ritman and A. Schick and J. Schwiening and A. Smith and S. Somov and I. Strakovsky and K. Suresh and V. V. Tarasov and S. Taylor and T. Xiao and Z. Zhang and X. Zhou}, doi = {10.1103/PhysRevLett.134.201903}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201903}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of near-threshold and subthreshold j/ψ photoproduction off nuclei}, volume = {134}, year = {2025}, }
• (2025). Observation of the W-annihilation process ds+→ωρ+ and measurement of ds+→ϕρ+ in ds+→π+π+π−π0π0 decays. PRL, 134(20), 201902. (www)

  @article{ , abstract = {We present the first amplitude analysis and branching fraction measurement of the decay , using collision data collected with the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV corresponding to an integrated luminosity of , and report the first observation of the pure -annihilation decay with a branching fraction of . In comparison to the low significance of the wave in the decay , the dominance of the wave over the and waves, with a fraction of observed in the decay , provides crucial information for the “polarization puzzle,” as well as for the understanding of charm meson decays. The branching fraction of is measured to be . Moreover, the branching fraction of is measured to be , and the is determined to be ( ), which is consistent with the previous measurement based on charm meson decays, but deviates from the results from annihilation and scattering experiments by more than .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and W. N. Lan and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and M. Q. Ruan and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and Bo Wang and C. Wang and D. Y. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and X. Wu and X. H. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. X. Yang and Y. Z. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and C. Z. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.201902}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201902}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of the W-annihilation process ds+→ωρ+ and measurement of ds+→ϕρ+ in ds+→π+π+π−π0π0 decays}, volume = {134}, year = {2025}, }
• (2025). Long-distance window of the hadronic vacuum polarization for the muon g−2. PRL, 134(20), 201901. (www)

  @article{ , abstract = {We provide the first ab initio calculation of the Euclidean long-distance window of the isospin-symmetric light-quark connected contribution to the hadronic vacuum polarization for the muon and find . We also provide the currently most precise calculation of the total isospin-symmetric light-quark connected contribution, in the BMW20 world, which is more than larger compared to the data-driven estimates of Boito et al. [ Phys. Rev. D 107 , 074001 (2023) ] and larger compared to the lattice QCD result of BMW20.}, archive = {J_PRL}, author = {RBC and UKQCD Collaborations and T. Blum and P. A. Boyle and M. Bruno and B. Chakraborty and F. Erben and V. Gülpers and A. Hackl and N. Hermansson-Truedsson and R. C. Hill and T. Izubuchi and L. Jin and C. Jung and C. Lehner and J. McKeon and A. S. Meyer and M. Tomii and J. T. Tsang and X.-Y. Tuo}, doi = {10.1103/PhysRevLett.134.201901}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201901}, shortjournal = {Phys. Rev. Lett.}, title = {Long-distance window of the hadronic vacuum polarization for the muon g−2}, volume = {134}, year = {2025}, }
• (2025). Comprehensive measurement of the reactor antineutrino spectrum and flux at daya bay. PRL, 134(20), 201802. (www)

  @article{ , abstract = {This Letter reports the precise measurement of the reactor antineutrino spectrum and flux based on the full dataset of 4.7 × 10 6 inverse-beta-decay candidates collected at Daya Bay near detectors. Expressed in terms of the inverse-beta-decay yield per fission, the antineutrino spectra from all reactor fissile isotopes and the specific U 235 and Pu 239 isotopes are measured with 1.3%, 3%, and 8% uncertainties, respectively, near the 3 MeV spectrum peak in reconstructed energy, reaching the best precision in the world. The total antineutrino flux and isotopic U 235 and Pu 239 fluxes are precisely measured to be 5.84 ± 0.07 , 6.16 ± 0.12 , and 4.16 ± 0.21 in units of 10 − 43 cm 2 / fission . These measurements are compared with the Huber-Mueller model, the reevaluated conversion model based on the Kurchatov Institute measurement, and the latest summation model (SM2023). The Daya Bay flux shows good consistency with the Kurchatov Institute and SM2023 models but disagrees with the Huber-Mueller model. The Daya Bay spectrum, however, disagrees with all model predictions.}, archive = {J_PRL}, author = {Daya Bay Collaboration and F. P. An and W. D. Bai and A. B. Balantekin and M. Bishai and S. Blyth and G. F. Cao and J. Cao and J. F. Chang and Y. Chang and H. S. Chen and H. Y. Chen and S. M. Chen and Y. Chen and Y. X. Chen and Z. Y. Chen and J. Cheng and Y.-C. Cheng and Z. K. Cheng and J. J. Cherwinka and M. C. Chu and J. P. Cummings and O. Dalager and F. S. Deng and X. Y. Ding and Y. Y. Ding and M. V. Diwan and T. Dohnal and D. Dolzhikov and J. Dove and K. V. Dugas and H. Y. Duyang and D. A. Dwyer and J. P. Gallo and M. Gonchar and G. H. Gong and H. Gong and W. Q. Gu and J. Y. Guo and L. Guo and X. H. Guo and Y. H. Guo and Z. Guo and R. W. Hackenburg and Y. Han and S. Hans and M. He and K. M. Heeger and Y. K. Heng and Y. K. Hor and Y. B. Hsiung and B. Z. Hu and J. R. Hu and T. Hu and Z. J. Hu and H. X. Huang and J. H. Huang and X. T. Huang and Y. B. Huang and P. Huber and D. E. Jaffe and K. L. Jen and X. L. Ji and X. P. Ji and R. A. Johnson and D. Jones and L. Kang and S. H. Kettell and S. Kohn and M. Kramer and T. J. Langford and J. Lee and J. H. C. Lee and R. T. Lei and R. Leitner and J. K. C. Leung and F. Li and H. L. Li and J. J. Li and Q. J. Li and R. H. Li and S. Li and S. C. Li and W. D. Li and X. N. Li and X. Q. Li and Y. F. Li and Z. B. Li and H. Liang and C. J. Lin and G. L. Lin and S. Lin and J. J. Ling and J. M. Link and L. Littenberg and B. R. Littlejohn and J. C. Liu and J. L. Liu and J. X. Liu and C. Lu and H. Q. Lu and K. B. Luk and B. Z. Ma and X. B. Ma and X. Y. Ma and Y. Q. Ma and R. C. Mandujano and C. Marshall and K. T. McDonald and R. D. McKeown and Y. Meng and J. Napolitano and D. Naumov and E. Naumova and T. M. T. Nguyen and J. P. Ochoa-Ricoux and A. Olshevskiy and J. Park and S. Patton and J. C. Peng and C. S. J. Pun and F. Z. Qi and M. Qi and X. Qian and N. Raper and J. Ren and C. Morales Reveco and R. Rosero and B. Roskovec and X. C. Ruan and B. Russell and H. Steiner and J. L. Sun and T. Tmej and W.-H. Tse and C. E. Tull and Y. C. Tung and B. Viren and V. Vorobel and C. H. Wang and J. Wang and M. Wang and N. Y. Wang and R. G. Wang and W. Wang and X. Wang and Y. F. Wang and Z. Wang and Z. M. Wang and H. Y. Wei and L. H. Wei and W. Wei and L. J. Wen and K. Whisnant and C. G. White and H. L. H. Wong and E. Worcester and D. R. Wu and Q. Wu and W. J. Wu and D. M. Xia and Z. Q. Xie and Z. Z. Xing and H. K. Xu and J. L. Xu and T. Xu and T. Xue and C. G. Yang and L. Yang and Y. Z. Yang and H. F. Yao and M. Ye and M. Yeh and B. L. Young and H. Z. Yu and Z. Y. Yu and B. B. Yue and V. Zavadskyi and S. Zeng and Y. Zeng and L. Zhan and C. Zhang and F. Y. Zhang and H. H. Zhang and J. L. Zhang and J. W. Zhang and Q. M. Zhang and S. Q. Zhang and X. T. Zhang and Y. M. Zhang and Y. X. Zhang and Y. Y. Zhang and Z. J. Zhang and Z. P. Zhang and Z. Y. Zhang and J. Zhao and R. Z. Zhao and L. Zhou and H. L. Zhuang and J. H. Zou}, doi = {10.1103/PhysRevLett.134.201802}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201802}, shortjournal = {Phys. Rev. Lett.}, title = {Comprehensive measurement of the reactor antineutrino spectrum and flux at daya bay}, volume = {134}, year = {2025}, }
• (2025). Improved evaluation of the electroweak contribution to muon g−2. PRL, 134(20), 201801. (www)

  @article{ , abstract = {A precise evaluation of the electroweak contribution to the anomalous magnetic moment of the muon requires control over all aspects of the standard model, ranging from Higgs physics, over multiloop computations for bosonic and (heavy-)fermion diagrams, to nonperturbative effects in the presence of light quarks. Currently, the dominant uncertainties arise from such hadronic effects in the vector–vector–axial-vector three-point function, an improved understanding of which has recently emerged in the context of hadronic light-by-light scattering. Profiting from these developments as well as new perturbative and nonperturbative input for the charm contribution, we obtain a μ EW = 154.4 ( 4 ) × 10 − 11 .}, archive = {J_PRL}, author = {Martin Hoferichter and Jan Lüdtke and Luca Naterop and Massimiliano Procura and Peter Stoffer}, doi = {10.1103/PhysRevLett.134.201801}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201801}, shortjournal = {Phys. Rev. Lett.}, title = {Improved evaluation of the electroweak contribution to muon g−2}, volume = {134}, year = {2025}, }
• (2025). One-dimensional ising model with 1/r1.99 interaction. PRL, 134(20), 201602. (www)

  @article{ , abstract = {We study the 1D Ising model with long-range interactions decaying as 1 / r 1 + s . The critical model corresponds to a family of 1D conformal field theories whose data depend nontrivially on s in the range 1 / 2 ≤ s ≤ 1 . The model is known to be described by a generalized free field with quartic interaction, which is weakly coupled near s = 1 / 2 but strongly coupled near the short-range crossover at s = 1 . We propose a dual description that becomes weakly coupled at s = 1 . At s = 1 , our model becomes an exactly solvable conformal boundary condition for the 2D free scalar. We perform a number of consistency checks of our proposal and calculate the perturbative conformal field theory data around s = 1 analytically using both (1) our proposed field theory and (2) the analytic conformal bootstrap. Our results show complete agreement between the two methods.}, archive = {J_PRL}, author = {Dario Benedetti and Edoardo Lauria and Dalimil Mazáč and Philine van Vliet}, doi = {10.1103/PhysRevLett.134.201602}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201602}, shortjournal = {Phys. Rev. Lett.}, title = {One-dimensional ising model with 1/r1.99 interaction}, volume = {134}, year = {2025}, }
• (2025). Type II superstring amplitude at one-loop and transcendentality. PRL, 134(20), 201601. (www)

  @article{ , abstract = {We calculate the four-graviton scattering amplitude in Type II superstring theory at one loop up to seventh order in the low-energy expansion through the recently developed iterated integral formalism of Modular Graph Functions (MGFs). The machinery of the novel method allows us to propose a general form of the amplitude, which suggests that the expansion is expressible in terms of single-valued multiple zeta values and logarithmic derivatives of the Riemann zeta function at positive and negative odd integers. Furthermore, we comment on the transcendental behavior of the amplitude.}, archive = {J_PRL}, author = {Emiel Claasen and Mehregan Doroudiani}, doi = {10.1103/PhysRevLett.134.201601}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201601}, shortjournal = {Phys. Rev. Lett.}, title = {Type II superstring amplitude at one-loop and transcendentality}, volume = {134}, year = {2025}, }
• (2025). Self-excited gravitational instantons. PRL, 134(20), 201501. (www)

  @article{ , abstract = {We present a novel approach to constructing gravitational instantons based on the observation that the gravitational action of general relativity in its teleparallel formulation can be expressed as a product of the torsion and excitation forms. We introduce a new class of solutions where these two forms are equal, which we term the self-excited instantons, and advocate for their use over the self-dual instantons of Eguchi and Hanson. These new self-excited instantons exhibit striking similarities to BPST instantons in Yang-Mills theory, as their action reduces to a topological Nieh-Yan term, which allows us to identify the axial torsion as a topological current and show that the gravitational action is given by a topological charge.}, archive = {J_PRL}, author = {Martin Krššák}, doi = {10.1103/PhysRevLett.134.201501}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201501}, shortjournal = {Phys. Rev. Lett.}, title = {Self-excited gravitational instantons}, volume = {134}, year = {2025}, }
• (2025). New constraints on axionlike particles with the NEON detector at a nuclear reactor. PRL, 134(20), 201002. (www)

  @article{ , abstract = {We report new constraints on axionlike particles (ALPs) using data from the NEON experiment, which features 16.7 kg of NaI(Tl) target located 23.7 m from a 2.8 GW thermal power nuclear reactor. Analyzing a total exposure of 3063 kg · day , with 1596 kg · day during reactor-on and 1467 kg · day during reactor-off periods, we compared energy spectra to search for ALP-induced signals. No significant signal was observed, enabling us to set exclusion limits at the 95% confidence level. These limits probe previously unexplored regions of the ALP parameter space, particularly for axion masses ( m a ) near 1 MeV / c 2 . For ALP-photon coupling ( g a γ ), limits reach as low as 6.24 × 10 − 6 GeV − 1 at m a = 3.0 MeV / c 2 , while for ALP-electron coupling ( g a e ), limits reach 4.95 × 10 − 8 at m a = 1.02 MeV / c 2 . This Letter demonstrates the potential for future reactor experiments to probe unexplored ALP parameter space.}, archive = {J_PRL}, author = {NEON Collaboration and Byung Ju Park and Jae Jin Choi and Eunju Jeon and Jinyu Kim and Kyungwon Kim and Sung Hyun Kim and Sun Kee Kim and Yeongduk Kim and Young Ju Ko and Byoung-Cheol Koh and Chang Hyon Ha and Seo Hyun Lee and In Soo Lee and Hyunseok Lee and Hyun Su Lee and Jaison Lee and Yoomin Oh and Doojin Kim and Gordan Krnjaic and Jacopo Nava}, doi = {10.1103/PhysRevLett.134.201002}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201002}, shortjournal = {Phys. Rev. Lett.}, title = {New constraints on axionlike particles with the NEON detector at a nuclear reactor}, volume = {134}, year = {2025}, }
• (2025). Properties of cosmic lithium isotopes measured by the alpha magnetic spectrometer. PRL, 134(20), 201001. (www)

  @article{ , abstract = {We present the first measurement of cosmic-ray fluxes of Li 6 and Li 7 isotopes in the rigidity range from 1.9 to 25 GV. The measurements are based on 9.7 × 10 5 Li 6 and 1.04 × 10 6 Li 7 nuclei collected by the Alpha Magnetic Spectrometer on the International Space Station from May 2011 to October 2023. We observe that over the entire rigidity range the Li 6 and Li 7 fluxes exhibit nearly identical time variations and, above ∼ 4 GV , the time variations of Li 6 , Li 7 , He, Be, B, C, N, and O fluxes are identical. Above ∼ 7 GV , we find an identical rigidity dependence of the Li 6 and Li 7 fluxes. This shows that they are both produced by collisions of heavier cosmic-ray nuclei with the interstellar medium and, in particular, excludes the existence of a sizable primary component in the Li 7 flux.}, archive = {J_PRL}, author = {AMS Collaboration and M. Aguilar and G. Ambrosi and H. Anderson and L. Arruda and N. Attig and C. Bagwell and F. Barao and M. Barbanera and L. Barrin and A. Bartoloni and R. Battiston and A. Bayyari and N. Belyaev and B. Bertucci and V. Bindi and K. Bollweg and J. Bolster and M. Borchiellini and B. Borgia and M. J. Boschini and M. Bourquin and C. Brugnoni and J. Burger and W. J. Burger and N. Burzillà and X. D. Cai and M. Capell and J. Casaus and G. Castellini and F. Cervelli and Y. H. Chang and G. M. Chen and G. R. Chen and H. Chen and H. S. Chen and Y. Chen and L. Cheng and H. Y. Chou and S. Chouridou and V. Choutko and C. H. Chung and C. Clark and G. Coignet and C. Consolandi and A. Contin and C. Corti and Z. Cui and K. Dadzie and F. D’Angelo and A. Dass and C. Delgado and S. Della Torre and M. B. Demirköz and L. Derome and S. Di Falco and V. Di Felice and C. Díaz and F. Dimiccoli and P. von Doetinchem and F. Dong and M. Duranti and A. Egorov and A. Eline and F. Faldi and D. Fehr and J. Feng and E. Fiandrini and P. Fisher and V. Formato and R. J. García-López and C. Gargiulo and H. Gast and M. Gervasi and F. Giovacchini and D. M. Gómez-Coral and J. Gong and D. Grandi and M. Graziani and S. Haino and K. C. Han and Z. H. He and B. Heber and F. Hernández-Nicolás and T. H. Hsieh and J. Y. Hu and B. W. Huang and M. Ionica and M. Incagli and Yi Jia and H. Jinchi and G. Karagöz and Th. Kirn and A. P. Klipfel and O. Kounina and A. Kounine and V. Koutsenko and D. Krasnopevtsev and A. Kuhlman and A. Kulemzin and G. La Vacca and E. Laudi and G. Laurenti and G. LaVecchia and I. Lazzizzera and H. T. Lee and S. C. Lee and H. L. Li and J. H. Li and J. Q. Li and M. Li and Q. Li and Q. Y. Li and S. L. Li and Z. H. Li and M. J. Liang and P. Liao and C. H. Lin and T. Lippert and J. H. Liu and P. C. Liu and Z. Liu and S. Q. Lu and J. Z. Luo and Q. Luo and S. D. Luo and Xi Luo and C. Mañá and J. Marín and J. Marquardt and G. Martínez and N. Masi and D. Maurin and T. Medvedeva and A. Menchaca-Rocha and Q. Meng and V. V. Mikhailov and M. Molero and P. Mott and L. Mussolin and Y. Najafi Jozani and R. Nicolaidis and N. Nikonov and F. Nozzoli and J. Ocampo-Peleteiro and A. Oliva and M. Orcinha and F. Palmonari and M. Paniccia and A. Pashnin and M. Pauluzzi and D. Pelosi and S. Pensotti and P. Pietzcker and V. Plyaskin and S. Poluianov and D. Pridöhl and Z. Y. Qu and L. Quadrani and P. G. Rancoita and D. Rapin and A. Reina Conde and E. Robyn and I. Rodríguez-García and L. Romaneehsen and F. Rossi and A. Rozhkov and D. Rozza and R. Sagdeev and S. Schael and A. Schultz von Dratzig and G. Schwering and E. S. Seo and B. S. Shan and A. Shukla and T. Siedenburg and A. Siemko and G. Silvestre and J. W. Song and X. J. Song and R. Sonnabend and L. Strigari and T. Su and Q. Sun and Z. T. Sun and L. Tabarroni and M. Tacconi and Z. C. Tang and J. Tian and Y. Tian and Samuel C. C. Ting and S. M. Ting and N. Tomassetti and J. Torsti and B. Türk and A. Ubaldi and T. Urban and I. Usoskin and V. Vagelli and R. Vainio and P. Väisänen and M. Valencia-Otero and E. Valente and E. Valtonen and M. Vázquez Acosta and M. Vecchi and M. Velasco and C. X. Wang and J. C. Wang and L. Wang and L. Q. Wang and N. H. Wang and Q. L. Wang and S. Wang and X. Wang and Z. M. Wang and J. Wei and Z. L. Weng and H. Wu and Y. Wu and Z. B. Wu and J. N. Xiao and R. Q. Xiong and X. Z. Xiong and W. Xu and Q. Yan and H. T. Yang and Y. Yang and H. Yi and Y. H. You and Y. M. Yu and Z. Q. Yu and C. Zhang and F. Z. Zhang and J. Zhang and J. H. Zhang and Z. Zhang and P. W. Zhao and C. Zheng and Z. M. Zheng and H. L. Zhuang and V. Zhukov and A. Zichichi and M. Zuberi and P. Zuccon}, doi = {10.1103/PhysRevLett.134.201001}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {201001}, shortjournal = {Phys. Rev. Lett.}, title = {Properties of cosmic lithium isotopes measured by the alpha magnetic spectrometer}, volume = {134}, year = {2025}, }
• (2025). Linear-optical fusion boosted by high-dimensional entanglement. PRL, 134(20), 200801. (www)

  @article{ , abstract = {We propose a quantum measurement that probabilistically projects a pair of qudits of dimension d onto a Bell state in a two-qubit subspace. It can be implemented using linear-optical circuits with the success probabilities of 1 − d − 1 without ancilla photons and 1 − d − ( k + 1 ) with 2 ( 2 k − 1 ) ancilla photons. It allows us to entangle two independently prepared high-dimensional entangled states two dimensionally with higher success probabilities than ones of linear-optical fusion gates on qubits. As an application, we propose a fast quantum repeater protocol with three-qudit GHZ states and quantum memories.}, archive = {J_PRL}, author = {Tomohiro Yamazaki and Koji Azuma}, doi = {10.1103/PhysRevLett.134.200801}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200801}, shortjournal = {Phys. Rev. Lett.}, title = {Linear-optical fusion boosted by high-dimensional entanglement}, volume = {134}, year = {2025}, }
• (2025). Experimental verifiable multiclient blind quantum computing on a qline architecture. PRL, 134(20), 200603. (www)

  @article{ , abstract = {The exploitation of certification tools by end users represents a fundamental aspect of the development of quantum technologies as the hardware scales up beyond the regime of classical simulability. Certifying quantum networks becomes even more crucial when the privacy of their users is exposed to malicious quantum nodes or servers as in the case of multiclient distributed blind quantum computing, where several clients delegate a joint private computation to remote quantum servers, such as federated quantum machine learning. In such protocols, security must be provided not only by keeping data hidden but also by verifying that the server is correctly performing the requested computation while minimizing the hardware assumptions on the employed devices. Notably, standard verification techniques fail in scenarios where the clients receive quantum states from untrusted sources such as in a recently demonstrated linear quantum network performing multiclient blind quantum computation. However, recent theoretical results provide techniques to verify blind quantum computations even in the case of untrusted state preparation. Equipped with such theoretical tools, in this Letter we provide the first experimental implementation of a multiclient verifiable blind quantum computing protocol in a distributed architecture. Our results represent novel perspectives for the verification of multitenant distributed quantum computation in large-scale networks.}, archive = {J_PRL}, author = {Beatrice Polacchi and Dominik Leichtle and Gonzalo Carvacho and Giorgio Milani and Nicolò Spagnolo and Marc Kaplan and Elham Kashefi and Fabio Sciarrino}, doi = {10.1103/PhysRevLett.134.200603}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200603}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental verifiable multiclient blind quantum computing on a qline architecture}, volume = {134}, year = {2025}, }
• (2025). Optimality condition for the petz map. PRL, 134(20), 200602. (www)

  @article{ , abstract = {In quantum error correction, the Petz map serves as a perfect recovery map when the Knill-Laflamme conditions are satisfied. Notably, while perfect recovery is generally infeasible for most quantum channels of finite dimension, the Petz map remains a versatile tool with near-optimal performance in recovering quantum states. This work introduces and proves, for the first time, the necessary and sufficient conditions for the optimality of the Petz map in terms of entanglement fidelity. In some special cases, the violation of this condition can be easily characterized by a simple commutator that can be efficiently computed. We provide multiple examples that substantiate our new findings.}, archive = {J_PRL}, author = {Bikun Li and Zhaoyou Wang and Guo Zheng and Yat Wong and Liang Jiang}, doi = {10.1103/PhysRevLett.134.200602}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200602}, shortjournal = {Phys. Rev. Lett.}, title = {Optimality condition for the petz map}, volume = {134}, year = {2025}, }
• (2025). Optimally generating su(2N) using pauli strings. PRL, 134(20), 200601. (www)

  @article{ , abstract = {Any quantum computation consists of a sequence of unitary evolutions described by a finite set of Hamiltonians. When this set is taken to consist of only products of Pauli operators, we show that the minimal such set generating contains elements. We provide a number of examples of such generating sets and furthermore provide an algorithm for producing a sequence of rotations corresponding to any given Pauli rotation, which is shown to have optimal complexity. We also observe that certain sets generate at a faster rate than others, and we show how this rate can be optimized by tuning the fraction of anticommuting pairs of generators. Finally, we briefly comment on implications for measurement-based and trapped ion quantum computation as well as the construction of fault-tolerant gate sets.}, archive = {J_PRL}, author = {Isaac D. Smith and Maxime Cautrès and David T. Stephen and Hendrik Poulsen Nautrup}, doi = {10.1103/PhysRevLett.134.200601}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200601}, shortjournal = {Phys. Rev. Lett.}, title = {Optimally generating su(2N) using pauli strings}, volume = {134}, year = {2025}, }
• (2025). Run-and-tumble exact work statistics in a lazy quantum measurement engine: Stochastic information processing. PRL, 134(20), 200402. (www)

  @article{ , abstract = {We introduce a single-qubit quantum measurement engine fuelled by backaction energy input. To reduce energetic costs associated with information processing, the measurement outcomes are only used with a prescribed laziness probability in the feedback step. As a result, we show that the work extracted over consecutive cycles is a second-order Markov process, analogous to a run-and-tumble process with transient anomalous diffusion. We derive exact analytical expressions for the work finite-time moments and first-passage-time statistics. Furthermore, we find the optimal laziness probability maximizing the mean power extracted per cycle.}, archive = {J_PRL}, author = {Léa Bresque and Debraj Das and Édgar Roldán}, doi = {10.1103/PhysRevLett.134.200402}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200402}, shortjournal = {Phys. Rev. Lett.}, title = {Run-and-tumble exact work statistics in a lazy quantum measurement engine: Stochastic information processing}, volume = {134}, year = {2025}, }
• (2025). Quantum processes as thermodynamic resources: The role of non-markovianity. PRL, 134(20), 200401. (www)

  @article{ , abstract = {Quantum thermodynamics studies how quantum systems and operations may be exploited as sources of work to perform useful thermodynamic tasks. In real-world conditions, the evolution of open quantum systems typically displays memory effects, resulting in a non-Markovian dynamics. The associated information backflow has been observed to provide advantage in certain thermodynamic tasks. However, a general operational connection between non-Markovianity and thermodynamics in the quantum regime has remained elusive. Here, we analyze the role of non-Markovianity in the central task of extracting work via thermal operations from general multitime quantum processes, as described by process tensors. By defining a hierarchy of four classes of extraction protocols, expressed as quantum combs, we reveal three different physical mechanisms (work investment, multitime correlations, and system-environment correlations) through which non-Markovianity increases the work distillable from the process. The advantages arising from these mechanisms are linked precisely to a quantifier of the non-Markovianity of the process. These results show in very general terms how non-Markovianity of any given quantum process is a fundamental resource that unlocks an enhanced performance in thermodynamics.}, archive = {J_PRL}, author = {Guilherme Zambon and Gerardo Adesso}, doi = {10.1103/PhysRevLett.134.200401}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum processes as thermodynamic resources: The role of non-markovianity}, volume = {134}, year = {2025}, }
• (2025). Experimental implementation of dimension-dependent contextuality inequality. PRL, 134(20), 200202. (www)

  @article{ , abstract = {We present a derivation and experimental implementation of a dimension-dependent contextuality inequality to certify both the quantumness and dimensionality of a given system. Existing methods for certification of the dimension of a quantum system can be cheated by using larger classical systems, creating a potential loophole in these benchmarks, or can in practice only be evaluated assuming pure quantum states. Our approach uses contextuality inequalities that cannot be violated by classical systems thus closing the previous loopholes. We validate this framework experimentally with photons, observing violations of a CHSH-based contextuality inequality and surpassing the qutrit bound of the -based contextuality inequality. These show that contextuality can be used for noise-robust tests of the number of qubits.}, archive = {J_PRL}, author = {Emil Håkansson and Amelie Piveteau and Alban Seguinard and Sadiq Muhammad and Mohamed Bourennane and Otfried Gühne and Martin Plávala}, doi = {10.1103/PhysRevLett.134.200202}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200202}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental implementation of dimension-dependent contextuality inequality}, volume = {134}, year = {2025}, }
• (2025). All incompatible measurements on qubits lead to multiparticle bell nonlocality. PRL, 134(20), 200201. (www)

  @article{ , abstract = {Bell nonlocality is a fundamental phenomenon of quantum physics as well as an essential resource for various tasks in quantum information processing. It is known that for the observation of nonlocality the measurements on a quantum system have to be incompatible, but the question of which incompatible measurements are useful, remained open. Here we prove that any set of incompatible measurements on qubits leads to a violation of a suitable Bell inequality in a multiparticle scenario, where all parties perform the same set of measurements. Since there exists incompatible measurements on qubits which do not lead to Bell nonlocality for two particles, our results demonstrate a fundamental difference between two-particle and multiparticle nonlocality, pointing at the superactivation of measurement incompatibility as a resource. In addition, our results imply that measurement incompatibility for qubits can always be certified in a device-independent manner.}, archive = {J_PRL}, author = {Martin Plávala and Otfried Gühne and Marco Túlio Quintino}, doi = {10.1103/PhysRevLett.134.200201}, journal = {Physical Review Letters}, month = {5}, number = {20}, pages = {200201}, shortjournal = {Phys. Rev. Lett.}, title = {All incompatible measurements on qubits lead to multiparticle bell nonlocality}, volume = {134}, year = {2025}, }
• (2025). Erratum: Clustering of conditional mutual information for quantum gibbs states above a threshold temperature [Phys. rev. lett. 124, 220601 (2020)]. PRL, 134(19), 199901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 199901 (2025)}, archive = {J_PRL}, author = {Tomotaka Kuwahara and Kohtaro Kato and Fernando G. S. L. Brandão}, doi = {10.1103/PhysRevLett.134.199901}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {199901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Clustering of conditional mutual information for quantum gibbs states above a threshold temperature [Phys. rev. lett. 124, 220601 (2020)]}, volume = {134}, year = {2025}, }
• (2025). Mechanics of soft-body rolling motion without external torque. PRL, 134(19), 198401. (www)

  @article{ , abstract = {The Drosophila larva, a soft-body animal, can bend its body and roll efficiently to escape danger. However, contrary to common belief, this rolling motion is not driven by the imbalance of gravity and ground reaction forces. Through functional imaging and ablation experiments, we demonstrate that the sequential actuation of axial muscles within an appropriate range of angles is critical for generating rolling. We model the interplay between muscle contraction, hydrostatic skeleton deformation, and body-environment interactions, and systematically explain how sequential muscle actuation generates the rolling motion. Additionally, we construct a pneumatic soft robot to mimic the larval rolling strategy, successfully validating our model. This mechanics model of soft-body rolling motion not only advances the study of related neural circuits, but also holds potential for applications in soft robotics.}, archive = {J_PRL}, author = {Xudong Liang and Yimiao Ding and Zihao Yuan and Yuxuan Han and Yutang Zhou and Junqi Jiang and Zongling Xie and Peng Fei and Yixuan Sun and Pan Jia and Guoying Gu and Zheng Zhong and Feifei Chen and Guangwei Si and Zhefeng Gong}, doi = {10.1103/PhysRevLett.134.198401}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {198401}, shortjournal = {Phys. Rev. Lett.}, title = {Mechanics of soft-body rolling motion without external torque}, volume = {134}, year = {2025}, }
• (2025). Entropic trapping of hard spheres in spherical confinement. PRL, 134(19), 198201. (www)

  @article{ , abstract = {Monodisperse spherical colloidal particles confined within emulsion droplets can crystallize into icosahedral clusters. Experimentally, it was observed that a few large colloidal particles added as defects preferentially migrate to the vertices of the icosahedral clusters. To understand this structure formation phenomenon, we simulate the confined self-assembly of hard spheres in the presence of a small number of larger particles. The results demonstrate that large spheres are significantly influenced by concentric shells of small spheres near the crystallization transition. Entropic forces drive the large spheres to the cluster surface, where they settle into free energy minima at the icosahedron vertices. Notably, the addition of twelve large spheres results in the formation of a perfect icosahedral frame. Free energy calculations via umbrella sampling are used to quantify this process and show that both the migration to the cluster surface and the trapping at the vertices with trapping strength of multiple results from free energy minimization. Moreover, our study reveals that the crystallization pathway and dynamics of large spheres are consistent across different systems, suggesting robustness of entropic trapping.}, archive = {J_PRL}, author = {Praveen K. Bommineni and Junwei Wang and Nicolas Vogel and Michael Engel}, doi = {10.1103/PhysRevLett.134.198201}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {198201}, shortjournal = {Phys. Rev. Lett.}, title = {Entropic trapping of hard spheres in spherical confinement}, volume = {134}, year = {2025}, }
• (2025). Mesoscopic theory for coupled stochastic oscillators. PRL, 134(19), 197201. (www)

  @article{ , abstract = {The celebrated Ott-Antonsen Ansatz for coupled oscillators provides a useful framework for working with deterministic systems in the thermodynamic limit, but it fails to capture many features of stochastic systems. Several solutions have been recently proposed to accurately describe the behavior of the order parameters in coupled oscillator systems. However, a fluctuating description of such order parameters has been still elusive. In this Letter, I construct for the first time a general mesoscopic description of finite-size populations of oscillators subject to white noise. The theory allows one to derive Langevin equations for the Kuramoto-Daido order parameters, opening the door to study features of synchronization phase transitions and finite-size effects, which were inaccessible before. The analysis of the fluctuations in the stochastic Kuramoto model uncovered highly accurate, closed analytical expressions for the average Kuramoto order parameter which outperforms previous approaches.}, archive = {J_PRL}, author = {Victor Buendía}, doi = {10.1103/PhysRevLett.134.197201}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {197201}, shortjournal = {Phys. Rev. Lett.}, title = {Mesoscopic theory for coupled stochastic oscillators}, volume = {134}, year = {2025}, }
• (2025). Persistence exponents of self-interacting random walks. PRL, 134(19), 197103. (www)

  @article{ , abstract = {The persistence exponent, which characterizes the long-time decay of the survival probability of stochastic processes in the presence of an absorbing target, plays a key role in quantifying the dynamics of fluctuating systems. Determining this exponent for non-Markovian processes is known to be a difficult task, and exact results remain scarce despite sustained efforts. In this Letter, we consider the fundamental class of self-interacting random walks (SIRWs), which display long-range memory effects that result from the interaction of the random walker at time t with the territory already visited at earlier times t ′ < t . We compute exactly the persistence exponent for all physically relevant SIRWs. As a byproduct, we also determine the splitting probability of these processes. Besides their intrinsic theoretical interest, these results provide a quantitative characterization of the exploration process of SIRWs, which are involved in fields as diverse as foraging theory, cell biology, and nonreversible Monte Carlo methods.}, archive = {J_PRL}, author = {J. Brémont and L. Régnier and R. Voituriez and O. Bénichou}, doi = {10.1103/PhysRevLett.134.197103}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {197103}, shortjournal = {Phys. Rev. Lett.}, title = {Persistence exponents of self-interacting random walks}, volume = {134}, year = {2025}, }
• (2025). Route of random process to ultraslow aging phenomena. PRL, 134(19), 197102. (www)

  @article{ , abstract = {Logarithmic aging phenomena are prevalent in various systems, including electronic materials and biological structures. This Letter utilizes a generalized continuous-time random walk framework to investigate the mechanisms behind the logarithmic aging phenomena. By incorporating non-Markovian processes with significant memory effects, we modify traditional diffusion models to exhibit logarithmic decay in both survival and returning probabilities. Importantly, we analyze the impact of aging on autocorrelation functions, illustrating how long-term memory behaviors affect the temporal evolution of physical observables. These results connect microscopic models to macroscopic manifestations in real-world systems, advancing the understanding of ultraslow dynamics in disordered systems.}, archive = {J_PRL}, author = {Chunyan Li and Haiwen Liu and X. C. Xie}, doi = {10.1103/PhysRevLett.134.197102}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {197102}, shortjournal = {Phys. Rev. Lett.}, title = {Route of random process to ultraslow aging phenomena}, volume = {134}, year = {2025}, }
• (2025). Multifractional brownian motion with telegraphic, stochastically varying exponent. PRL, 134(19), 197101. (www)

  @article{ , abstract = {The diversity of diffusive systems exhibiting long-range correlations characterized by a stochastically varying Hurst exponent calls for a generic multifractional model. We present a simple, analytically tractable model which fills the gap between mathematical formulations of multifractional Brownian motion and empirical studies. In our model, called telegraphic multifractional Brownian motion, the Hurst exponent is modeled by a smoothed telegraph process which results in a stationary beta distribution of exponents as observed in biological experiments. We also provide a methodology to identify our model in experimental data and present concrete examples from biology, climate, and finance to demonstrate the efficacy of our approach.}, archive = {J_PRL}, author = {Michał Balcerek and Samudrajit Thapa and Krzysztof Burnecki and Holger Kantz and Ralf Metzler and Agnieszka Wyłomańska and Aleksei Chechkin}, doi = {10.1103/PhysRevLett.134.197101}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {197101}, shortjournal = {Phys. Rev. Lett.}, title = {Multifractional brownian motion with telegraphic, stochastically varying exponent}, volume = {134}, year = {2025}, }
• (2025). Optical signatures of spin symmetries in unconventional magnets. PRL, 134(19), 196907. (www)

  @article{ , abstract = {The concept of spin symmetries has gained renewed interest as a valuable tool for classifying unconventional magnetic phases, including altermagnets and recently identified p -wave magnets. In this work, we show that in compounds with weak spin-orbit coupling, the dominant spin and charge photoresponse is determined by spin group rather than the conventional magnetic group symmetry. As a concrete realization we consider the nonlinear shift photocurrent in Mn 5 Si 3 , a material that features the two possible classes of unconventional p -wave magnetism in the form of two competing spin structures, a coplanar and noncoplanar one. While both are predicted to generate shift currents based on magnetic symmetry considerations, only the noncoplanar configuration survives the spin symmetry requirements. This is numerically confirmed by our ab initio calculations, providing a protocol to experimentally identify the spin configuration of this promising material in photogalvanic or transport measurements.}, archive = {J_PRL}, author = {Javier Sivianes and Flaviano José dos Santos and Julen Ibañez-Azpiroz}, doi = {10.1103/PhysRevLett.134.196907}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196907}, shortjournal = {Phys. Rev. Lett.}, title = {Optical signatures of spin symmetries in unconventional magnets}, volume = {134}, year = {2025}, }
• (2025). Magnetic order induced chiral phonons in a ferromagnetic weyl semimetal. PRL, 134(19), 196906. (www)

  @article{ , abstract = {Chiral phonons are vibrational modes in a crystal that possess a well-defined handedness or chirality, typically found in materials that lack inversion symmetry. Here, we report the discovery of chiral phonon modes in the kagome ferromagnetic Weyl semimetal Co 3 Sn 2 S 2 , a material that preserves inversion symmetry but breaks time-reversal symmetry. Using helicity-resolved magneto-Raman spectroscopy, we observe the spontaneous splitting of the doubly degenerate in-plane E g modes into two distinct chiral phonon modes of opposite helicity when the sample is zero-field cooled below the Curie temperature in the absence of an external magnetic field. As we sweep the out-of-plane magnetic field, this E g phonon splitting exhibits a well-defined hysteresis loop directly correlated with the material’s magnetization. The observed spontaneous splitting reaches up to 1.2 7 cm − 1 at low temperatures, progressively diminishes with increasing temperature, and completely vanishes near the Curie temperature. Our findings highlight the role of the magnetic order in inducing chiral phonons, paving the way for novel methods to manipulate chiral phonons through magnetization and vice versa. Additionally, our Letter introduces new possibilities for controlling chiral Weyl fermions using chiral phonons.}, archive = {J_PRL}, author = {Mengqian Che and Jinxuan Liang and Yunpeng Cui and Hao Li and Bingru Lu and Wenbo Sang and Xiang Li and Xuebin Dong and Le Zhao and Shuai Zhang and Tao Sun and Wanjun Jiang and Enke Liu and Feng Jin and Tiantian Zhang and Luyi Yang}, doi = {10.1103/PhysRevLett.134.196906}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196906}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic order induced chiral phonons in a ferromagnetic weyl semimetal}, volume = {134}, year = {2025}, }
• (2025). Inherent circular dichroism of phonons in magnetic weyl semimetal Co3Sn2S2. PRL, 134(19), 196905. (www)

  @article{ , abstract = {We investigated the infrared-active phonons in ferromagnetic Weyl semimetal Co 3 Sn 2 S 2 using optical spectroscopy. Below the Curie temperature ( T C ≈ 175 K ), we observed asymmetric Fano line shapes of phonons peaks in the optical conductivities, reflecting the presence of electron-phonon coupling. Additionally, the detected phonon signals by the polar Kerr rotation and the ellipticity spectroscopy indicate the circular dichroism (CD) of phonons. We attribute the CD of phonons to their distinct couplings with charge excitations on the tilted Weyl nodal rings in two circularly polarized channels. Our findings provide experimental evidence that, without external fields, phonons can also become circularly polarized by coupling with the electronic topology. Since the magnetic exchange splitting gradually shifts the topological bands in Co 3 Sn 2 S 2 , the CD of phonons exhibits significant temperature dependence, hinting at a promising approach for manipulation.}, archive = {J_PRL}, author = {R. Yang and Y.-Y. Zhu and M. Steigleder and Y.-C. Liu and C.-C. Liu and X.-G. Qiu and Tiantian Zhang and M. Dressel}, doi = {10.1103/PhysRevLett.134.196905}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196905}, shortjournal = {Phys. Rev. Lett.}, title = {Inherent circular dichroism of phonons in magnetic weyl semimetal Co3Sn2S2}, volume = {134}, year = {2025}, }
• (2025). Nonreciprocal control of the speed of light using cavity magnonics. PRL, 134(19), 196904. (www)

  @article{ , abstract = {We demonstrate nonreciprocal control of the speed of light by sending a microwave pulse through a cavity magnonics device. In contrast to reciprocal group velocity controlled by conventional electromagnetically induced transparency (EIT) effects, incorporating a dissipative magnon-photon coupling establishes a nonreciprocal EIT effect, allowing slow and fast light propagation in opposite directions at the same frequency with comparable amplitude. Remarkably, reversing the magnetic field enables a directional switch between nonreciprocal fast and slow light. This discovery may offer new possibilities for pulse time regulation in microwave signal communications, neuromorphic computing, and quantum signal processing.}, archive = {J_PRL}, author = {Jiguang Yao and Chenyang Lu and Xiaolong Fan and Desheng Xue and Greg E. Bridges and C.-M. Hu}, doi = {10.1103/PhysRevLett.134.196904}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196904}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal control of the speed of light using cavity magnonics}, volume = {134}, year = {2025}, }
• (2025). Electrically tunable interband collective excitations in biased bilayer and trilayer graphene. PRL, 134(19), 196903. (www)

  @article{ , abstract = {Collective excitations of charged particles under the influence of an electromagnetic field give rise to a rich variety of hybrid light-matter quasiparticles with unique properties. In metals, intraband collective response manifested by negative permittivity leads to plasmon polaritons with extreme field confinement, wavelength “squeezing,” and potentially low propagation losses. In contrast, photons in semiconductors commonly couple to interband collective response in the form of exciton polaritons, which give rise to completely different polaritonic properties, described by a superposition of the photon and exciton and an anti-crossing of the eigenstates. In this work, we identify the existence of plasmon-like collective excitations originating from the interband excitonic response of biased bilayer and trilayer graphene, in the form of graphene exciton polaritons (GEPs). We find that GEPs possess electrically tunable polaritonic properties and discover that such excitations follow a universal dispersion law for all surface polaritons in 2D excitonic systems. Accounting for nonlocal corrections to the excitonic response, we find that the GEPs exhibit confinement factors that can exceed those of graphene plasmons, and with moderate losses that would enable their observation in cryo-SNOM experiments. These predictions of plasmon-like interband collective excitations in biased graphene systems open up new research avenues for tunable plasmonic phenomena based on excitonic systems, and the ability to control and manipulate such phenomena at the atomic scale.}, archive = {J_PRL}, author = {Tomer Eini and M. F. C. Martins Quintela and J. C. G. Henriques and R. M. Ribeiro and Yarden Mazor and N. M. R. Peres and Itai Epstein}, doi = {10.1103/PhysRevLett.134.196903}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196903}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically tunable interband collective excitations in biased bilayer and trilayer graphene}, volume = {134}, year = {2025}, }
• (2025). Beyond electric-dipole treatment of light-matter interactions in materials: Nondipole harmonic generation in bulk si. PRL, 134(19), 196902. (www)

  @article{ , abstract = {A beyond electric-dipole light-matter theory is needed to describe emerging x-ray and THz applications for characterization and control of quantum materials but inaccessible as nondipole lattice-aperiodic terms impede on the use of Bloch’s theorem. To circumvent this, we derive a formalism that captures dominant nondipole effects in intense electromagnetic fields while conserving lattice translational symmetry. Our approach enables the first accurate nondipole first-principles microscopic simulation of nonperturbative harmonic generation in Si. We reveal nondipole-induced transverse currents generating perturbative even-ordered harmonics and display the onset of nondipole high harmonic generation near the laser damage threshold.}, archive = {J_PRL}, author = {Simon Vendelbo Bylling Jensen and Nicolas Tancogne-Dejean and Angel Rubio and Lars Bojer Madsen}, doi = {10.1103/PhysRevLett.134.196902}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196902}, shortjournal = {Phys. Rev. Lett.}, title = {Beyond electric-dipole treatment of light-matter interactions in materials: Nondipole harmonic generation in bulk si}, volume = {134}, year = {2025}, }
• (2025). Non-hermitian thermophotonic funneling via nonreciprocal surface waves. PRL, 134(19), 196901. (www)

  @article{ , abstract = {Non-Hermitian photonics revolutionizes the understanding and manipulation of wave propagation in open systems. However, due to the interplay of non-Hermitian light-matter interactions and complex long-range couplings, miniaturizing topological features into deep-subwavelength regimes remains a significant challenge, and state-of-the-art explorations have thus far remained on the reciprocal topological photonic states. Here, we introduce nonreciprocal surface waves into deep-subwavelength dimerized lattices to theoretically demonstrate an efficient thermophotonic funnel. The system comprises an array of silicon carbide nanoparticles coupled with a graphene substrate. Under electrical bias, the graphene substrate enables the breaking of time-reversal symmetry in a magnetic-free and compact configuration, while also providing additional channels for photonic-based heat flow. The synergy between nonreciprocal surface waves and collective thermophotonic interactions drives all eigenstates to collapse toward the truncation of the lattice, exhibiting up to a 278-fold enhancement in one-way radiative field intensity. The topological fingerprints of this funneling effect are characterized by point-gap topology and complex-eigenspectrum braiding. Our findings bridge non-Hermitian physics and nonreciprocal thermophotonics, unlocking new possibilities for topological applications.}, archive = {J_PRL}, author = {Shuihua Yang and Guoqiang Xu and Chenglong Zhou and Mengqi Liu and Lei Qu and Jianfeng Chen and Jiaxin Li and Jing Wu and Zhipeng Li and Cheng-Wei Qiu}, doi = {10.1103/PhysRevLett.134.196901}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196901}, shortjournal = {Phys. Rev. Lett.}, title = {Non-hermitian thermophotonic funneling via nonreciprocal surface waves}, volume = {134}, year = {2025}, }
• (2025). Ferroelectricity-driven magnetism in a metal halide monolayer. PRL, 134(19), 196801. (www)

  @article{ , abstract = {Electrical control of magnetism promises potential applications in low-cost, high-density spintronic devices; however, it remains a great challenge in traditional multiferroics. Here we propose that a type-III multiferroic material, where magnetism is driven by ferroelectricity, can be used to achieve effective electrical control of magnetism. We reveal that the emergence of ferroelectricity in a low-dimensional system could significantly reduce the interatomic orbital overlap and narrow the electronic bands, which increases the Stoner instability and, thus, results in a transition from nonmagnetic to ferromagnetic states. Based on first-principles calculations, the ferroelectricity-driven magnetism is demonstrated in a two-dimensional monolayer adsorbed by Cu single atoms (denoted as ). When an out-of-plane shift of the Cu atom induces an out-of-plane ferroelectricity, the system is transferred from a nonmagnetic to a ferromagnetic phase. The revealed type-III multiferroics and electrical control of magnetism offer an innovative strategy for developing multiferroic and magnetoelectric devices.}, archive = {J_PRL}, author = {Jintao Jiang and Fang Wu and Yi Wan and Ang Li and Chengxi Huang and Erjun Kan}, doi = {10.1103/PhysRevLett.134.196801}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196801}, shortjournal = {Phys. Rev. Lett.}, title = {Ferroelectricity-driven magnetism in a metal halide monolayer}, volume = {134}, year = {2025}, }
• (2025). Weak ferromagnetism in altermagnets from alternating g-tensor anisotropy. PRL, 134(19), 196703. (www)

  @article{ , abstract = {Altermagnets are magnetic materials with antiferromagnetic spin ordering but exhibit ferromagnetic properties. Understanding the microscopic origin of the latter is a central problem. Ferromagnetlike properties such as the anomalous Hall effect are linked with weak ferromagnetism, whose microscopic origin in altermagnets remains unclear however. We show theoretically that the alternating g -tensor anisotropy in altermagnets can induce weak orbital ferromagnetism even when the Dzyaloshinskii-Moriya interaction is forbidden. We demonstrate this mechanism to explain weak ferromagnetism for both collinear and noncollinear spin altermagnets. Our findings provide new insights into the origin of weak ferromagnetism and suggest orbital-based ways for manipulating magnetic configurations in altermagnets.}, archive = {J_PRL}, author = {Daegeun Jo and Dongwook Go and Yuriy Mokrousov and Peter M. Oppeneer and Sang-Wook Cheong and Hyun-Woo Lee}, doi = {10.1103/PhysRevLett.134.196703}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196703}, shortjournal = {Phys. Rev. Lett.}, title = {Weak ferromagnetism in altermagnets from alternating g-tensor anisotropy}, volume = {134}, year = {2025}, }
• (2025). Phase diagram of the easy-axis triangular-lattice J1−J2 model. PRL, 134(19), 196702. (www)

  @article{ , abstract = {The phase diagram of the S = 1 / 2 easy-axis triangular-lattice J 1 − J 2 model is investigated using the density-matrix renormalization group and analytical insights. We find a significant spin-liquid region extending from the Heisenberg limit and residing between the Y phase—known as the magnetic analogue of the “supersolid”—and collinear stripe phase. The order parameters of the supersolid are analyzed and an understanding of its lack of a ferromagnetic moment is suggested.}, archive = {J_PRL}, author = {Cesar A. Gallegos and Shengtao Jiang (蒋晟韬 and Steven R. White and A. L. Chernyshev}, doi = {10.1103/PhysRevLett.134.196702}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196702}, shortjournal = {Phys. Rev. Lett.}, title = {Phase diagram of the easy-axis triangular-lattice J1−J2 model}, volume = {134}, year = {2025}, }
• (2025). SU(N) altermagnetism: Lattice models, magnon modes, and flavor-split bands. PRL, 134(19), 196701. (www)

  @article{ , abstract = {Altermagnetism, a type of magnetic order that combines properties of ferro- and antiferromagnets, has stirred great interest lately, not only as a promising source of spintronics applications, but also as a potential gateway to exotic phases of matter. Here, we demonstrate how to generalize collinear altermagnetism to magnets with . Guided by symmetry principles, we present a recipe to construct Heisenberg models for such generalized altermagnets and apply it explicitly for , 4. Using flavor-wave theory, we compute the excitation spectrum of a two-dimensional SU(3) model and show that it exhibits magnon bands with altermagnetic splitting according to magnetic quantum numbers; we connect this quantum-number splitting to the frequently used concept of magnon chirality. We also compute the electronic band structure for a metallic system of the same symmetry and map out the polarization of the resulting flavor-split bands.}, archive = {J_PRL}, author = {Pedro M. Cônsoli and Matthias Vojta}, doi = {10.1103/PhysRevLett.134.196701}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196701}, shortjournal = {Phys. Rev. Lett.}, title = {SU(N) altermagnetism: Lattice models, magnon modes, and flavor-split bands}, volume = {134}, year = {2025}, }
• (2025). Boundary-induced topological chiral extended states in weyl metamaterial waveguides. PRL, 134(19), 196601. (www)

  @article{ , abstract = {In topological physics, it is commonly understood that the existence of the boundary states of a topological system is inherently dictated by its bulk. A classic example is that the surface Fermi-arc states of a Weyl system are determined by the chiral charges of Weyl points within the bulk. Contrasting with this established perspective, here, we theoretically and experimentally discover a family of topological chiral bulk states extending over photonic Weyl metamaterial waveguides, solely induced by the waveguide boundaries, independently of the waveguide width. Notably, these chiral bulk states showcase discrete momenta and function as tunnels that connect Fermi-arc surface states living in different two-dimensional spaces via a third dimension. Our work offers an alternative mechanism for robust chiral bulk transport of waves and highlights the boundaries as a new degree of freedom to regulate bulk Weyl quasiparticles.}, archive = {J_PRL}, author = {Ning Han and Fujia Chen and Mingzhu Li and Rui Zhao and Wenhao Li and Qiaolu Chen and Li Zhang and Yuang Pan and Yuze Hu and Mingyu Tong and Lu Qi and Jingwen Ma and Zhi-Ming Yu and Hongsheng Chen and Yihao Yang}, doi = {10.1103/PhysRevLett.134.196601}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196601}, shortjournal = {Phys. Rev. Lett.}, title = {Boundary-induced topological chiral extended states in weyl metamaterial waveguides}, volume = {134}, year = {2025}, }
• (2025). Distinct terahertz third-harmonic generation of many-body excitonic states. PRL, 134(19), 196503. (www)

  @article{ , abstract = {The dynamics of an electron-hole plasma governed by strong Coulomb interaction is a challenging many-body problem. We report on experimental realization of electron-hole many-body states in the picosecond time scale, with tunable densities in a representative semiconductor Cu 2 O . By using time-resolved optical-pump terahertz third-harmonic-generation spectroscopy, we study the nonlinear terahertz dynamical characteristics of the many-body electron-hole states. We find not only efficient and nonperturbative terahertz third-harmonic yield associated with the excitonic formation but also a nonmonotonic dependence of the excitonic nonlinear response on the electron-hole density, reflecting the exciton dissociation at high charge density. Our results provide an efficient excitonic sensing of the far-from-equilibrium electron-hole many-body states.}, archive = {J_PRL}, author = {Changqing Zhu and Anneke Reinold and Patrick Pilch and Sergey Kovalev and Julian Heckötter and Doris Reiter and Manfred Bayer and Marc Assmann and Zhe Wang}, doi = {10.1103/PhysRevLett.134.196503}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196503}, shortjournal = {Phys. Rev. Lett.}, title = {Distinct terahertz third-harmonic generation of many-body excitonic states}, volume = {134}, year = {2025}, }
• (2025). Intertwined superconductivity and orbital selectivity in a three-orbital hubbard model for the iron pnictides. PRL, 134(19), 196502. (www)

  @article{ , abstract = {We study a three-orbital Hubbard-Kanamori model relevant for iron-based superconductors using variational wave functions explicitly including spatial correlations and electron pairing. We span the nonmagnetic sector from filling , which is representative of undoped iron-based superconductors, to , where a Mott insulating state with each orbital at half filling is found. In the strong-coupling regime, when the electron density is increased, we find a spontaneous differentiation between the occupation of and orbitals, leading to an orbital-selective state with a nematic character that becomes stronger at increasing density. One of these orbitals stays half filled for all densities while the other one hosts (together with the orbital) the excess of electron density. Most importantly, in this regime long-range pairing correlations appear in the orbital with the largest occupation. Our results highlight a strong link between orbital-selective correlations, nematicity, and superconductivity, which requires the presence of a significant Hund’s coupling.}, archive = {J_PRL}, author = {Vito Marino and Alberto Scazzola and Federico Becca and Massimo Capone and Luca F. Tocchio}, doi = {10.1103/PhysRevLett.134.196502}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196502}, shortjournal = {Phys. Rev. Lett.}, title = {Intertwined superconductivity and orbital selectivity in a three-orbital hubbard model for the iron pnictides}, volume = {134}, year = {2025}, }
• (2025). Fractional quantum anomalous hall effect in a singular flat band. PRL, 134(19), 196501. (www)

  @article{ , abstract = {In the search of fractional quantum anomalous Hall (FQAH) effect, the conventional wisdom is to start from a flat Chern band isolated from the rest of the Hilbert space by band gaps, so that many-body interaction can be projected to a landscape that mimics a Landau level. Singular flat bands (SFB), which share protected touching points with other dispersive bands, represent another type of flat landscapes differing from Landau levels and Chern bands in topological and geometric properties. Here we report the finding of FQAH phases in a SFB, which emerges in the bipartite limit of the nearest-neighbor tight-binding model of twisted bilayer . At and filling of the SFB, FQAH effects are demonstrated using density matrix renormalization group calculations with all bands, as well as exact diagonalization calculations with the two touching bands. Gapping the band touching can turn the SFB into a nearly flat Chern band, but counterintuitively this suppresses the FQAH effect, as the gap opening introduces strong inhomogeneity to the quantum geometry. An optical scheme to realize such SFB for cold atoms is provided. Our findings uncover a new arena for the exploration of fractional quantum Hall physics beyond the Landau level and Chern insulator paradigms.}, archive = {J_PRL}, author = {Wenqi Yang and Dawei Zhai and Tixuan Tan and Feng-Ren Fan and Zuzhang Lin and Wang Yao}, doi = {10.1103/PhysRevLett.134.196501}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196501}, shortjournal = {Phys. Rev. Lett.}, title = {Fractional quantum anomalous hall effect in a singular flat band}, volume = {134}, year = {2025}, }
• (2025). Ultracritical floquet non-fermi liquid. PRL, 134(19), 196401. (www)

  @article{ , abstract = {We demonstrate that periodically driven Fermions coupled to simple bosonic baths have steady state occupations of Floquet Bloch bands that generically display nonanalyticities at certain momenta that resemble the Fermi surfaces of equilibrium non-Fermi liquids. Remarkably these nonequilibrium Fermi surfaces remain sharp even when the bath is at finite temperature, leading to critical power-law decaying correlations at finite temperature, a phenomenon with no analog in equilibrium. We also show that generically there is in-gap current rectification for clean metals lacking inversion symmetry, and explain why this occurs universally regardless of the details of collisions.}, archive = {J_PRL}, author = {Li-kun Shi and Oles Matsyshyn and Justin C. W. Song and Inti Sodemann Villadiego}, doi = {10.1103/PhysRevLett.134.196401}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196401}, shortjournal = {Phys. Rev. Lett.}, title = {Ultracritical floquet non-fermi liquid}, volume = {134}, year = {2025}, }
• (2025). Resistivity of non-galilean-invariant two-dimensional dirac systems. PRL, 134(19), 196303. (www)

  @article{ , abstract = {We revisited the influence of electron-electron scattering on the resistivity of a two-dimensional system with a linear spectrum. In conventional systems with a parabolic spectrum, where umklapp scattering is either prohibited or ineffective due to the small Fermi surface, particle-particle scattering does not contribute to conductivity because it does not change the total momentum. However, within the framework of the Boltzmann kinetic model, we demonstrate that electron-electron scattering in Dirac systems can significantly contribute to conductivity, producing distinct temperature-dependent corrections: a behavior at low temperatures and a dependence at moderate temperatures. While the predicted scaling is not observed experimentally—likely suppressed by dominant weak localization effects—the scaling is clearly confirmed in our measurements. Specifically, temperature-dependent resistivity data from a gapless single-valley HgTe quantum well exhibit corrections, which align well with theoretical predictions. Thus, we challenge the paradigm that the term in resistivity is absent in single-band 2D metals.}, archive = {J_PRL}, author = {V. M. Kovalev and M. V. Entin and Z. D. Kvon and A. D. Levin and V. A. Chitta and G. M. Gusev and N. N. Mikhailov}, doi = {10.1103/PhysRevLett.134.196303}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196303}, shortjournal = {Phys. Rev. Lett.}, title = {Resistivity of non-galilean-invariant two-dimensional dirac systems}, volume = {134}, year = {2025}, }
• (2025). Erratic non-hermitian skin localization. PRL, 134(19), 196302. (www)

  @article{ , abstract = {A novel localization phenomenon, termed erratic non-Hermitian skin localization, has been identified in disordered globally reciprocal non-Hermitian lattices. Unlike conventional non-Hermitian skin effect and Anderson localization, it features macroscopic eigenstate localization at irregular, disorder-dependent positions with subexponential decay. Using the Hatano-Nelson model with disordered imaginary gauge fields as a case study, this effect is linked to stochastic interfaces governed by the universal order statistics of random walks. Finite-size scaling analysis confirms the localized nature of the eigenstates. This discovery challenges conventional wave localization paradigms, offering new avenues for understanding and controlling localization phenomena in non-Hermitian physics.}, archive = {J_PRL}, author = {Stefano Longhi}, doi = {10.1103/PhysRevLett.134.196302}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196302}, shortjournal = {Phys. Rev. Lett.}, title = {Erratic non-hermitian skin localization}, volume = {134}, year = {2025}, }
• (2025). Vortical currents and reciprocal relations for transport coefficients in the electron hydrodynamic regime. PRL, 134(19), 196301. (www)

  @article{ , abstract = {We investigate the hydrodynamic regime in metals with momentum-conserving electron-electron scattering. The conservation of momentum results in well-defined dynamics whose effects we investigate via the relevant continuity equations. We find anomalous contributions to the charge and heat transport currents arising from gradients of the velocity field in a semiclassical treatment with a Berry curvature. These contributions are nonvanishing for systems lacking inversion symmetry, and the corresponding transport coefficients do not obey the standard Onsager reciprocity relations. Instead, we show that the response coefficients relating the currents to the stress tensor obey independent reciprocity relations with the stress tensor and thus exhibit cross-tensor effects of charge and heat transport with the momentum transport. The Berry curvature contribution to the stress magnetization tensor is also derived.}, archive = {J_PRL}, author = {Nisarg Chadha and Subroto Mukerjee}, doi = {10.1103/PhysRevLett.134.196301}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196301}, shortjournal = {Phys. Rev. Lett.}, title = {Vortical currents and reciprocal relations for transport coefficients in the electron hydrodynamic regime}, volume = {134}, year = {2025}, }
• (2025). High pressure synthesis of rubidium superhydrides. PRL, 134(19), 196102. (www)

  @article{ , abstract = {Through laser-heated diamond anvil cell experiments, we synthesize a series of rubidium superhydrides and explore their properties with synchrotron x-ray powder diffraction and Raman spectroscopy measurements, combined with density functional theory calculations. Upon heating rubidium monohydride embedded in H 2 at a pressure of 18 GPa, we form RbH 9 − I , which is stable upon decompression down to 8.7 GPa, the lowest stability pressure of any known superhydride. At 22 GPa, another polymorph, RbH 9 − II is synthesised at high temperature. Unique to the Rb-H system among binary metal hydrides is that further compression does not promote the formation of polyhydrides with higher hydrogen content. Instead, heating above 87 GPa yields RbH 5 , which exhibits two polymorphs ( RbH 5 − I and RbH 5 − II ). All of the crystal structures comprise a complex network of quasimolecular H 2 units and H − anions, with RbH 5 providing the first experimental evidence of linear H 3 − anions.}, archive = {J_PRL}, author = {Mikhail A. Kuzovnikov and Busheng Wang and Xiaoyu Wang and Tomas Marqueño and Hannah A. Shuttleworth and Calum Strain and Eugene Gregoryanz and Eva Zurek and Miriam Peña-Alvarez and Ross T. Howie}, doi = {10.1103/PhysRevLett.134.196102}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196102}, shortjournal = {Phys. Rev. Lett.}, title = {High pressure synthesis of rubidium superhydrides}, volume = {134}, year = {2025}, }
• (2025). Quartic scaling of sound attenuation with frequency in vitreous silica. PRL, 134(19), 196101. (www)

  @article{ , abstract = {Many theories predict a quartic increase of the acoustic damping at sub-THz frequencies in glassy media, related to the excess vibrational modes known as the boson peak anomaly. Here by introducing phase-sensitive acoustic spectroscopy techniques with a THz bandwidth, we investigate the acoustic properties of vitreous silica at 15 and 300 K in the crucial but unexplored sub-THz gap region below the boson peak. Our results indicate a negative dispersion below the THz range and the onset of an athermal quartic frequency scaling acoustic attenuation term, which appears above all other thermal losses.}, archive = {J_PRL}, author = {Peng-Jui Wang and Agnès Huynh and Jinn-Kong Sheu and Xavier Lafosse and Aristide Lemaître and Benoit Rufflé and René Vacher and Bernard Perrin and Chi-Kuang Sun and Marie Foret}, doi = {10.1103/PhysRevLett.134.196101}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196101}, shortjournal = {Phys. Rev. Lett.}, title = {Quartic scaling of sound attenuation with frequency in vitreous silica}, volume = {134}, year = {2025}, }
• (2025). Quantum size effects on andreev transport in Nb/Au/Nb josephson junctions: A combined ab initio and experimental study. PRL, 134(19), 196002. (www)

  @article{ , abstract = {We have measured the critical current density, superconducting coherence length, and superconducting transition temperature of single-domain, epitaxially grown trilayers, all of which show a nonmonotonic dependence on the thickness of the Au layer. These results are compared with the predictions of a relativistic, ab initio theory, which incorporates superconducting correlations. We find good agreement with experiment, coming from a rich interplay between superconducting proximity and quantum size effects, mediated by Andreev bound states. These results suggest that quantum size effects could provide a systematic method of controlling the transport properties of superconducting multilayers.}, archive = {J_PRL}, author = {Hiroki Yamazaki and Gábor Csire and Nóra Kucska and Nic Shannon and Balázs Győrffy and Hidenori Takagi and Balázs Újfalussy}, doi = {10.1103/PhysRevLett.134.196002}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196002}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum size effects on andreev transport in Nb/Au/Nb josephson junctions: A combined ab initio and experimental study}, volume = {134}, year = {2025}, }
• (2025). Enhancement of superconductivity by anderson localization in three-dimensional crystalline phase of BiSe. PRL, 134(19), 196001. (www)

  @article{ , abstract = {We report a remarkable enhancement of superconductivity near the Anderson metal-insulator transition in the three-dimensional (3D) BCS-superconductor bismuth selenide (BiSe). The SnSe-type orthorhombic BiSe is successfully stabilized upon decompression after this phase is formed at high pressure from the two-dimensional layered BiSe phase and the intrinsic disorder concomitantly approaches the localization threshold near ambient pressure. A dramatic enhancement of the superconducting transition temperature near the localization transition is associated with the sharp increase in the local density of states and significant increase in the background dielectric constant, hence providing a short-ranged Coulomb interaction. This study, for the first time, validates the theoretical formulation for the superconductivity enhancement in a 3D system near localization and demonstrates the novel compression-decompression route to induce high homogeneous disorder.}, archive = {J_PRL}, author = {Pallavi Malavi and S. Karmakar}, doi = {10.1103/PhysRevLett.134.196001}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {196001}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancement of superconductivity by anderson localization in three-dimensional crystalline phase of BiSe}, volume = {134}, year = {2025}, }
• (2025). Spontaneous capillary-inertial dewetting at the microscopic scale. PRL, 134(19), 194001. (www)

  @article{ , abstract = {We resolve the dewetting dynamics of water films on partially wetting surfaces at the microscopic scale and highlight its distinctions from liquid wetting. Fast dewetting occurring at the millisecond scale is dominated by capillary and inertial forces, obeying a power law with a wettability-independent exponent, which is different from the capillary-inertial dynamic wetting. Molecular-level inspections of moving contact lines further reveal that liquid molecules retract from solid surfaces through a rolling motion, whereas dynamic wetting proceeds mainly with the sliding motion. These distinct hydrodynamic behaviors and molecular kinetics explicitly suggest that dynamic dewetting is not simply the reverse of dynamic wetting, which has significant implications for interfacial fluid physics.}, archive = {J_PRL}, author = {Yile Wang and Yakang Jin and Youquan Jia and Elmar Bonaccurso and Huali Yu and Xu Deng and Zhigang Li and Longquan Chen}, doi = {10.1103/PhysRevLett.134.194001}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {194001}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous capillary-inertial dewetting at the microscopic scale}, volume = {134}, year = {2025}, }
• (2025). Manipulation of strongly interacting solitons in optical fiber experiments. PRL, 134(19), 193804. (www)

  @article{ , abstract = {The model underlying physics of guiding light in single-mode fibers—the one-dimensional nonlinear Schrödinger equation (NLSE)—reveals a remarkable balance of the fiber dispersion and nonlinearity, leading to the existence of optical solitons. With the inverse scattering transform (IST) method and its perturbation theory extension, one can go beyond single-soliton physics and investigate nonlinear dynamics of complex optical pulses driven by soliton interactions. Here, advancing the IST perturbation theory approach, we introduce the eigenvalue response functions, which provide an intuitively clear way to manipulate individual characteristics of solitons even in the case of their entire overlapping, i.e., very strong interactions. The response functions reveal the spatial sensitivity of the multisoliton pulse concerning its instantaneous perturbations, allowing one to manipulate the velocities and amplitudes of each soliton. Based on a recirculating optical fiber loop system and homodyne measurement, our experimental setup enables observation of long-distance spatiotemporal NLSE dynamics and complete phase-amplitude characterization of optical pulses containing several solitons, which provides accurate experimental IST spectra. Adding a localized phase perturbation on a box-shaped wave field, we change individual soliton characteristics and can detach solitons selectively from the whole pulse. The detached solitons exhibit velocities very close to the theoretical predictions, thereby demonstrating the efficiency and robustness of the response functions approach.}, archive = {J_PRL}, author = {Alexandre Mucci and Pierre Suret and François Copie and Stephane Randoux and Rustam Mullyadzhanov and Andrey Gelash}, doi = {10.1103/PhysRevLett.134.193804}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193804}, shortjournal = {Phys. Rev. Lett.}, title = {Manipulation of strongly interacting solitons in optical fiber experiments}, volume = {134}, year = {2025}, }
• (2025). Nonlinear semiclassical spectroscopy of ultrafast molecular polariton dynamics. PRL, 134(19), 193803. (www)

  @article{ , abstract = {We introduce a theoretical framework that allows for the systematic and efficient description of the ultrafast nonlinear response of molecular polaritons, i.e., hybrid light-matter states, in the collective regime of large numbers of molecules coupled to the cavity photon mode. Our approach is based on a semiclassical, mean-field evolution of the molecular Hamiltonian and the cavity field, which is complemented by a perturbative expansion of both light and matter counterparts in the input fields entering the cavity. In addition, expansion in terms of the pulse phases enables us to disentangle different excitation pathways in Liouville space, thereby distinguishing contributions to the nonlinear response. The formalism extends traditional free-space nonlinear spectroscopy by incorporating the feedback of matter onto the light field via the induced polarization. We demonstrate the utility of the framework by applying it to the calculation of pump-probe polariton spectra and show how, by storing the pulses, the cavity facilitates additional excitation pathways, which can be used to isolate purely bright state contributions. Our method, which does not scale with , is broadly applicable and can be extended to model a wide range of current experiments investigating the dynamical nonlinear response of hybrid light-matter states.}, archive = {J_PRL}, author = {Michael Reitz and Arghadip Koner and Joel Yuen-Zhou}, doi = {10.1103/PhysRevLett.134.193803}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193803}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear semiclassical spectroscopy of ultrafast molecular polariton dynamics}, volume = {134}, year = {2025}, }
• (2025). On-chip parametric synchronization of a dissipative kerr soliton microcomb. PRL, 134(19), 193802. (www)

  @article{ , abstract = {Synchronization of oscillators is ubiquitous in nature. Often, the synchronized oscillators couple directly, yet in some cases synchronization can arise from their parametric interactions. Here, we theoretically predict and experimentally demonstrate the parametric synchronization of a dissipative Kerr soliton frequency comb. We specifically show that the parametric interaction between the soliton and two auxiliary lasers permits the entrainment of the frequency comb repetition rate. Besides representing the first prediction and demonstration of parametric synchronization of soliton frequency combs, our scheme offers significant flexibility for all-optical metrological-scale stabilization of the comb.}, archive = {J_PRL}, author = {Grégory Moille and Pradyoth Shandilya and Miro Erkintalo and Curtis R. Menyuk and Kartik Srinivasan}, doi = {10.1103/PhysRevLett.134.193802}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193802}, shortjournal = {Phys. Rev. Lett.}, title = {On-chip parametric synchronization of a dissipative kerr soliton microcomb}, volume = {134}, year = {2025}, }
• (2025). Nonmonotonic radiative heat transfer in the transition from far field to near field. PRL, 134(19), 193801. (www)

  @article{ , abstract = {We present high precision measurements of the radiative heat transfer of a glass microsphere immersed in a thermal bath in vacuum facing three different planar substrates ( , SiC, and Au), which exhibit very different optical behaviors in the infrared region. Using a thermoresistive probe on a cantilever, we show the nonmonotonic behavior of the radiative flux between the microsphere and its environment when the microsphere is brought closer to the substrate in the far-field to near-field transition regime. We demonstrate that this unexpected behavior is related to the singularities of dressed emission mechanisms in this three-body system sphere-substrate bath with respect to the separation distance.}, archive = {J_PRL}, author = {Victor Guillemot and Riccardo Messina and Valentina Krachmalnicoff and Rémi Carminati and Philippe Ben-Abdallah and Wilfrid Poirier and Yannick De Wilde}, doi = {10.1103/PhysRevLett.134.193801}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193801}, shortjournal = {Phys. Rev. Lett.}, title = {Nonmonotonic radiative heat transfer in the transition from far field to near field}, volume = {134}, year = {2025}, }
• (2025). Experimental observation of parity-symmetry-protected phenomena in the quantum rabi model with a trapped ion. PRL, 134(19), 193604. (www)

  @article{ , abstract = {Symmetry is crucial for gaining insights into the fundamental properties of physical systems, bringing possibilities in studying exotic phenomena such as quantum phase transitions and ground-state entanglement. Here, we experimentally simulate a highly controllable extended quantum Rabi model, capable of tuning into the ultrastrong or deep coupling regime, in a spin-motion-coupled trapped ion. We observe that the phonon driven by such a model with Z 2 symmetry preserved (broken) would experience double (single) excitation in the ultrastrong coupling regime. Quantum phenomena such as strong ground-state entanglement and quantum superposition in systems occur with parity symmetry, and these phenomena disappear following the symmetry breaking. We also find sensitive responses for the two-level system entropy and phonon Wigner function in the deep coupling regime, depending on the parameter across the symmetry transition point. This Letter offers the prospect of exploring symmetry-controlled quantum phenomena and their applications in high-precision quantum technologies.}, archive = {J_PRL}, author = {Xingyu Zhao and Qian Bin and Waner Hou and Yi Li and Yue Li and Yiheng Lin and Xin-You Lü and Jiangfeng Du}, doi = {10.1103/PhysRevLett.134.193604}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193604}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental observation of parity-symmetry-protected phenomena in the quantum rabi model with a trapped ion}, volume = {134}, year = {2025}, }
• (2025). Nonreciprocal interactions induce frequency shifts in superradiant lasers. PRL, 134(19), 193603. (www)

  @article{ , abstract = {Superradiant lasers, which consist of incoherently driven atoms coupled to a lossy cavity, are a promising source of coherent light due to their stable frequency and superior narrow linewidth. We show that when a fraction of the atoms is not driven, a shift in the lasing frequency and a broadening of the linewidth occur, limiting the performance of a superradiant laser. We explain this behavior by identifying nonreciprocal interactions between driven and undriven atoms, i.e., competing alignment and antialignment of their dipoles. Our results have implications for the realization of superradiant lasers, establishing the relevance of nonreciprocal phenomena for quantum technologies.}, archive = {J_PRL}, author = {Tobias Nadolny and Matteo Brunelli and Christoph Bruder}, doi = {10.1103/PhysRevLett.134.193603}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193603}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal interactions induce frequency shifts in superradiant lasers}, volume = {134}, year = {2025}, }
• (2025). Zak phase induced topological nonreciprocity. PRL, 134(19), 193602. (www)

  @article{ , abstract = {Topological physics provides novel insights for designing functional photonic devices, such as magnetic-free optical diodes, which are important in optical engineering and quantum information processing. Past efforts mostly focus on the topological edge modes in two-dimensional (2D) photonic Chern lattices, which, however, require delicate fabrication and temporal modulation. In particular, the 1D nonreciprocal edge mode needs to be embedded in a 2D lattice, contradicting with the compactness of integrated photonics. To address these challenges, we investigate the optical nonreciprocity of the 1D Su-Schrieffer-Heeger (SSH) superradiance lattices in room-temperature atoms. The probe fields propagating in two opposite directions perceive two different SSH topological phases, which have different absorption spectra due to the interplay between the Zak phase and the thermal motion of atoms, resulting in optical nonreciprocity. Our findings reveal the relationship between 1D topological matter and optical nonreciprocity, simplifying the design of topologically resilient nonreciprocal devices.}, archive = {J_PRL}, author = {Xiao Liu and Jiefei Wang and Ruosong Mao and Huizhu Hu and Shi-Yao Zhu and Xingqi Xu and Han Cai and Da-Wei Wang}, doi = {10.1103/PhysRevLett.134.193602}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193602}, shortjournal = {Phys. Rev. Lett.}, title = {Zak phase induced topological nonreciprocity}, volume = {134}, year = {2025}, }
• (2025). Quantum states imaging of magnetic field contours based on autler-townes effect in ytterbium atoms. PRL, 134(19), 193201. (www)

  @article{ , abstract = {An intercombination transition in Yb enables a novel approach for rapidly imaging magnetic field variations with excellent spatial and temporal resolution and accuracy. This quantum imaging magnetometer reveals “dark stripes” that are contours of constant magnetic field visible by eye or capturable by standard cameras. These dark lines result from a combination of Autler-Townes splitting and the spatial Hanle effect in the transition of Yb when driven by multiple strong coherent laser fields (carrier and AM/FM modulation sidebands of a single-mode 556 nm laser). We show good agreement between experimental data and our theoretical model for the closed, 4-level Zeeman shifted V system and demonstrate scalar and vector magnetic field measurements at video frame rates over spatial dimensions of 5 cm with 0.1 mm resolution. Additionally, the transition allows for response time and a large dynamic range (from microtesla to many tesla).}, archive = {J_PRL}, author = {Tanaporn Na Narong and Hongquan Li and Joshua Tong and Mario Dueñas and Leo Hollberg}, doi = {10.1103/PhysRevLett.134.193201}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum states imaging of magnetic field contours based on autler-townes effect in ytterbium atoms}, volume = {134}, year = {2025}, }
• (2025). Time-resolved cryogenic action spectroscopy of dipole-bound states in phenoxide. PRL, 134(19), 193002. (www)

  @article{ , abstract = {Dipole-bound states of cryogenically cooled phenoxide anions (deprotonated phenol) have been investigated by combining trapping in a 6 K ion trap and subsequent action-absorption spectroscopy in an ion-storage ring. As action we consider creation of neutral phenoxy radicals. A multitude of dipole-bound resonances, not previously observed, are assigned to vibrations in the phenoxyl radical core molecule. By using the storage ring, we include prompt as well as delayed light-induced action. The dipole-bound states decay primarily by prompt action (faster than ), but some resonance states live longer than . This suggests that in addition to vibrational autodetachment, internal conversion with subsequent thermionic emission from a hot electronic ground state may be operative. The resonances associated with the delayed decay are red-shifted relative to those of the faster (prompt) decay, which may imply that rotations play a role for the excited-state dynamics.}, archive = {J_PRL}, author = {L. H. Andersen and A. P. Rasmussen and H. B. Pedersen and N. Klinkby}, doi = {10.1103/PhysRevLett.134.193002}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193002}, shortjournal = {Phys. Rev. Lett.}, title = {Time-resolved cryogenic action spectroscopy of dipole-bound states in phenoxide}, volume = {134}, year = {2025}, }
• (2025). Orbital collapse in exotic atoms and its effect on dynamics. PRL, 134(19), 193001. (www)

  @article{ , abstract = {We study the energy structures of muonic Ar atoms and find the muon orbital collapses at a critical angular momentum using density-functional theory (DFT). The may provide an upper limit for the muon-captured states in muon-Ar collisions. We confirm the existence of this upper limit by calculating the state-specified capture probability using the time-dependent Schrödinger equation (TDSE) and the classical trajectory Monte Carlo (CTMC) method with the single-active-particle approximation. Modifying the mapping between the classical orbital energy and the principal quantum number led to a reasonable agreement in the state-specified muon capture probabilities obtained by the TDSE and CTMC methods. We propose a simple method to estimate for exotic noble atoms from atomic model potentials. The estimated values agree with those calculated by DFT.}, archive = {J_PRL}, author = {X. M. Tong and K. Tőkési and D. Kato and T. Okumura and S. Okada and T. Azuma}, doi = {10.1103/PhysRevLett.134.193001}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {193001}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital collapse in exotic atoms and its effect on dynamics}, volume = {134}, year = {2025}, }
• (2025). Spin response of neutron matter in ab initio approach. PRL, 134(19), 192701. (www)

  @article{ , abstract = {We propose a general method embedded in the ab initio nuclear framework to reconstruct linear response functions and calculate sum rules. Within our approach, based on the Gaussian integral transform, we consistently treat the ground state and the excited spectrum. Crucially, the method allows for a robust uncertainty estimation of the spectral reconstruction. We employ it to obtain the spin response in neutron matter. Our calculations are performed using state-of-the-art many-body coupled-cluster method and Hamiltonians derived in the chiral effective field theory, emphasizing the analysis of finite-size effects. Our findings reveal that the spin response exhibits a strong dependence on both nuclear interactions and many-body wave functions, offering a new avenue for exploring nuclear correlations and dynamics in infinite systems. This work serves as a stepping stone toward further studies of neutrino interactions in astrophysical environments from first principles.}, archive = {J_PRL}, author = {J. E. Sobczyk and W. Jiang and A. Roggero}, doi = {10.1103/PhysRevLett.134.192701}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {192701}, shortjournal = {Phys. Rev. Lett.}, title = {Spin response of neutron matter in ab initio approach}, volume = {134}, year = {2025}, }
• (2025). QED corrections to the parity-violating asymmetry in high-energy electron-nucleus collisions. PRL, 134(19), 192501. (www)

  @article{ , abstract = {The parity-violating asymmetry, including leading-order QED corrections to the Coulomb potential, is calculated nonperturbatively by solving the Dirac equation. At GeV collision energies and forward scattering angles, QED effects enhance the asymmetry by approximately 5% for the recently measured nuclei , and . The corrections result in a shift of the estimated neutron radius, leading to an increase in the inferred neutron skin thicknesses of these nuclei and, thus, to the pressure neutrons feel around nuclear saturation density.}, archive = {J_PRL}, author = {Xavier Roca-Maza and D. H. Jakubassa-Amundsen}, doi = {10.1103/PhysRevLett.134.192501}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {192501}, shortjournal = {Phys. Rev. Lett.}, title = {QED corrections to the parity-violating asymmetry in high-energy electron-nucleus collisions}, volume = {134}, year = {2025}, }
• (2025). Zero-jettiness soft function to third order in perturbative QCD. PRL, 134(19), 191902. (www)

  @article{ , abstract = {We present the high-precision result for the zero-jettiness soft function at next-to-next-to-next-to-leading order (N3LO) in perturbative QCD. At this perturbative order, the soft function is the last missing ingredient required for the computation of a hadronic color singlet production or a color singlet decay into two jets using the zero-jettiness variable as the slicing parameter. Furthermore, the knowledge of the N3LO soft function enables the resummed description of the thrust distribution in the process e + e − → hadrons through next-to-next-to-next-to-leading logarithmic order, which is important for the extraction of the strong coupling constant using this shape variable. On the methodological side, the complexity of the zero-jettiness variable forced us to develop a new semi-analytic method for phase-space integration in the presence of constraints parameterized through Heaviside functions which, hopefully, will be useful for further development of the N -jettiness slicing scheme.}, archive = {J_PRL}, author = {Daniel Baranowski and Maximilian Delto and Kirill Melnikov and Andrey Pikelner and Chen-Yu Wang}, doi = {10.1103/PhysRevLett.134.191902}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191902}, shortjournal = {Phys. Rev. Lett.}, title = {Zero-jettiness soft function to third order in perturbative QCD}, volume = {134}, year = {2025}, }
• (2025). Observation of an axial-vector state in the study of the decay ψ(3686)→ϕηη′. PRL, 134(19), 191901. (www)

  @article{ , abstract = {Using ( 2712.4 ± 14.3 ) × 10 6 ψ ( 3686 ) events collected with the BESIII detector at BEPCII, a partial wave analysis of the decay ψ ( 3686 ) → ϕ η η ′ is performed with the covariant tensor approach. In addition to the established states h 1 ( 1900 ) and ϕ ( 2170 ) , an axial-vector state with a mass near 2.3 GeV / c 2 is observed for the first time. Its mass and width are measured to be 2316 ± 9 stat ± 3 0 syst MeV / c 2 and 89 ± 1 5 stat ± 2 6 syst MeV , respectively. The product branching fractions of B [ ψ ( 3686 ) → X ( 2300 ) η ′ ] B [ X ( 2300 ) → ϕ η ] and B [ ψ ( 3686 ) → X ( 2300 ) η ] B [ X ( 2300 ) → ϕ η ′ ] are determined to be ( 4.8 ± 1.3 stat ± 0.7 syst ) × 10 − 6 and ( 2.2 ± 0.7 stat ± 0.7 syst ) × 10 − 6 , respectively. The branching fraction B [ ψ ( 3686 ) → ϕ η η ′ ] is measured for the first time to be ( 3.14 ± 0.1 7 stat ± 0.2 4 syst ) × 10 − 5 . The first uncertainties are statistical and the second are systematic.}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and J. F. Chang and W. L. Chang and G. R. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and K. Fischer and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and Z. L. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and M. Irshad and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and J. J. Lane and P. Larin and L. Lavezzi and T. T. Lei and Z. H. Lei and H. Leithoff and M. Lellmann and T. Lenz and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and Ke Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and Xiaoyu Li and Y. G. Li and Z. J. Li and Z. X. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. Z. Liao and Y. P. Liao and J. Libby and A. Limphirat and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. H. Liu and Fang Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. M. Liu and Huanhuan Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and X. T. Ma and X. Y. Ma and Y. Ma and Y. M. Ma and F. E. Maas and M. Maggiora and S. Malde and A. Mangoni and Y. J. Mao and Z. P. Mao and S. Marcello and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and P. Patteri and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and S. Q. Qu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. C. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and R. S. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and Meng Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. Wei and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. C. Xu and Z. P. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and Tao Yang and Y. Yang and Y. F. Yang and Y. X. Yang and Yifan Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and Shuihan Zhang and Shulei Zhang and X. D. Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Yao Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and Lei Zhao and Ling Zhao and M. G. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and J. Zhu and K. Zhu and K. J. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and S. Q. Zhu and T. J. Zhu and W. J. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.191901}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of an axial-vector state in the study of the decay ψ(3686)→ϕηη′}, volume = {134}, year = {2025}, }
• (2025). Construction of a gapless phase with haagerup symmetry. PRL, 134(19), 191602. (www)

  @article{ , abstract = {We construct a ( 1 + 1 ) d gapless theory which has Haagerup H 3 symmetry. The construction relies on the recent exploration of the categorical Landau paradigm applied to fusion category symmetries. First, using the symmetry topological field theory, we construct all gapped phases with Haagerup symmetry. Extending this construction to gapless phases, we study the second order phase transition between gapped phases, and determine analytically a Haagerup-symmetric conformal field theory. This is given in terms of two copies of the three-state Potts model, on which we realize the full H 3 symmetry action and determine the relevant deformations to the H 3 -symmetric gapped phases. This continuum analysis is corroborated by a lattice model construction of the gapped and gapless phases, using the anyon chain.}, archive = {J_PRL}, author = {Lea E. Bottini and Sakura Schäfer-Nameki}, doi = {10.1103/PhysRevLett.134.191602}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191602}, shortjournal = {Phys. Rev. Lett.}, title = {Construction of a gapless phase with haagerup symmetry}, volume = {134}, year = {2025}, }
• (2025). I-extremization with baryonic charges. PRL, 134(19), 191601. (www)

  @article{ , abstract = {We propose an entropy function for AdS 4 BPS black holes in M theory with general magnetic charges, resolving in particular a long-standing puzzle about baryonic charges. The entropy function is constructed from a gravitational block defined solely in terms of topological data of the internal manifold. We show that the entropy of twisted black holes can always be reformulated as an I -extremization problem—even in cases where existing large- N field theory computations fail to provide an answer. Furthermore, we correctly reproduce the entropy for a class of known black holes with purely baryonic magnetic charges. Our results offer both a conjecture for the general gravitational block for AdS 4 black holes in M theory and a prediction for the large- N limit of several partition functions whose saddle points have yet to be found.}, archive = {J_PRL}, author = {Seyed Morteza Hosseini and Alberto Zaffaroni}, doi = {10.1103/PhysRevLett.134.191601}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191601}, shortjournal = {Phys. Rev. Lett.}, title = {I-extremization with baryonic charges}, volume = {134}, year = {2025}, }
• (2025). Bayesian search of massive scalar fields from LIGO-virgo-KAGRA binaries. PRL, 134(19), 191402. (www)

  @article{ , abstract = {Massive scalar fields are promising candidates for addressing many unresolved problems in fundamental physics. We report the first model-agnostic Bayesian search of massive scalar fields that are nonminimally coupled to gravity in LIGO/Virgo/KAGRA gravitational-wave data. We find no evidence for such fields and place the most stringent upper limits on their coupling for scalar masses . We exemplify the strength of these bounds by applying them to massive scalar-Gauss-Bonnet gravity, finding the tightest constraints on the coupling constant to date, for scalar masses to 90% credible level.}, archive = {J_PRL}, author = {Yiqi Xie and Adrian Ka-Wai Chung and Thomas P. Sotiriou and Nicolás Yunes}, doi = {10.1103/PhysRevLett.134.191402}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191402}, shortjournal = {Phys. Rev. Lett.}, title = {Bayesian search of massive scalar fields from LIGO-virgo-KAGRA binaries}, volume = {134}, year = {2025}, }
• (2025). Isospectrality in effective field theory extensions of general relativity. PRL, 134(19), 191401. (www)

  @article{ , abstract = {Two universal predictions of general relativity are the propagation of gravitational waves of large momentum along null geodesics and the isospectrality of quasinormal modes in many families of black holes. In extensions of general relativity, these properties are typically lost: quasinormal modes are no longer isospectral and gravitational wave propagation is no longer geodesic and it exhibits birefringence—polarization-dependent speed. We study these effects in an effective-field-theory extension of general relativity with up to eight-derivative terms and show that there is a unique Lagrangian that has a nonbirefringent dispersion relation for gravitational waves and isospectral quasinormal modes in the eikonal limit. We argue that both properties are related through a generalized correspondence between eikonal quasinormal modes and unstable photon-sphere orbits. These properties define a special class of theories that we denote as isospectral effective field theories. We note that the lowest-order isospectral correction to general relativity coincides with the quartic-curvature correction arising from type II string theory, suggesting that isospectrality might be a key feature of quantum gravity.}, archive = {J_PRL}, author = {Pablo A. Cano and Marina David}, doi = {10.1103/PhysRevLett.134.191401}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191401}, shortjournal = {Phys. Rev. Lett.}, title = {Isospectrality in effective field theory extensions of general relativity}, volume = {134}, year = {2025}, }
• (2025). Cold dark matter based on an analogy with superconductivity. PRL, 134(19), 191004. (www)

  @article{ , abstract = {We present a novel candidate for cold dark matter consisting of condensed Cooper pairs in a theory of interacting fermions with broken chiral symmetry. Establishing the thermal history from the early radiation era to the present, the fermions are shown to behave like standard radiation at high temperatures, but then experience a critical era decaying faster than radiation, akin to freeze-out, which sets the relic abundance. Through a second-order phase transition, fermion-antifermion pairs condense and the system asymptotes toward zero temperature and pressure. By the present era, the nonrelativistic, massive condensate decays slightly faster than in the standard scenario–a unique prediction that may be tested by combined measurements of the cosmic microwave background and large scale structure. We also show that in the case of massive fermions, the phase transition is frustrated, and instead leaves a residual, long-lived source of dark energy.}, archive = {J_PRL}, author = {Guanming Liang (梁冠铭 and Robert R. Caldwell}, doi = {10.1103/PhysRevLett.134.191004}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191004}, shortjournal = {Phys. Rev. Lett.}, title = {Cold dark matter based on an analogy with superconductivity}, volume = {134}, year = {2025}, }
• (2025). Dilatonic couplings and the relic abundance of ultralight dark matter. PRL, 134(19), 191003. (www)

  @article{ , abstract = {Models of scalar field dark matter where the scalar is a dilaton have a special behavior, since nontrivial couplings, d , to matter result in a contribution to the potential for the field that is proportional to the trace of the stress-energy tensor. We look in more detail at the dilaton mass, m ϕ , and initial conditions required to yield the correct relic abundance for couplings that are not already excluded by terrestrial experiments. In minimal models with only couplings accessible to terrestrial searches, we find that dilaton dark matter with m ϕ ≳ 10 − 10 eV requires couplings suppressed compared to constraints from equivalence principle tests and fifth force searches in order to not produce too much dark matter, improving on the strongest current experimental constraints by up to ∼ O ( 10 ) , with consequences for the proposed mechanical resonator dilaton dark matter searches. In nonminimal or universally coupled models, the unconstrained couplings of the dilaton to, e.g., the top quark can strongly influence the relic abundance at all masses. In particular, this implies that atom interferometry searches at masses m ϕ ≈ 10 − 19 eV are unable to constrain the early Universe behavior or UV physics of the dilaton. We also find that dilatonic couplings allow for compatibility of m ϕ ≳ 10 − 7 eV with an observably large tensor-to-scalar ratio in the cosmic microwave background, which is not possible for a decoupled scalar of the same mass.}, archive = {J_PRL}, author = {Ahmad Alachkar and Malcolm Fairbairn and David J. E. Marsh}, doi = {10.1103/PhysRevLett.134.191003}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191003}, shortjournal = {Phys. Rev. Lett.}, title = {Dilatonic couplings and the relic abundance of ultralight dark matter}, volume = {134}, year = {2025}, }
• (2025). Optimal factorization of cosmological large-scale structure observables. PRL, 134(19), 191002. (www)

  @article{ , abstract = {We introduce cobra (Cosmology with Optimally factorized Bases for Rapid Approximation), a novel framework for rapid computation of large-scale structure observables. cobra separates scale dependence from cosmological parameters in the linear matter power spectrum while also minimizing the number of necessary basis terms , thus enabling direct and efficient computation of derived and nonlinear observables. Moreover, the dependence on cosmological parameters is efficiently approximated using radial basis function interpolation. We apply our framework to decompose the linear matter power spectrum in the standard scenario, as well as by adding curvature, dynamical dark energy and massive neutrinos, covering all redshifts relevant for Stage IV surveys. With only a dozen basis terms , cobra reproduces exact Boltzmann solver calculations to precision, which improves further to in the pure scenario. Using our decomposition, we recast the one-loop redshift space galaxy power spectrum in a separable minimal-basis form, enabling model evaluations per second at precision on a single thread. This constitutes a considerable improvement over previously existing methods (e.g., FFTLog) opening a new window for efficient computations of higher loop and higher order correlators involving multiple powers of the linear matter power spectra. The resulting factorization can also be utilized in clustering, weak lensing, and CMB analyses.}, archive = {J_PRL}, author = {Thomas Bakx and Nora Elisa Chisari and Zvonimir Vlah}, doi = {10.1103/PhysRevLett.134.191002}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191002}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal factorization of cosmological large-scale structure observables}, volume = {134}, year = {2025}, }
• (2025). Observation of a spectral hardening in cosmic ray boron spectrum with the DAMPE space mission. PRL, 134(19), 191001. (www)

  @article{ , abstract = {Secondary cosmic ray fluxes are important probes of the propagation and interaction of high-energy particles in the Galaxy. Recent measurements of primary and secondary cosmic ray nuclei have revealed unexpected spectral features that demand a deeper understanding. In this work we report the direct measurement of the cosmic ray boron spectrum from to with eight years of data collected by the Dark Matter Particle Explorer (DAMPE) mission. The measured spectrum shows a hardening at with a spectral index of before the break and an index change of after the break. A simple power law model is disfavored at a confidence level of . Compared with the hardenings measured in the DAMPE proton and helium spectra, the secondary boron spectrum hardens roughly twice as much as these primaries, which is consistent with a propagation related mechanism to interpret the spectral hardenings of cosmic rays observed at hundreds of .}, archive = {J_PRL}, author = {DAMPE Collaboration and F. Alemanno and C. Altomare and Q. An and P. Azzarello and F. C. T. Barbato and P. Bernardini and X. J. Bi and H. Boutin and I. Cagnoli and M. S. Cai and E. Casilli and E. Catanzani and J. Chang and D. Y. Chen and J. L. Chen and Z. F. Chen and Z. X. Chen and P. Coppin and M. Y. Cui and T. S. Cui and Y. X. Cui and I. De Mitri and F. de Palma and A. Di Giovanni and T. K. Dong and Z. X. Dong and G. Donvito and D. Droz and J. L. Duan and K. K. Duan and R. R. Fan and Y. Z. Fan and F. Fang and K. Fang and C. Q. Feng and L. Feng and J. M. Frieden and P. Fusco and M. Gao and F. Gargano and E. Ghose and K. Gong and Y. Z. Gong and D. Y. Guo and J. H. Guo and S. X. Han and Y. M. Hu and G. S. Huang and X. Y. Huang and Y. Y. Huang and M. Ionica and L. Y. Jiang and Y. Z. Jiang and W. Jiang and J. Kong and A. Kotenko and D. Kyratzis and S. J. Lei and W. H. Li and W. L. Li and X. Li and X. Q. Li and Y. M. Liang and C. M. Liu and H. Liu and J. Liu and S. B. Liu and Y. Liu and F. Loparco and M. Ma and P. X. Ma and T. Ma and X. Y. Ma and G. Marsella and M. N. Mazziotta and D. Mo and X. Y. Niu and A. Parenti and W. X. Peng and X. Y. Peng and C. Perrina and E. Putti-Garcia and R. Qiao and J. N. Rao and R. Sarkar and P. Savina and A. Serpolla and Z. Shangguan and W. H. Shen and Z. Q. Shen and Z. T. Shen and L. Silveri and J. X. Song and M. Stolpovskiy and H. Su and M. Su and H. R. Sun and Z. Y. Sun and A. Surdo and X. J. Teng and A. Tykhonov and J. Z. Wang and L. G. Wang and S. Wang and X. L. Wang and Y. F. Wang and Y. Wang and D. M. Wei and J. J. Wei and Y. F. Wei and D. Wu and J. Wu and S. S. Wu and X. Wu and Z. Q. Xia and E. H. Xu and H. T. Xu and J. Xu and Z. H. Xu and Z. L. Xu and Z. Z. Xu and G. F. Xue and H. B. Yang and P. Yang and Y. Q. Yang and H. J. Yao and Y. H. Yu and Q. Yuan and C. Yue and J. J. Zang and S. X. Zhang and W. Z. Zhang and Yan Zhang and Yi Zhang and Y. J. Zhang and Y. L. Zhang and Y. P. Zhang and Y. Q. Zhang and Z. Zhang and Z. Y. Zhang and C. Zhao and H. Y. Zhao and X. F. Zhao and C. Y. Zhou and Y. Zhu}, doi = {10.1103/PhysRevLett.134.191001}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {191001}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of a spectral hardening in cosmic ray boron spectrum with the DAMPE space mission}, volume = {134}, year = {2025}, }
• (2025). Quantum-enhanced beam tracking surpassing the heisenberg uncertainty limit. PRL, 134(19), 190804. (www)

  @article{ , abstract = {Determining a beam’s full trajectory requires tracking both its position and momentum (angular) information. However, the product of position and momentum uncertainty in a simultaneous measurement of the two parameters is bound by the Heisenberg uncertainty limit (HUL). In this work, we present a proof-of-principle demonstration of a quantum-enhanced beam tracking technique, leveraging the inherent position and momentum entanglement between photons produced via spontaneous parametric down-conversion (SPDC). We show that quantum entanglement can be exploited to achieve a beam tracking accuracy beyond the HUL in a simultaneous measurement. Moreover, with existing detection technologies, it is already possible to achieve near real-time beam tracking capabilities at the single-photon level. The technique also exhibits high resilience to background influences, with negligible reduction in tracking accuracy even when subjected to a disruptive beam that is significantly brighter than SPDC.}, archive = {J_PRL}, author = {Yingwen Zhang and Duncan England and Noah Lupu-Gladstein and Frédéric Bouchard and Guillaume Thekkadath and Philip J. Bustard and Ebrahim Karimi and Benjamin Sussman}, doi = {10.1103/PhysRevLett.134.190804}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190804}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-enhanced beam tracking surpassing the heisenberg uncertainty limit}, volume = {134}, year = {2025}, }
• (2025). No-go theorems for universal entanglement purification. PRL, 134(19), 190803. (www)

  @article{ , abstract = {An entanglement purification protocol (EPP) aims to transform multiple noisy entangled states into a single entangled state with higher fidelity. In this work we consider input-independent EPPs that always yield an output fidelity no worse than each of the original noisy states, a property we call universality . We prove there is no -to-1 EPP implementable by local operations and classical communication that is universal for all two-qubit entangled states, whereas such an EPP is possible using more general positive partial transpose-preserving (PPT) operations. We also show that universality is impossible by any bilocal Clifford EPP even when restricted to states with fidelities above an arbitrarily high threshold.}, archive = {J_PRL}, author = {Allen Zang and Xinan Chen and Eric Chitambar and Martin Suchara and Tian Zhong}, doi = {10.1103/PhysRevLett.134.190803}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190803}, shortjournal = {Phys. Rev. Lett.}, title = {No-go theorems for universal entanglement purification}, volume = {134}, year = {2025}, }
• (2025). Super-heisenberg scaling in a triple-point criticality. PRL, 134(19), 190802. (www)

  @article{ , abstract = {We investigate quantum-enhanced metrology in a triple point criticality and discover that quantum criticality does not always enhance measurement precision. We have developed suitable adiabatic evolution protocols to effectively restrain excitations, which could accelerate the adiabatic evolutions and lead to an exponential super-Heisenberg scaling. This scaling behavior is quite valuable in practical parameter estimating experiments with limited coherence time. Dissipation can strengthen the super-Heisenberg scaling until decoherence increases to dominate in the dissipative dynamics. Additionally, measurement precisions beyond Heisenberg scaling can be experimentally achieved in the trapped ion system. Our findings strongly indicate that criticality-enhanced metrology can indeed significantly enhance measurement precisions to a super-Heisenberg scaling when combining a triple point and beneficial parameter modulations, which will be conducive to the exploration of other super-Heisenberg scaling and their applications.}, archive = {J_PRL}, author = {Jia-Ming Cheng and Yong-Chang Zhang and Xiang-Fa Zhou and Zheng-Wei Zhou}, doi = {10.1103/PhysRevLett.134.190802}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190802}, shortjournal = {Phys. Rev. Lett.}, title = {Super-heisenberg scaling in a triple-point criticality}, volume = {134}, year = {2025}, }
• (2025). Generalized quantum repeater graph states. PRL, 134(19), 190801. (www)

  @article{ , abstract = {All-photonic quantum repeaters are essential for establishing long-range quantum entanglement. Within repeater nodes, reliably performing entanglement swapping is a key component of scalable quantum communication. To tackle the challenge of probabilistic Bell state measurement in linear optics, which often leads to information loss, various approaches have been proposed to ensure the loss tolerance of distributing a single ebit. We have generalized previous work regarding repeater graph states with elaborate connectivity, enabling the efficient establishment of exploitable ebits at a finite rate with high probability. We demonstrate that our new scheme significantly outperforms the previous work with much flexibility and discuss the generation overhead of such resource states. These findings offer new insights into the scalability and reliability of loss-tolerant quantum networks.}, archive = {J_PRL}, author = {Bikun Li and Kenneth Goodenough and Filip Rozpędek and Liang Jiang}, doi = {10.1103/PhysRevLett.134.190801}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190801}, shortjournal = {Phys. Rev. Lett.}, title = {Generalized quantum repeater graph states}, volume = {134}, year = {2025}, }
• (2025). Exact decoding of quantum error-correcting codes. PRL, 134(19), 190603. (www)

  @article{ , abstract = {We study the exact maximum-likelihood decoding of quantum error-correcting codes. Our primary focus is on the repetition code under circuit-level noise, which serves as a fundamental basis for quantum error correction experiments and is the only code that has achieved large distances and extremely low error rates. We uncover that the repetition code under circuit-level noise has an exact solution and propose an optimal maximum-likelihood decoding algorithm called “ planar .” This algorithm is based on the exact solution of the spin-glass partition function on planar graphs and has polynomial computational complexity. Through extensive numerical experiments, we demonstrate that our algorithm uncovers the exact threshold for depolarizing noise and realistic superconductor SI1000 noise. Furthermore, we apply our method to analyze data from recent quantum memory experiments conducted by Google Quantum AI, revealing that part of the error floor was attributed to the decoding algorithm used by Google. Finally, we implemented the repetition code quantum memory on superconducting systems using a 72-qubit quantum chip lacking reset gates, demonstrating that even with an unknown error model, the proposed algorithm achieves a significantly lower logical error rate than the matching-based algorithm. We also discuss the application of our approach to quantum codes whose maximum-likelihood decoding problem corresponds to a spin-glass problem, including the surface code under independent code-capacity noise.}, archive = {J_PRL}, author = {Hanyan Cao and Shoukuan Zhao and Dongyang Feng and Zisong Shen and Haisheng Yan and Tang Su and Weijie Sun and Huikai Xu and Feng Pan and Haifeng Yu and Pan Zhang}, doi = {10.1103/PhysRevLett.134.190603}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190603}, shortjournal = {Phys. Rev. Lett.}, title = {Exact decoding of quantum error-correcting codes}, volume = {134}, year = {2025}, }
• (2025). Stabilizer tensor networks with magic state injection. PRL, 134(19), 190602. (www)

  @article{ , abstract = {This Letter augments the recently introduced stabilizer tensor network (STN) protocol with magic state injection, reporting a new framework with significantly enhanced ability to simulate circuits with an extensive number of non-Clifford operations. Specifically, for random -doped -qubit Clifford circuits the computational cost of circuits prepared with magic state injection scales as when the circuit has gates compared to an exponential scaling for the STN approach, which is demonstrated in systems of up to 200 qubits. In the case of the hidden bit shift circuit, a paradigmatic benchmarking system for extended stabilizer methods with a tunable amount of magic, we report that our magic state injected STN framework can efficiently simulate 4000 qubits and gates. These findings provide a promising outlook for the use of this protocol in the classical modeling of quantum circuits that are conventionally difficult to simulate efficiently.}, archive = {J_PRL}, author = {Azar C. Nakhl and Ben Harper and Maxwell West and Neil Dowling and Martin Sevior and Thomas Quella and Muhammad Usman}, doi = {10.1103/PhysRevLett.134.190602}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190602}, shortjournal = {Phys. Rev. Lett.}, title = {Stabilizer tensor networks with magic state injection}, volume = {134}, year = {2025}, }
• (2025). Universal quantum computer from relativistic motion. PRL, 134(19), 190601. (www)

  @article{ , abstract = {We present an explicit construction of a relativistic quantum computing architecture using a variational quantum circuit approach that is shown to allow for universal quantum computing. The variational quantum circuit consists of tunable single-qubit rotations and entangling gates that are implemented successively. The single-qubit rotations are parameterized by the proper time intervals of the qubits’ trajectories and can be tuned by varying their relativistic motion in spacetime. The entangling layer is mediated by a relativistic quantum field instead of through direct coupling between the qubits. Within this setting, we give a prescription for how to use quantum field-mediated entanglement and manipulation of the relativistic motion of qubits to obtain a universal gate set, for which compact nonperturbative expressions that are valid for general spacetimes are also obtained. We also derive a lower bound on the channel fidelity that shows the existence of parameter regimes in which all entangling operations are effectively unitary, despite the noise generated from the presence of a mediating quantum field. Finally, we consider an explicit implementation of the quantum Fourier transform with relativistic qubits.}, archive = {J_PRL}, author = {Philip A. LeMaitre and T. Rick Perche and Marius Krumm and Hans J. Briegel}, doi = {10.1103/PhysRevLett.134.190601}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190601}, shortjournal = {Phys. Rev. Lett.}, title = {Universal quantum computer from relativistic motion}, volume = {134}, year = {2025}, }
• (2025). Provably efficient simulation of 1D long-range interacting systems at any temperature. PRL, 134(19), 190404. (www)

  @article{ , abstract = {We introduce a method that ensures efficient computation of one-dimensional quantum systems with long-range interactions across all temperatures. Our algorithm operates within a quasipolynomial run-time for inverse temperatures up to . At the core of our approach is the density matrix renormalization group algorithm, which typically does not guarantee efficiency. We have created a new truncation scheme for the matrix product operator of the quantum Gibbs states, which allows us to control the error analytically. Additionally, our method can be applied to simulate the time evolution of systems with long-range interactions, achieving significantly better precision than that offered by the Lieb-Robinson bound.}, archive = {J_PRL}, author = {Rakesh Achutha and Donghoon Kim and Yusuke Kimura and Tomotaka Kuwahara}, doi = {10.1103/PhysRevLett.134.190404}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190404}, shortjournal = {Phys. Rev. Lett.}, title = {Provably efficient simulation of 1D long-range interacting systems at any temperature}, volume = {134}, year = {2025}, }
• (2025). Dissecting quantum many-body chaos in the krylov space. PRL, 134(19), 190403. (www)

  @article{ , abstract = {The growth of simple operators is essential for the emergence of chaotic dynamics and quantum thermalization. Recent studies have proposed different measures, including the out-of-time-order correlator and Krylov complexity. It is established that the out-of-time-order correlator serves as the signature of quantum many-body chaos, while the Krylov complexity provides its upper bound. However, there exist nonchaotic systems in which Krylov complexity grows exponentially, indicating that the Krylov complexity itself is not a witness of many-body chaos. In this Letter, we introduce the missing ingredient called the Krylov metric , which probes the size of the Krylov basis. We propose that the universal criteria for fast scramblers include (i) the exponential growth of Krylov complexity, (ii) the diagonal elements with , and (iii) the negligibility of off-diagonal elements with . We further show that is a ratio between the quantum Lyapunov exponent and the Krylov exponent . This proposal is supported by both generic arguments and explicit examples, including solvable Sachdev-Ye-Kitaev models, Luttinger liquids, and many-body localized systems. Our results provide a refined understanding of how chaotic dynamics emerge from the Krylov space perspective.}, archive = {J_PRL}, author = {Liangyu Chen and Baoyuan Mu and Huajia Wang and Pengfei Zhang}, doi = {10.1103/PhysRevLett.134.190403}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190403}, shortjournal = {Phys. Rev. Lett.}, title = {Dissecting quantum many-body chaos in the krylov space}, volume = {134}, year = {2025}, }
• (2025). How pure can we go with adiabatic state manipulation?. PRL, 134(19), 190402. (www)

  @article{ , abstract = {Dissipative systems with decoherence-free subspaces, also known as dark spaces (DSs), can be used to protect quantum information. At the same time, dissipation is expected to give rise to coherent information degradation outside the DS. Employed to support quantum information platforms, DSs can be adiabatically modified in a way that resembles adiabatic control of coherent systems. Here we study the slow evolution of a purely dissipative system with a spectral gap , characterized by a strong symmetry, under a cyclic protocol with period . Nonadiabatic corrections to the state evolution give rise to decoherence: the evolution within the instantaneous DS is described by a time-local effective Liouvillian operator that leads to purity degradation over a period, of order . We obtain a closed form of the latter to order . Our analysis underlines fundamental limitations of coherent quantum information processing in the absence of corrective measures.}, archive = {J_PRL}, author = {Raul A. Santos and Alex Kamenev and Yuval Gefen}, doi = {10.1103/PhysRevLett.134.190402}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190402}, shortjournal = {Phys. Rev. Lett.}, title = {How pure can we go with adiabatic state manipulation?}, volume = {134}, year = {2025}, }
• (2025). Universal characterization of quantum many-body states through local information. PRL, 134(19), 190401. (www)

  @article{ , abstract = {We propose a universal framework for classifying quantum states based on their scale-resolved correlation structure. Using the recently introduced information lattice, which provides an operational definition of the total amount of correlations at each scale, we define intrinsic characteristic length scales of quantum states. We analyze ground and midspectrum eigenstates of the disordered interacting Kitaev chain, showing that our framework provides a novel unbiased approach to quantum matter.}, archive = {J_PRL}, author = {Claudia Artiaco and Thomas Klein Kvorning and David Aceituno Chávez and Loïc Herviou and Jens H. Bardarson}, doi = {10.1103/PhysRevLett.134.190401}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal characterization of quantum many-body states through local information}, volume = {134}, year = {2025}, }
• (2025). Self-testing composite measurements and bound entangled state in a single quantum network. PRL, 134(19), 190203. (www)

  @article{ , abstract = {Within the quantum networks scenario we introduce a single scheme allowing one to certify three different types of composite projective measurements acting on a three-qubit Hilbert space: one constructed from genuinely entangled GHZ-like states, one constructed from fully product vectors that exhibit the phenomenon of nonlocality without entanglement, and a hybrid measurement obtained from an unextendible product basis. Noticeably, we certify a basis exhibiting nonlocality without entanglement in the smallest dimension capable of supporting this phenomenon. On the other hand, the possibility of certification of a measurement obtained from an unextendible product basis has an interesting implication that one can also self-test a bound entangled state in the considered quantum network. Such a possibility does not seem to exist in the standard Bell scenario. Furthermore, we also analyze the robustness of our scheme toward experimental errors.}, archive = {J_PRL}, author = {Shubhayan Sarkar and Chandan Datta and Saronath Halder and Remigiusz Augusiak}, doi = {10.1103/PhysRevLett.134.190203}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190203}, shortjournal = {Phys. Rev. Lett.}, title = {Self-testing composite measurements and bound entangled state in a single quantum network}, volume = {134}, year = {2025}, }
• (2025). Computable and faithful lower bound on entanglement cost. PRL, 134(19), 190202. (www)

  @article{ , abstract = {Quantifying the minimum entanglement needed to prepare quantum states and implement quantum processes is a key challenge in quantum information theory. In this Letter, we develop computable and faithful lower bounds on the entanglement cost under quantum operations that completely preserve the positivity of partial transpose (PPT operations), by introducing the generalized divergence of -negativity, a generalization of logarithmic negativity. Our bounds are efficiently computable via semidefinite programming and provide nontrivial values for all states that are non-PPT (NPT), establishing their faithfulness for the resource theory of NPT entanglement. Notably, we find and affirm the irreversibility of asymptotic entanglement manipulation under PPT operations for full-rank entangled states. Furthermore, we extend our methodology to derive lower bounds on the entanglement cost of both point-to-point and bipartite quantum channels. Our bound demonstrates improvements over previously known computable bounds for a wide range of quantum states and channels. These findings push the boundaries of understanding the structure of entanglement and the fundamental limits of entanglement manipulation.}, archive = {J_PRL}, author = {Xin Wang and Mingrui Jing and Chengkai Zhu}, doi = {10.1103/PhysRevLett.134.190202}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190202}, shortjournal = {Phys. Rev. Lett.}, title = {Computable and faithful lower bound on entanglement cost}, volume = {134}, year = {2025}, }
• (2025). Tsirelson’s inequality for the precession protocol is maximally violated by quantum theory. PRL, 134(19), 190201. (www)

  @article{ , abstract = {The precession protocol involves measuring , the probability that a uniformly precessing observable (like the position of a harmonic oscillator or a coordinate undergoing spatial rotation) is positive at one of three equally spaced times. Tsirelson’s inequality, which states that in classical theory, is violated in quantum theory by certain states. In this Letter, we address some open questions about the inequality: What is the maximum violation of Tsirelson’s inequality possible in quantum theory? Might other theories do better? By considering the precession protocol in a theory-independent manner for systems with finitely many outcomes, we derive a general bound for the maximum possible violation. This theory-independent bound must be satisfied by any theory whose expectation values are linear functions of observables—which includes classical, quantum, and all general probabilistic theories—and depends only on the minimum positive and negative measurement outcomes. Given any such two values, we prove by construction that quantum theory always saturates this bound. Some notable examples include the angular momentum of a spin- particle and a family of observables that outperform the quantum harmonic oscillator in the precession protocol. Finally, we also relate our findings to the recently introduced notion of constrained conditional probabilities.}, archive = {J_PRL}, author = {Lin Htoo Zaw and Mirjam Weilenmann and Valerio Scarani}, doi = {10.1103/PhysRevLett.134.190201}, journal = {Physical Review Letters}, month = {5}, number = {19}, pages = {190201}, shortjournal = {Phys. Rev. Lett.}, title = {Tsirelson’s inequality for the precession protocol is maximally violated by quantum theory}, volume = {134}, year = {2025}, }
• (2025). Erratum: Boundary critical behavior of the three-dimensional heisenberg universality class [Phys. rev. lett. 126, 135701 (2021)]. PRL, 134(18), 189901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 189901 (2025)}, archive = {J_PRL}, author = {Francesco Parisen Toldin}, doi = {10.1103/PhysRevLett.134.189901}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {189901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Boundary critical behavior of the three-dimensional heisenberg universality class [Phys. rev. lett. 126, 135701 (2021)]}, volume = {134}, year = {2025}, }
• (2025). Universal law for the dispersal of motile microorganisms in porous media. PRL, 134(18), 188303. (www)

  @article{ , abstract = {Dispersal is essential to the plethora of motile microorganisms living in porous environments, yet how it relates to movement patterns and pore space structure remains largely unknown. Here we investigate numerically the long-time dispersal of a run-and-tumble microorganism that remains trapped at solid surfaces and escapes from them by tumbling. We find that dispersal and mean run time are connected by a universal relation, that applies for a variety of porous microstructures and swimming strategies. We explain how this generic dependence originates in the invariance of the mean free path with respect to the movement pattern, and we discuss the optimal strategy that maximizes dispersal. Finally, we extend our approach to microorganisms moving along the surface. Our results provide a general framework to quantify dispersal that works across the vast diversity of movement patterns and porous media.}, archive = {J_PRL}, author = {T. Pietrangeli and R. Foffi and R. Stocker and C. Ybert and C. Cottin-Bizonne and F. Detcheverry}, doi = {10.1103/PhysRevLett.134.188303}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188303}, shortjournal = {Phys. Rev. Lett.}, title = {Universal law for the dispersal of motile microorganisms in porous media}, volume = {134}, year = {2025}, }
• (2025). Active-hydraulic flows solve the six-vertex model (and vice versa). PRL, 134(18), 188302. (www)

  @article{ , abstract = {By confining colloidal active fluids in microchannel networks, we demonstrate that their degenerate flows correspond to the configurations of the six-vertex model. We use this quantitative correspondence to control and explain the active flows that emerge in square-grid networks. In particular, we show that the Lagrangian trajectories of active particles realize the Baxter-Kelland-Wu mapping and form completely packed loops, whose geometry can be exactly predicted and explained. We then go beyond the square-grid geometry and introduce a general framework for predicting the geometry of active-hydraulic flows in arbitrary networks.}, archive = {J_PRL}, author = {Camille Jorge and Denis Bartolo}, doi = {10.1103/PhysRevLett.134.188302}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188302}, shortjournal = {Phys. Rev. Lett.}, title = {Active-hydraulic flows solve the six-vertex model (and vice versa)}, volume = {134}, year = {2025}, }
• (2025). Activity leads to topological phase transition in 2D populations of heterogeneous oscillators. PRL, 134(18), 188301. (www)

  @article{ , abstract = {Populations of heterogeneous, noisy oscillators on a two-dimensional lattice display short-range order. Here, we show that if the oscillators are allowed to actively move in space, the system undergoes instead a Berezenskii-Kosterlitz-Thouless transition and exhibits quasi-long-range order. This fundamental result connects two paradigmatic models—the XY and Kuramoto models—and provides insight into the emergence of order in active systems.}, archive = {J_PRL}, author = {Ylann Rouzaire and Parisa Rahmani and Ignacio Pagonabarraga and Fernando Peruani and Demian Levis}, doi = {10.1103/PhysRevLett.134.188301}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188301}, shortjournal = {Phys. Rev. Lett.}, title = {Activity leads to topological phase transition in 2D populations of heterogeneous oscillators}, volume = {134}, year = {2025}, }
• (2025). Soft condensation. PRL, 134(18), 188204. (www)

  @article{ , abstract = {When moist air meets a cold surface, it creates a breath figure characterized by numerous small droplets. The central question is how the vapor flux is distributed between the growth of condensed drops and the nucleation of new ones. Here, we investigate the nucleation, growth, and coalescence of droplets on soft substrates consisting of cross-linked polymer networks. The number of droplets initially remains constant, until drops start to coarsen according to a universal law; both phenomena are explained via the formation of a saturated boundary layer. We quantitatively unveil an algebraic sensitivity of the number of droplets on substrate elasticity, which is unexpected since nucleation occurs at a scale where the polymer network resembles a melt. Breath figures thus offer a macroscopic probe of the molecular characteristics of the polymer surface, and suggest a surprisingly low-energy pathway for nucleation.}, archive = {J_PRL}, author = {Ambre Bouillant and Christopher Henkel and Uwe Thiele and Bruno Andreotti and Jacco H. Snoeijer}, doi = {10.1103/PhysRevLett.134.188204}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188204}, shortjournal = {Phys. Rev. Lett.}, title = {Soft condensation}, volume = {134}, year = {2025}, }
• (2025). Formation of topological bigels in mixtures of colloidal rings and polymers. PRL, 134(18), 188203. (www)

  @article{ , abstract = {We study a spherically confined mixture of polymers and colloidal rings. Unlike in standard colloid-polymer mixtures, the polymers interact topologically with the rings by threading them. We find that, above a critical value of the ring radius, threading yields a topological transition from a fluid to a gel-like phase characterized by a space-spanning network of interlocked polymers and rings, which we refer to as a bicomponent gel, or bigel. By exploiting the mixture dual character (rings and polymers), we predict analytically the value of the critical radius. We also show that the mobility of entanglements in the mixture slows down upon entering the gel phase, due to topological hindrance arising from threadings, while the transition rates between topological states of the colloidal probes provide another strong dynamical signature of the gel phase.}, archive = {J_PRL}, author = {Andrea Bonato and Davide Marenduzzo and Enzo Orlandini}, doi = {10.1103/PhysRevLett.134.188203}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188203}, shortjournal = {Phys. Rev. Lett.}, title = {Formation of topological bigels in mixtures of colloidal rings and polymers}, volume = {134}, year = {2025}, }
• (2025). Shape of a membrane on a liquid interface with arbitrary curvatures. PRL, 134(18), 188202. (www)

  @article{ , abstract = {We study the deformation of a liquid interface with arbitrary principal curvatures by a flat circular sheet. Working first at small slopes, we determine the shape of the sheet analytically in the membrane limit, where the sheet is inextensible yet free to bend and compress. We find that the sheet takes a cylindrical shape on interfaces with negative Gaussian curvature. On interfaces with positive Gaussian curvature, an inner region still adopts a cylindrical shape while the outer region is under azimuthal compression. Numerical energy minimization confirms our predictions and shows that this behavior holds for finite slopes. Experiments on a thin polystyrene film at an anisotropic air-water interface show consistent behaviors.}, archive = {J_PRL}, author = {Zachariah S. Schrecengost and Seif Hejazine and Jordan V. Barrett and Vincent Démery and Joseph D. Paulsen}, doi = {10.1103/PhysRevLett.134.188202}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188202}, shortjournal = {Phys. Rev. Lett.}, title = {Shape of a membrane on a liquid interface with arbitrary curvatures}, volume = {134}, year = {2025}, }
• (2025). Geometric control and memory in networks of hysteretic elements. PRL, 134(18), 188201. (www)

  @article{ , abstract = {The response of driven frustrated media stems from interacting hysteretic elements. We derive explicit mappings from networks of hysteretic springs to their abstract representation as interacting hysterons. These mappings reveal how the physical network controls the signs, magnitudes, symmetries, and pairwise nature of the hysteron interactions. In addition, strong geometric nonlinearities can produce pathways that require excess hysterons or even break hysteron models. Our results pave the way for metamaterials with geometrically controlled interactions, pathways, and functionalities, and highlight fundamental limitations of abstract hysterons in modeling disordered systems.}, archive = {J_PRL}, author = {Dor Shohat and Martin van Hecke}, doi = {10.1103/PhysRevLett.134.188201}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188201}, shortjournal = {Phys. Rev. Lett.}, title = {Geometric control and memory in networks of hysteretic elements}, volume = {134}, year = {2025}, }
• (2025). Controlling molecular dynamics by exciting atoms in a cavity. PRL, 134(18), 188001. (www)

  @article{ , abstract = {Placing an atom and a molecule in a cavity opens the door to initialize molecular dynamics by exciting a level of the atom. This approach enlarges the range of choosing the light source to trigger molecular dynamics substantially. The interplay of the atomic, molecular, and photonic populations gives rise to rich dynamics. The cavity photon plays the role of a mediator between the atom and the molecule and it is found that the photonic population is rather low throughout and its evolution follows that of the molecule. Cavities are known to be subject to losses. In spite of the losses it is demonstrated that the presence of the atom gives rise to a long-lived dynamics that should be of relevance for experimental investigations. The presence of more atoms and molecules is expected to further enrich the dynamics.}, archive = {J_PRL}, author = {András Csehi and Krisztián Szabó and Ágnes Vibók and Lorenz S. Cederbaum and Gábor J. Halász}, doi = {10.1103/PhysRevLett.134.188001}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {188001}, shortjournal = {Phys. Rev. Lett.}, title = {Controlling molecular dynamics by exciting atoms in a cavity}, volume = {134}, year = {2025}, }
• (2025). Dynamics of critical cascades in interdependent networks. PRL, 134(18), 187401. (www)

  @article{ , abstract = {The failure of interdependent networks, as well as similar avalanche phenomena, is driven by cascading failures. At the critical point, the cascade begins as a critical branching process, where each failing node (element) triggers, on average, the failure of one other node. As nodes continue to fail, the network becomes increasingly fragile, and the branching factor grows. If the failure process does not reach extinction during its critical phase, the network undergoes an abrupt collapse. Here, we implement the analogy between this dynamic and birth-death processes to derive new analytical results and significantly optimize numerical calculations. Using this approach, we analyze three key aspects of the dynamics: the probability of collapse, the duration of avalanches, and the length of the cascading plateau phase preceding a collapse. This analysis quantifies how the system size and the intensity of the initial triggering event influence these characteristics.}, archive = {J_PRL}, author = {Dolev Dilmoney and Bnaya Gross and Shlomo Havlin and Nadav M. Shnerb}, doi = {10.1103/PhysRevLett.134.187401}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {187401}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamics of critical cascades in interdependent networks}, volume = {134}, year = {2025}, }
• (2025). Fractals in the critical attractor of the classical sandpile model. PRL, 134(18), 187201. (www)

  @article{ , abstract = {The classical sandpile model for self-organized criticality is analyzed with deterministic perturbations. This allows us to explore underlying long-range correlations in the critical attractor and quantify these as the fractal dimension of excitable sites and the fractal dimension of avalanche termination sites. The fractal of highly excitable sites, characterized by a dimension of 1.3, is associated with the avalanches responsible for most of the relaxations in the system. Furthermore, the fractal dimension of these highly excitable sites suggests a scaling exponent for avalanche sizes of 1.26, consistent with earlier literature.}, archive = {J_PRL}, author = {Marcus Engsig and Kim Sneppen}, doi = {10.1103/PhysRevLett.134.187201}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {187201}, shortjournal = {Phys. Rev. Lett.}, title = {Fractals in the critical attractor of the classical sandpile model}, volume = {134}, year = {2025}, }
• (2025). Diffusive hydrodynamics from long-range correlations. PRL, 134(18), 187101. (www)

  @article{ , abstract = {In the hydrodynamic theory, the nonequilibrium dynamics of a many-body system is approximated, at large scales of space and time, by irreversible relaxation to local entropy maximization. This results in a convective equation corrected by viscous or diffusive terms in a gradient expansion, such as the Navier-Stokes equations. Diffusive terms are evaluated using the Kubo formula, and possibly arising from an emergent noise due to discarded microscopic degrees of freedom. In one dimension of space, diffusive scaling is often broken as noise leads to superdiffusion. But in linearly degenerate hydrodynamics, such as that of integrable models, diffusive behaviors are observed, and it has long been thought that the standard diffusive picture remains valid. In this Letter, we show that in such systems, the Navier-Stokes equation breaks down beyond linear response. We demonstrate that diffusive-order corrections do not take the form of a gradient expansion. Instead, they are completely determined by ballistic transport of initial-state fluctuations, and obtained from the nonlocal two-point correlations recently predicted by the ballistic macroscopic fluctuation theory; the resulting hydrodynamic equations are reversible. To do so, we establish a regularized fluctuation theory, putting on a firm basis the recent idea that ballistic transport of initial-state fluctuations determines fluctuations and correlations beyond the Euler scale. This extends the idea of “diffusion from convection” previously developed to explain the Kubo formula in integrable systems to generic nonequilibrium settings.}, archive = {J_PRL}, author = {Friedrich Hübner and Leonardo Biagetti and Jacopo De Nardis and Benjamin Doyon}, doi = {10.1103/PhysRevLett.134.187101}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {187101}, shortjournal = {Phys. Rev. Lett.}, title = {Diffusive hydrodynamics from long-range correlations}, volume = {134}, year = {2025}, }
• (2025). Mass-singularity-induced phase jump in high-harmonic generation from symmetry-breaking crystals. PRL, 134(18), 186901. (www)

  @article{ , abstract = {Symmetry plays a central role in fundamental physics. Here we identify a phase-jump phenomenon in high-order harmonic generation in symmetry-breaking crystals. This phenomenon originates from the singularity in the effective mass of electron-hole pairs at nonzero-distance collisions, a factor usually ignored in the literature. However, it determines the basic properties of harmonic emissions. This phase-jump phenomenon results in a suppression of the harmonic spectrum by orders, which is strongly orientation dependent. It is universal and not limited to a specific crystal. Clues to this can be found in published ab initio simulations and experimental results, but not interpreted. Our findings pave the way for a better understanding of the ultrafast dynamics of electron-hole pairs in XUV photon emission.}, archive = {J_PRL}, author = {Jia-Xiang Chen and Xue-Bin Bian}, doi = {10.1103/PhysRevLett.134.186901}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186901}, shortjournal = {Phys. Rev. Lett.}, title = {Mass-singularity-induced phase jump in high-harmonic generation from symmetry-breaking crystals}, volume = {134}, year = {2025}, }
• (2025). Non-abelian gauge theory for magnons in topologically textured frustrated magnets. PRL, 134(18), 186701. (www)

  @article{ , abstract = {We develop an effective gauge theory for three-flavored magnons in frustrated magnets hosting topological textures with the aid of the quaternion representation of the SO(3) order parameter. We find that the effect of topological solitons on magnons is captured generally by the non-Abelian emergent electromagnetic fields, distinct from the previously established gauge theory for magnons in collinear magnets where the gauge theory is often restricted to be Abelian. As concrete examples, vortices in two- and three-dimensional magnets and Shankar skyrmions in three-dimensional magnets are discussed in detail, which are shown to induce, respectively, the Abelian and the non-Abelian topological magnetic field on magnons, and thereby engender the topological Hall transport in textured frustrated magnets. We also discuss the effect of magnon-magnon interactions on our effective theory. Our work is applicable to a broad class of magnetic materials whose low-energy manifold is described by the SO(3) order parameter. We envision that the discovery of the non-Abelian magnonic gauge theory will enrich the field of magnonics as well as prompt the study of magnon transport in textured frustrated magnets.}, archive = {J_PRL}, author = {Ricardo Zarzuela and Se Kwon Kim}, doi = {10.1103/PhysRevLett.134.186701}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186701}, shortjournal = {Phys. Rev. Lett.}, title = {Non-abelian gauge theory for magnons in topologically textured frustrated magnets}, volume = {134}, year = {2025}, }
• (2025). Tensor-monopole-induced topological boundary effects in four-dimensional acoustic metamaterials. PRL, 134(18), 186601. (www)

  @article{ , abstract = {Gauge field theory provides the mathematical and conceptual framework to describe and understand topological singularities such as Weyl points and magnetic monopoles. While singularities associated with vector electromagnetic gauge fields have been well studied, those of higher-form tensor gauge fields, like the four-dimensional (4D) tensor monopoles predicted by string theory, have remained largely theoretical or limited to experimental demonstration in pure synthetic dimensions, thereby not allowing investigations of the associated boundary effects. Here, we present a 4D system with tensor monopoles using engineered acoustic metamaterials. Our momentum space combines three real momentum dimensions and a geometric parameter as the fourth. By varying this fourth momentum, we experimentally reveal two distinct topological surface states in 3D subsystems: Fermi-arc surface states in a gapless subsystem and Dirac-cone surface states in a gapped subsystem. Our work introduces a novel platform for exploring new topological structures associated with tensor gauge field and topological phenomena in higher dimensions.}, archive = {J_PRL}, author = {Qingyang Mo and Shanjun Liang and Cuicui Lu and Jie Zhu and Shuang Zhang}, doi = {10.1103/PhysRevLett.134.186601}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186601}, shortjournal = {Phys. Rev. Lett.}, title = {Tensor-monopole-induced topological boundary effects in four-dimensional acoustic metamaterials}, volume = {134}, year = {2025}, }
• (2025). Anomalous electrical transport in the kagome magnet YbFe6Ge6. PRL, 134(18), 186501. (www)

  @article{ , abstract = {Two-dimensional (2D) kagome metals offer a unique platform for exploring electron correlation phenomena derived from quantum many-body effects. Here, we report a combined study of electrical magnetotransport and neutron scattering on , where the Fe moments in the 2D kagome layers exhibit an -type collinear antiferromagnetic order below . Interactions between the Fe ions in the layers and the localized Yb magnetic ions in between reorient the -axis-aligned Fe moments to the kagome plane below . Our magnetotransport measurements show an intriguing anomalous Hall effect (AHE) that emerges in the spin-reorientated collinear state, accompanied by the closing of the spin anisotropy gap as revealed from inelastic neutron scattering. The gapless spin excitations and the Yb-Fe interaction are able to support a dynamic scalar spin chirality, which explains the observed AHE. Therefore, our Letter demonstrates that spin fluctuations may provide an additional scattering channel for the conduction electrons and give rise to AHE even in a collinear antiferromagnet.}, archive = {J_PRL}, author = {Weiliang Yao and Supeng Liu and Hodaka Kikuchi and Hajime Ishikawa and Øystein S. Fjellvåg and David W. Tam and Feng Ye and Douglas L. Abernathy and George D. A. Wood and Devashibhai Adroja and Chun-Ming Wu and Chien-Lung Huang and Bin Gao and Yaofeng Xie and Yuxiang Gao and Karthik Rao and Emilia Morosan and Koichi Kindo and Takatsugu Masuda and Kenichiro Hashimoto and Takasada Shibauchi and Pengcheng Dai}, doi = {10.1103/PhysRevLett.134.186501}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186501}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous electrical transport in the kagome magnet YbFe6Ge6}, volume = {134}, year = {2025}, }
• (2025). Nonperturbative self-consistent electron-phonon spectral functions and transport. PRL, 134(18), 186401. (www)

  @article{ , abstract = {Electron-phonon coupling often dominates the electron spectral functions and carrier transport properties. However, studies of this effect in real materials have largely relied on perturbative one-shot methods due to the lack of a first-principles theoretical and computational framework. Here, we present a self-consistent theory and implementation for the nonperturbative calculations of spectral functions and conductivity due to electron-phonon coupling. Applying this method to monolayer InSe, we demonstrate that self-consistency qualitatively affects the spectral function and transport properties compared to state-of-the-art one-shot calculations and allow one to reconcile calculations with angle-resolved photoemission experiments. The developed method can be widely applied to materials with dominant electron-phonon coupling at moderate computational cost.}, archive = {J_PRL}, author = {Jae-Mo Lihm and Samuel Poncé}, doi = {10.1103/PhysRevLett.134.186401}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186401}, shortjournal = {Phys. Rev. Lett.}, title = {Nonperturbative self-consistent electron-phonon spectral functions and transport}, volume = {134}, year = {2025}, }
• (2025). Interfacial heat transport via evanescent radiation by hot electrons. PRL, 134(18), 186302. (www)

  @article{ , abstract = {We predict an additional thermal transport pathway across metal-nonmetal interfaces with large electron-phonon nonequilibrium via evanescent radiative heat transfer. In such systems, electron scattering processes vary drastically and can be leveraged to guide heat across interfaces via radiative heat transport without engaging the lattice directly. We employ the formalism of fluctuational electrodynamics to simulate the spectral radiative heat flux across the interface of a metal film and a nonmetal substrate. We find that the radiative conductance can exceed 300 MW m − 2 K − 1 at an electron temperature of 5000 K for an emitting tungsten film on a hexagonal boron nitride substrate, becoming comparable to its conductive counterpart. This allows for a more holistic approach to the heat flow across interfaces, accounting for electron-phonon nonequilibrium and ultrafast near-field phonon-polariton coupling.}, archive = {J_PRL}, author = {William D. Hutchins and Saman Zare and Mehran Habibzadeh and Sheila Edalatpour and Patrick E. Hopkins}, doi = {10.1103/PhysRevLett.134.186302}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186302}, shortjournal = {Phys. Rev. Lett.}, title = {Interfacial heat transport via evanescent radiation by hot electrons}, volume = {134}, year = {2025}, }
• (2025). Scattering theory of thermal and bipolar thermoelectric diodes. PRL, 134(18), 186301. (www)

  @article{ , abstract = {We investigate the minimal requirements that induce a nonreciprocal response to temperature differences in a mesoscopic electronic conductor. We identify two distinct mechanisms involved in electron-electron interactions, namely inelastic scattering and screening, that locally affect the internal properties of the device, leading to thermal and thermoelectric rectification effects in the absence of inversion symmetry. We propose resonant tunneling samples to efficiently exploit these effects, and find configurations acting as bipolar thermoelectric diodes whose current flows in the same direction irrespective of the sign of the temperature difference, a case of antireciprocity.}, archive = {J_PRL}, author = {José Balduque and Rafael Sánchez}, doi = {10.1103/PhysRevLett.134.186301}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186301}, shortjournal = {Phys. Rev. Lett.}, title = {Scattering theory of thermal and bipolar thermoelectric diodes}, volume = {134}, year = {2025}, }
• (2025). Transitional supersolidity in ion doped helium droplets. PRL, 134(18), 186001. (www)

  @article{ , abstract = {nanodroplets doped with an alkali ion feature a snowball of crystallized layers surrounded by superfluid helium. For large droplets, we predict that a transitional supersolid layer can form, bridging between the solid core and the liquid bulk, where the density displays modulations of icosahedral group symmetry. To identify the different phases, we combine density functional theory with the semiclassical Gaussian time-dependent Hartree method for localized many-body systems. This hybrid approach can handle large particle numbers and provides insight into the physical origin of the supersolid layer. For small droplets, we verify that the predictions of our approach are in excellent agreement with Path-Integral Monte Carlo calculations.}, archive = {J_PRL}, author = {Juan Carlos Acosta Matos and P. Giannakeas and Matteo Ciardi and Thomas Pohl and Jan M. Rost}, doi = {10.1103/PhysRevLett.134.186001}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {186001}, shortjournal = {Phys. Rev. Lett.}, title = {Transitional supersolidity in ion doped helium droplets}, volume = {134}, year = {2025}, }
• (2025). X-point target radiator regime in tokamak divertor plasmas. PRL, 134(18), 185102. (www)

  @article{ , abstract = {Fusion plasma regimes with a strongly radiating magnetic point are promising candidates to tackle the outstanding power exhaust challenge in reactor-scale devices. In this Letter, we report on a new type of -point radiator, the XPTR ( -point target radiator), produced by a secondary point placed well away from the confined plasma. This XPTR features strongly facilitated detachment access and significantly reduced sensitivity of the radiative front position near the secondary point. Consistent with a reduced analytical model, the physical origin of -point radiation is rooted in its magnetic geometry, irrespective of whether the field lines are closed or open. The results presented open up a class of novel power exhaust concepts where radiative edge cooling can be robustly avoided during divertor detachment.}, archive = {J_PRL}, author = {the TCV Team and the EUROfusion Tokamak Exploitation Team and K. Lee and C. Theiler and M. Carpita and O. Février and A. Perek and M. Zurita and D. Brida and R. Ducker and G. Durr-Legoupil-Nicoud and B. P. Duval and S. Gorno and D. Hamm and D. S. Oliveira and F. Pastore and M. Pedrini and H. Reimerdes and L. Simons and E. Tonello and K. Verhaegh and Y. Wang and C. Wüthrich}, doi = {10.1103/PhysRevLett.134.185102}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {185102}, shortjournal = {Phys. Rev. Lett.}, title = {X-point target radiator regime in tokamak divertor plasmas}, volume = {134}, year = {2025}, }
• (2025). Reduced model of ionization lag in intense laser-produced plasmas. PRL, 134(18), 185101. (www)

  @article{ , abstract = {A physics-based empirical formula is derived to predict the ionization lag in underdense plasmas generated by an intense laser. Time-dependent nonlocal thermodynamic equilibrium calculations demonstrate significantly delayed ionization, due to rapid changes in plasma conditions, which critically impacts plasma properties such as opacity, emissivity, and heat transport. The reduced model, based on these calculations, enables the estimation of ionization lag without requiring in-depth knowledge of nonlocal thermodynamic equilibrium modeling. Furthermore, modeling reveals that the two-step ionization process—collisional excitation followed by photoionization—plays a crucial role in this ionization delay, with collisional excitation setting the timescale for ionization. Simulations across a range of elements, from beryllium to germanium, demonstrate that ionization lag is a widespread phenomenon, underscoring the importance of incorporating such processes into ionization modeling in radiation hydrodynamic simulations for various laser-plasma experiments.}, archive = {J_PRL}, author = {M. S. Cho and A. L. Milder and W. Rozmus and H. P. Le and H. A. Scott and D. T. Bishel and D. Turnbull and S. B. Libby and M. E. Foord}, doi = {10.1103/PhysRevLett.134.185101}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {185101}, shortjournal = {Phys. Rev. Lett.}, title = {Reduced model of ionization lag in intense laser-produced plasmas}, volume = {134}, year = {2025}, }
• (2025). Nonmonotonic motion of sliding droplets on strained soft solids. PRL, 134(18), 184001. (www)

  @article{ , abstract = {Soft materials are ubiquitous in technological applications that require deformability, for instance, in flexible, water-repellent coatings. However, the wetting properties of prestrained soft materials are only beginning to be explored. Here we study the sliding dynamics of droplets on prestrained soft silicone gels, both in tension and in compression. Intriguingly, in compression we find a nonmonotonic strain dependence of the sliding speed: mild compressions decelerate the droplets, but stronger compressions lead again to faster droplet motion. Upon further compression, creases nucleate under the droplets until, finally, the entire surface undergoes the creasing instability, causing a “run-and-stop” motion. We quantitatively elucidate the speed modification for moderate prestrains by incremental viscoelasticity, while the acceleration for larger prestrains turns out to be linked to the solid pressure, presumably through a lubrication effect of expelled oligomers.}, archive = {J_PRL}, author = {Youchuang Chao and Hansol Jeon and Stefan Karpitschka}, doi = {10.1103/PhysRevLett.134.184001}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {184001}, shortjournal = {Phys. Rev. Lett.}, title = {Nonmonotonic motion of sliding droplets on strained soft solids}, volume = {134}, year = {2025}, }
• (2025). Detecting and focusing on a nonlinear target in a complex medium. PRL, 134(18), 183802. (www)

  @article{ , abstract = {Wavefront shaping techniques allow waves to be focused on a diffraction-limited target deep inside disordered media. To identify the target position, a guidestar is required that typically emits a frequency-shifted signal. Here, we present a noninvasive matrix approach operating at a single frequency only, based on the variation of the field scattered by a nonlinear target illuminated at two different incident powers. The local perturbation induced by the nonlinearity serves as a guide for identifying optimal incident wavefronts. We demonstrate maximal focusing on electronic devices embedded in chaotic microwave cavities and extend our approach to temporal signals. Finally, we exploit the programmability offered by reconfigurable smart surfaces to enhance the intensity delivered to a nonlinear target. Our results pave the way for deep imaging protocols that use any type of nonlinearity as feedback, requiring only the measurement of a monochromatic scattering matrix.}, archive = {J_PRL}, author = {Antton Goïcoechea and Jakob Hüpfl and Stefan Rotter and François Sarrazin and Matthieu Davy}, doi = {10.1103/PhysRevLett.134.183802}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183802}, shortjournal = {Phys. Rev. Lett.}, title = {Detecting and focusing on a nonlinear target in a complex medium}, volume = {134}, year = {2025}, }
• (2025). Plasmonic time crystals. PRL, 134(18), 183801. (www)

  @article{ , abstract = {We study plasmonic time crystals, an extension of dielectric-based photonic time crystals to plasmonic media. We demonstrate that such systems may amplify both longitudinal and transverse modes. In particular, we show that plasmonic time crystals support “collective resonances” of longitudinal modes, which occur independent of the wave vector , even in the presence of significant dissipation. These resonances originate from the coupling between the positive- and negative-frequency branches of the plasmonic dispersion relation of the unmodulated system and from the divergence of the density of states near the plasma ( -near-zero) frequency . The strongest resonance arises at a modulation frequency , corresponding to a direct interband transition. We demonstrate these resonances for various periodic modulation profiles and provide a generic perturbative formula for resonance widths in the weak modulation limit. Furthermore, we propose transparent conducting oxides as promising platforms for realizing plasmonic time crystals, as they enable significant modulation of the electron effective mass while maintaining moderate dissipation levels. Our findings provide new insights into leveraging time-modulated plasmonic media to enhance optical gain and control wave dynamics at the nanoscale.}, archive = {J_PRL}, author = {Joshua Feinberg and David E. Fernandes and Boris Shapiro and Mário G. Silveirinha}, doi = {10.1103/PhysRevLett.134.183801}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183801}, shortjournal = {Phys. Rev. Lett.}, title = {Plasmonic time crystals}, volume = {134}, year = {2025}, }
• (2025). Cavity-enhanced solid-state nuclear spin gyroscope. PRL, 134(18), 183603. (www)

  @article{ , abstract = {Solid-state quantum sensors based on ensembles of nitrogen-vacancy (NV) centers in diamond have emerged as powerful tools for precise sensing applications. Nuclear spin sensors are particularly well suited for applications requiring long coherence times, such as inertial sensing, but remain underexplored due to control complexity and limited optical readout efficiency. In this work, we propose cooperative cavity quantum electrodynamic (cQED) coupling to achieve efficient nuclear spin readout. Unlike previous cQED methods used to enhance electron spin readout, here we employ two-field interference in the NV hyperfine subspace to directly probe the nuclear spin transitions. We model the nuclear spin NV-cQED system (nNV-cQED) and observe several distinct regimes, including electromagnetically induced transparency, masing without inversion, and oscillatory behavior. We then evaluate the nNV-cQED system as an inertial sensor, indicating a rotation sensitivity improved by 3 orders of magnitude compared to previous solid-state spin demonstrations. Furthermore, we show that the NV electron spin can be simultaneously used as a comagnetometer, and the four crystallographic axes of NVs can be employed for vector resolution in a single nNV-cQED system. These results showcase the applications of two-field interference using the nNV-cQED platform, providing critical insights into the manipulation and control of quantum states in hybrid NV systems and unlocking new possibilities for high-performance quantum sensing.}, archive = {J_PRL}, author = {Hanfeng Wang and Shuang Wu and Kurt Jacobs and Yuqin Duan and Dirk R. Englund and Matthew E. Trusheim}, doi = {10.1103/PhysRevLett.134.183603}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183603}, shortjournal = {Phys. Rev. Lett.}, title = {Cavity-enhanced solid-state nuclear spin gyroscope}, volume = {134}, year = {2025}, }
• (2025). Continuous-variable square-ladder cluster states in a microwave frequency comb. PRL, 134(18), 183602. (www)

  @article{ , abstract = {We describe an experiment demonstrating the generation of three independent square-ladder continuous-variable cluster states with up to 94 qumodes of a microwave frequency comb. This entanglement structure at a large scale is realized by injecting vacuum fluctuations into a Josephson Parametric Amplifier pumped by three coherent signals around twice its resonance frequency, each having a particular well-defined phase relation. We reach up to 1.4 dB of squeezing of the nullifier that verifies the cluster state on the square ladder graph. Our results are consistent with a more familiar measure of two-mode squeezing, where we find up to 5.42 dB for one pump, and up to 1 dB for three pumps.}, archive = {J_PRL}, author = {Fabio Lingua and J. C. Rivera Hernández and Michele Cortinovis and David B. Haviland}, doi = {10.1103/PhysRevLett.134.183602}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183602}, shortjournal = {Phys. Rev. Lett.}, title = {Continuous-variable square-ladder cluster states in a microwave frequency comb}, volume = {134}, year = {2025}, }
• (2025). Universal photon blockade. PRL, 134(18), 183601. (www)

  @article{ , abstract = {Photon blockades are traditionally classified into conventional and unconventional types, depending on distinct physical mechanisms. Regarding the cavity decay rate , the conventional photon blockade takes place under strong nonlinearity condition ( ), whereas the unconventional photon blockade occurs in the regime of weak nonlinearity ( ). We here propose how to derive an optimal condition for photon blockade utilizing a two-photon Jaynes-Cummings model. Under this condition, the equal-time second-order correlation function reaches its minimum, leading to photon antibunching in both conventional and unconventional photon blockade regimes ( and ), even in . This characteristic is termed universal photon blockade . By comparing it with the conventional and the unconventional photon blockades in the weak-driving limit, the advantages of universal photon blockade are revealed. Our proposal paves an avenue towards the future study of photon blockades and has potential applications in generating antibunched photons.}, archive = {J_PRL}, author = {Yan-Hui Zhou and Tong Liu and Qi-Ping Su and Xing-Yuan Zhang and Qi-Cheng Wu and Dong-Xu Chen and Zhi-Cheng Shi and H. Z. Shen and Chui-Ping Yang}, doi = {10.1103/PhysRevLett.134.183601}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183601}, shortjournal = {Phys. Rev. Lett.}, title = {Universal photon blockade}, volume = {134}, year = {2025}, }
• (2025). Detecting phase coherence of 2D bose gases via noise correlations. PRL, 134(18), 183407. (www)

  @article{ , abstract = {We measure the noise correlations of two-dimensional (2D) Bose gases after free expansion and use them to characterize the in situ phase coherence across the Berezinskii-Kosterlitz-Thouless (BKT) transition. The noise correlation function features a characteristic spatial oscillatory behavior in the superfluid phase, which gives direct access to the superfluid exponent. This oscillatory behavior vanishes above the BKT critical point, as we demonstrate for both single-layer and decoupled bilayer 2D Bose gases. Our Letter establishes noise interferometry as an important general tool to probe and identify many-body states of quantum gases, extending its application to previously inaccessible correlation properties in multimode systems.}, archive = {J_PRL}, author = {Shinichi Sunami and Vijay P. Singh and Erik Rydow and Abel Beregi and En Chang and Ludwig Mathey and Christopher J. Foot}, doi = {10.1103/PhysRevLett.134.183407}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183407}, shortjournal = {Phys. Rev. Lett.}, title = {Detecting phase coherence of 2D bose gases via noise correlations}, volume = {134}, year = {2025}, }
• (2025). Thermodynamics of spin-imbalanced fermi gases with SU(N)-symmetric interaction. PRL, 134(18), 183406. (www)

  @article{ , abstract = {Thermodynamics of degenerate Fermi gases has been extensively studied through various aspects such as Pauli blocking effects, collective modes, BCS superfluidity, and more. Despite this, multicomponent fermions with imbalanced spin configurations remain largely unexplored, particularly beyond the two-component scenario. In this Letter, we generalize the thermodynamic study of fermions to spin-imbalanced configurations based on density fluctuations. Theoretically, we provide closed-form expressions of density fluctuation across all temperature ranges for general spin population setups. Experimentally, after calibrating the measurements with deeply degenerate Fermi gases under spin-balanced configurations ( ), we examine the density fluctuations in spin-imbalanced systems. Specifically, we investigate two-species and four-species configurations to validate our theoretical predictions. Our analysis indicates that interaction enhancement effects can be significant even in highly spin-imbalanced systems. Finally, as an application, we use this approach to examine the decoherence process. Our Letter provides a deeper understanding of the thermodynamic features of spin-imbalanced multicomponent Fermi gases and opens new avenues for exploring complex quantum many-body systems.}, archive = {J_PRL}, author = {Chengdong He and Xin-Yuan Gao and Ka Kwan Pak and Yu-Jun Liu and Peng Ren and Mengbo Guo and Entong Zhao and Yangqian Yan and Gyu-Boong Jo}, doi = {10.1103/PhysRevLett.134.183406}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183406}, shortjournal = {Phys. Rev. Lett.}, title = {Thermodynamics of spin-imbalanced fermi gases with SU(N)-symmetric interaction}, volume = {134}, year = {2025}, }
• (2025). Self-organized cavity bosons beyond the adiabatic elimination approximation. PRL, 134(18), 183405. (www)

  @article{ , abstract = {The longtime behavior of weakly interacting bosons moving in a two-dimensional optical lattice and coupled to a lossy cavity is investigated numerically via the truncated Wigner method, which allows us to take into full account the dynamics of the cavity mode, quantum fluctuations, cavity-boson correlations, and self-organization of individual runs. We first compare our results for small systems with quasi-exact calculations based on quantum trajectories, finding a remarkably good agreement for experimentally relevant boson fillings that improves further with system size. For large systems, we observe metastability at very long times and superfluid quasi–long range order, in sharp contrast with the true long range order found in the ground state of the approximate Bose-Hubbard model with extended interactions, obtained by adiabatically eliminating the cavity field. As the strength of the light-matter coupling increases, the system first becomes supersolid at the Dicke superradiant transition and then turns into a charge-density wave via the Berezinskii-Kosterlitz-Thouless mechanism. The two phase transitions are characterized via an accurate finite-size scaling analysis.}, archive = {J_PRL}, author = {Giuliano Orso and Jakub Zakrzewski and Piotr Deuar}, doi = {10.1103/PhysRevLett.134.183405}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183405}, shortjournal = {Phys. Rev. Lett.}, title = {Self-organized cavity bosons beyond the adiabatic elimination approximation}, volume = {134}, year = {2025}, }
• (2025). Time-resolved spectral gap spectroscopy in a quantum simulator of fermionic superfluidity inside an optical cavity. PRL, 134(18), 183404. (www)

  @article{ , abstract = {We use an ensemble of laser-cooled strontium atoms in a high-finesse cavity to cleanly emulate the technique of rf spectroscopy employed in studies of BEC-BCS physics in fermionic superfluids of degenerate cold gases. Here, we leverage the multilevel internal structure of the atoms to study the physics of Cooper pair breaking in this system. In doing so, we observe and distinguish the properties of two distinct many-body gaps, the BCS pairing gap and the spectral gap, using nondestructive readout techniques. The latter is found to depend on the populations of the internal atomic states, reflecting the chemical potential dependence predicted in fermionic superfluids. This work opens the path for more fully exploiting the rich internal structure of atoms in cavity QED emulators to study both analogous systems and also more exotic states yet to be realized.}, archive = {J_PRL}, author = {Dylan J. Young and Eric Yilun Song and Anjun Chu and Diego Barberena and Zhijing Niu and Vera M. Schäfer and Robert J. Lewis-Swan and Ana Maria Rey and James K. Thompson}, doi = {10.1103/PhysRevLett.134.183404}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183404}, shortjournal = {Phys. Rev. Lett.}, title = {Time-resolved spectral gap spectroscopy in a quantum simulator of fermionic superfluidity inside an optical cavity}, volume = {134}, year = {2025}, }
• (2025). Quantum gas microscopy of fermions in the continuum. PRL, 134(18), 183403. (www)

  @article{ , abstract = {Atom-based quantum simulators offer a unique platform that enables the imaging of each particle in a many-body system. Until now, however, this capability has been limited to quantum systems in discretized space such as optical lattices and tweezers, where spatial degrees of freedom are quantized. Here, we introduce a novel method for imaging atomic quantum many-body systems in the continuum, allowing for in situ resolution of every particle. We demonstrate the capabilities of our approach on a two-dimensional atomic Fermi gas. We probe the density correlation functions, resolving their full spatial functional form, and reveal the shape of the Fermi hole arising from Pauli exclusion as a function of temperature. Our method opens the door to probing strongly correlated quantum gases in the continuum with unprecedented spatial resolution, providing in situ access to spatially resolved correlation functions of arbitrarily high order across the entire system.}, archive = {J_PRL}, author = {Tim de Jongh and Joris Verstraten and Maxime Dixmerias and Cyprien Daix and Bruno Peaudecerf and Tarik Yefsah}, doi = {10.1103/PhysRevLett.134.183403}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183403}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum gas microscopy of fermions in the continuum}, volume = {134}, year = {2025}, }
• (2025). Measuring pair correlations in bose and fermi gases via atom-resolved microscopy. PRL, 134(18), 183402. (www)

  @article{ , abstract = {We demonstrate atom-resolved detection of itinerant bosonic and fermionic quantum gases, enabling the direct in situ measurement of interparticle correlations. In contrast to prior work on lattice-trapped gases, here we realize microscopy of quantum gases in the continuum. We reveal Bose-Einstein condensation with single-atom resolution, measure the enhancement of two-particle correlations of thermal bosons, and observe the suppression of for fermions; the Fermi or exchange hole. For strongly interacting Fermi gases confined to two dimensions, we directly observe nonlocal fermion pairs in the BEC-BCS crossover. We obtain the pair size and the short-range contact directly from the pair correlations. In situ thermometry is enabled via the fluctuation-dissipation theorem. Our technique opens the door to the atom-resolved study of strongly correlated quantum gases of bosons, fermions, and their mixtures.}, archive = {J_PRL}, author = {Ruixiao Yao and Sungjae Chi and Mingxuan Wang and Richard J. Fletcher and Martin Zwierlein}, doi = {10.1103/PhysRevLett.134.183402}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183402}, shortjournal = {Phys. Rev. Lett.}, title = {Measuring pair correlations in bose and fermi gases via atom-resolved microscopy}, volume = {134}, year = {2025}, }
• (2025). In situ imaging of the thermal de broglie wavelength in an ultracold bose gas. PRL, 134(18), 183401. (www)

  @article{ , abstract = {We report the first direct in situ observation of density fluctuations on the scale of the thermal de Broglie wavelength in an ultracold gas of bosons. Bunching of atoms in a quasi-two-dimensional system is observed by single-atom imaging using a quantum gas microscope. Compared to a classical ensemble, we observe a 30% enhancement of the second-order correlation function. We show the spatial and thermal dependence of these correlations. The reported method of detecting in situ correlations can be applied to interacting many-body systems and to the study of critical phenomena near phase transitions.}, archive = {J_PRL}, author = {Jinggang Xiang and Enid Cruz-Colón and Candice C. Chua and William R. Milner and Julius de Hond and Jacob F. Fricke and Wolfgang Ketterle}, doi = {10.1103/PhysRevLett.134.183401}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {183401}, shortjournal = {Phys. Rev. Lett.}, title = {In situ imaging of the thermal de broglie wavelength in an ultracold bose gas}, volume = {134}, year = {2025}, }
• (2025). Diagrammatic monte carlo for finite systems at zero temperature. PRL, 134(18), 182502. (www)

  @article{ , abstract = {High-order virtual excitations play an important role in microscopic models of nuclear reactions at intermediate energies. However, the factorial growth of their complexity has prevented their consistent inclusion in ab initio many-body calculations. For infinite systems at finite temperature, such drawbacks can be overcome using diagrammatic Monte Carlo techniques to resum entire series of Feynman diagrams. We present a diagrammatic Monte Carlo algorithm that can be applied to self-bound systems with discrete energy levels at zero temperature, and demonstrate its potential for the Richardson model of nuclear pairing. We show that sampling the topological space of diagrams allows the inclusion of high-order excitations that are neglected in state-of-the-art approximations used in nuclear physics and quantum chemistry. We propose that sampling the diagrammatic space can overcome the long-standing gap between our microscopic understanding of structure and reactions in nuclear physics.}, archive = {J_PRL}, author = {Stefano Brolli and Carlo Barbieri and Enrico Vigezzi}, doi = {10.1103/PhysRevLett.134.182502}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {182502}, shortjournal = {Phys. Rev. Lett.}, title = {Diagrammatic monte carlo for finite systems at zero temperature}, volume = {134}, year = {2025}, }
• (2025). Charge radii of neutron-rich scandium isotopes and the seniority symmetry in the 0f7/2 shell. PRL, 134(18), 182501. (www)

  @article{ , abstract = {Nuclear charge radii of neutron-rich Sc 47 – 49 isotopes were measured using collinear laser spectroscopy at CERN-ISOLDE. The new data reveal that the charge radii of scandium isotopes exhibit a distinct trend between N = 20 and N = 28 , with Sc 41 and Sc 49 isotopes having similar values, mirroring the closeness of the charge radii of Ca 40 and Ca 48 . Theoretical models that successfully interpret the radii of calcium isotopes could not account for the observed behavior in scandium radii, in particular the reduced odd-even staggering. Remarkably, the inclusion of the new Sc 49 radius data has unveiled a similar trend in the charge radii of N = 28 isotones and Z = 20 isotopes when adding the protons atop the Ca 48 core and the neutrons atop the Ca 40 core, respectively. We demonstrate that this trend is consistent with the prediction of the seniority model.}, archive = {J_PRL}, author = {S. W. Bai and X. F. Yang and Á. Koszorús and J. C. Berengut and J. Billowes and M. L. Bissell and K. Blaum and A. Borschevsky and P. Campbell and B. Cheal and C. S. Devlin and K. T. Flanagan and R. F. Garcia Ruiz and H. Heylen and J. D. Holt and B. S. Hu and A. Kanellakopoulos and J. Krämer and V. Lagaki and B. Maaß and S. Malbrunot-Ettenauer and T. Miyagi and K. König and M. Kortelainen and W. Nazarewicz and R. Neugart and G. Neyens and W. Nörtershäuser and P.-G. Reinhard and M. L. Reitsma and L. V. Rodríguez and F. Sommer and Z. Y. Xu}, doi = {10.1103/PhysRevLett.134.182501}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {182501}, shortjournal = {Phys. Rev. Lett.}, title = {Charge radii of neutron-rich scandium isotopes and the seniority symmetry in the 0f7/2 shell}, volume = {134}, year = {2025}, }
• (2025). Domain-wall skyrmion phase in dense QCD at strong magnetic fields using leading-order chiral perturbation theory. PRL, 134(18), 181902. (www)

  @article{ , abstract = {Low-energy dynamics of QCD can be described by pion degrees of freedom in terms of the chiral perturbation theory. A chiral soliton lattice, an array of solitons, is the ground state due to the chiral anomaly in the presence of a magnetic field larger than a certain critical value at finite density. Here, we show in a model-independent and fully analytic manner (at the leading order of the chiral perturbation theory) that the chiral soliton lattice phase transits to a “domain-wall skyrmion phase” when the chemical potential is larger than the critical value μ c = 16 π f π 2 / 3 m π ∼ 1.03 GeV with the pion’s decay constant f π and mass m π , which can be regarded as the nuclear saturation density. There spontaneously appear stable two-dimensional skyrmions or lumps on a soliton surface, which can be viewed as three-dimensional skyrmions carrying even baryon numbers from the bulk. They behave as superconducting rings with persistent currents due to a charged pion condensation. This phase is in scope of future heavy-ion collider experiments.}, archive = {J_PRL}, author = {Minoru Eto and Kentaro Nishimura and Muneto Nitta}, doi = {10.1103/PhysRevLett.134.181902}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181902}, shortjournal = {Phys. Rev. Lett.}, title = {Domain-wall skyrmion phase in dense QCD at strong magnetic fields using leading-order chiral perturbation theory}, volume = {134}, year = {2025}, }
• (2025). Observation of the charmonium decay ηc→γγ in j/ψ→γηc. PRL, 134(18), 181901. (www)

  @article{ , abstract = {Using ( 2712.4 ± 14.3 ) × 10 6 ψ ( 3686 ) events collected with the BESIII detector at the BEPCII collider, the decay η c → γ γ in J / ψ → γ η c is observed. We determine the product branching fraction B ( J / ψ → γ η c ) × B ( η c → γ γ ) = ( 5.23 ± 0.2 6 stat ± 0.3 0 syst ) × 10 − 6 . This result is consistent with the lattice QCD calculation ( 5.34 ± 0.16 ) × 10 − 6 from HPQCD in 2023. By using the world-average values of B ( J / ψ → γ η c ) and the total decay width of η c , the partial decay width Γ ( η c → γ γ ) is determined to be ( 11.30 ± 0.5 6 stat ± 0.6 6 syst ± 1.1 4 ref ) keV , which deviates from the corresponding world-average value by 3.4 σ .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and M. H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and S. K. Choi and X. Chu and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. X. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and G. F. Fan and J. J. Fan and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Y. Y. Gao and Yang Gao and S. Garbolino and I. Garzia and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and P. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. J. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and Q. Lan and W. N. Lan and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and C. K. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and Lei Li and M. H. Li and M. R. Li and P. L. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and L. Q. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. J. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and W. T. Liu and X. Liu and X. Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and Y. Lu and Y. H. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and J. S. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and Y. H. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and Q. M. Ma and R. Q. Ma and R. Y. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. R. Qi and M. Qi and S. Qian and W. B. Qian and C. F. Qiao and J. H. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and P. B. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and A. Rivetti and M. Rolo and G. Rong and S. S. Rong and Ch. Rosner and M. Q. Ruan and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and Y. C. Sun and Y. H. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and L. F. Tang and M. Tang and Y. A. Tang and L. Y. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and B. Wang and Bo Wang and C. Wang and D. Y. Wang and H. J. Wang and J. J. Wang and K. Wang and L. L. Wang and L. W. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and Lianjie Wu and S. G. Wu and S. M. Wu and X. Wu and X. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and K. J. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and H. Y. Yan and L. Yan and W. B. Yan and W. C. Yan and W. P. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and R. J. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. Q. Yang and Y. X. Yang and Y. Z. Yang and M. Ye and M. H. Ye and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and H. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and Ying Yue and A. A. Zafar and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and N. Zhang and P. Zhang and Q. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. X. Zhang and Z. Y. Zhang and Z. Z. Zhang and Zh. Zh. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and X. R. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and W. J. Zhu and W. Z. Zhu and Y. C. Zhu and Z. A. Zhu and X. Y. Zhuang and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.181901}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of the charmonium decay ηc→γγ in j/ψ→γηc}, volume = {134}, year = {2025}, }
• (2025). Test of lepton flavor universality with B+→K+π+π−ℓ+ℓ− decays. PRL, 134(18), 181803. (www)

  @article{ , abstract = {The first test of lepton flavor universality between muons and electrons using ( , ) decays is presented. The measurement is performed with data from proton-proton collisions collected by the LHCb experiment at center-of-mass energies of 7, 8, and 13 TeV, corresponding to an integrated luminosity of . The ratio of branching fractions between and decays is measured in the dilepton invariant-mass-squared range and is found to be , in agreement with the standard model prediction. The first observation of the decay is also reported.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and E. Bottalico and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and J. D. Brandenburg and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and L. Buonincontri and M. Burgos Marcos and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. C. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and E. Govorkova and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and G. Loachamin Ordonez and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and R. N. Pilato and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and M. Stefaniak and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and T. Tork and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and B. Urbach and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and J. van Eldik and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and T. X. Xing and A. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Z. Zhang and Y. Zhao and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.181803}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181803}, shortjournal = {Phys. Rev. Lett.}, title = {Test of lepton flavor universality with B+→K+π+π−ℓ+ℓ− decays}, volume = {134}, year = {2025}, }
• (2025). Discovering electroweak interacting dark matter at muon colliders using soft tracks. PRL, 134(18), 181802. (www)

  @article{ , abstract = {Minimal dark matter models feature one neutral particle that serves as a thermal relic dark matter candidate, as well as quasidegenerate charged states with TeV masses. When the charged states are produced at colliders, they can decay into dark matter and a low-momentum (soft) charged particle, which is challenging to reconstruct at hadron colliders. We demonstrate that a 3 TeV muon collider is capable of detecting these soft tracks, enabling the discovery of thermal Higgsinos and similar dark matter candidates that constitute highly motivated scenarios for future collider searches.}, archive = {J_PRL}, author = {Rodolfo Capdevilla and Federico Meloni and Jose Zurita}, doi = {10.1103/PhysRevLett.134.181802}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181802}, shortjournal = {Phys. Rev. Lett.}, title = {Discovering electroweak interacting dark matter at muon colliders using soft tracks}, volume = {134}, year = {2025}, }
• (2025). Constraints on axion mediated dipole-dipole interactions. PRL, 134(18), 181801. (www)

  @article{ , abstract = {The search for axions sits at the intersection of solving critical problems in fundamental physics, including the strong C P problem in QCD, uncovering the nature of dark matter, and understanding the origin of the Universe’s matter-antimatter asymmetry. The measurement of axion mediated spin-dependent interactions offers a powerful approach for axion detection. However, it has long been restricted to regions outside the “axion window” due to a significant trade-off: the need to effectively suppress the magnetic leakage from highly polarized spin sources while simultaneously detecting subfemtotesla level exotic physics signals at sub-decimeter-scale distances. In this work, we report new experimental results on axion mediated exotic spin-spin interactions using an iron-shielded SmCo 5 spin source in combination with a specially designed self-compensation comagnetometer. Employing a composite shielding structure, we achieved a suppression of the magnetic field by up to 10 11 . This enabled us to establish new constraints on the coupling between electrons and neutrons, improving previous experimental limits by up to 10 000 times within the axion window. Furthermore, we also set the strongest constraints on the coupling between electrons and protons. The proposed method holds substantial potential not only for advancing the search for new physics beyond the standard model but also for enabling transformative applications in biological and chemical research.}, archive = {J_PRL}, author = {Zitong Xu and Xing Heng and Guoqing Tian and Di Gong and Lei Cong and Wei Ji and Dmitry Budker and Kai Wei}, doi = {10.1103/PhysRevLett.134.181801}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181801}, shortjournal = {Phys. Rev. Lett.}, title = {Constraints on axion mediated dipole-dipole interactions}, volume = {134}, year = {2025}, }
• (2025). Class s superconformal indices from maximal supergravity. PRL, 134(18), 181601. (www)

  @article{ , abstract = {We present a new gauging of maximal supergravity in five spacetime dimensions with gauge group containing ISO(5), involving the local scaling symmetry of the metric, and admitting a supersymmetric anti–de Sitter vacuum. We show this maximal supergravity to arise by consistent truncation of M theory on the (nonspherical, nonparallelizable) six-dimensional geometry associated to a stack of N M5 branes wrapped on a smooth Riemann surface. The existence of this truncation allows us to holographically determine the complete, universal spectrum of light operators of the dual four-dimensional N = 2 theory of class S . We then compute holographically the superconformal index of the dual field theory at large N , finding perfect agreement with previously known field theory results in specific limits.}, archive = {J_PRL}, author = {Ritabrata Bhattacharya and Abhay Katyal and Oscar Varela}, doi = {10.1103/PhysRevLett.134.181601}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181601}, shortjournal = {Phys. Rev. Lett.}, title = {Class s superconformal indices from maximal supergravity}, volume = {134}, year = {2025}, }
• (2025). Superconducting levitated detector of gravitational waves. PRL, 134(18), 181402. (www)

  @article{ , abstract = {A magnetically levitated mass couples to gravity and can act as an effective gravitational wave detector. We show that a superconducting sphere levitated in a quadrupolar magnetic field, when excited by a gravitational wave, will produce magnetic field fluctuations that can be read out using a flux tunable microwave resonator. With a readout operating at the standard quantum limit, such a system could achieve broadband strain noise sensitivity of for frequencies of 1 kHz–1 MHz, opening new corridors for astrophysical probes of new physics.}, archive = {J_PRL}, author = {Daniel Carney and Gerard Higgins and Giacomo Marocco and Michael Wentzel}, doi = {10.1103/PhysRevLett.134.181402}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181402}, shortjournal = {Phys. Rev. Lett.}, title = {Superconducting levitated detector of gravitational waves}, volume = {134}, year = {2025}, }
• (2025). Dynamical formation of regular black holes. PRL, 134(18), 181401. (www)

  @article{ , abstract = {We study dynamical gravitational collapse in a theory with an infinite tower of higher-derivative corrections to the Einstein-Hilbert action and we show that, under very general conditions, it leads to the formation of regular black holes. Our results are facilitated by the use of a class of theories that possess second-order equations on spherically symmetric metrics, but which are general enough to provide a basis for the gravitational effective action in any . We analytically solve the collapse of a thin shell of dust and show that it inevitably experiences a bounce at small radius and that its motion can be extended to arbitrary proper time. The collapse of the shell always gives rise to a singularity-free, geodesically complete spacetime that contains horizons if the total mass is above a critical value. In that case, the shell bounces into a new universe through a white hole explosion. Our construction provides, to the best of our knowledge, the first fully dynamical description of formation of regular black holes, and it suggests that higher-derivative corrections may be the most natural way to resolve the singularities of Einstein’s theory.}, archive = {J_PRL}, author = {Pablo Bueno and Pablo A. Cano and Robie A. Hennigar and Ángel J. Murcia}, doi = {10.1103/PhysRevLett.134.181401}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181401}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical formation of regular black holes}, volume = {134}, year = {2025}, }
• (2025). Detectable MeV neutrino signals from neutron-star common-envelope systems. PRL, 134(18), 181003. (www)

  @article{ , abstract = {Common envelope evolution—where a star is engulfed by a companion—is a critical but poorly understood step in, e.g., the formation pathways for gravitational-wave sources. However, it has been extremely challenging to identify observable signatures of such systems. We show that for systems involving a neutron star, the hypothesized super-Eddington accretion onto the neutron star produces MeV-range, months-long neutrino signals within reach of present and planned detectors. While there are substantial uncertainties on the rate of such events ( in the Milky Way) and the neutrino luminosity (which may be less than the accretion power), this signal can only be found if dedicated new analyses are developed. If detected, the neutrino signal would probe super-Eddington accretion, leading to significant new insights into the astrophysics of common envelope evolution.}, archive = {J_PRL}, author = {Ivan Esteban and John F. Beacom and Joachim Kopp}, doi = {10.1103/PhysRevLett.134.181003}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181003}, shortjournal = {Phys. Rev. Lett.}, title = {Detectable MeV neutrino signals from neutron-star common-envelope systems}, volume = {134}, year = {2025}, }
• (2025). Hints of nonminimally coupled gravity in DESI 2024 baryon acoustic oscillation measurements. PRL, 134(18), 181002. (www)

  @article{ , abstract = {The cosmic microwave background (CMB) and baryon acoustic oscillations (BAO) are two of the most robust observations in cosmology. The recent BAO measurements from the DESI collaboration have presented, for the first time, inconsistency between BAO and CMB within the standard cosmological model , indicating a preference for dynamical dark energy over a cosmological constant. We analyze the theoretical implication of the DESI BAO observation for dark energy and gravity employing a nonparametric reconstruction approach for both the dark energy equation of state and the effective field theory coefficients. We find that the DESI data can rule out quintessence dark energy by indicating a crossing of the phantom divide at . Furthermore, when analyzed within the broad context of Horndeski gravity which includes general relativity and many known modified gravity theories such as generalized Galileons, and Brans-Dicke, our result implies that gravity should be nonminimally coupled to explain the observations, establishing the DESI result as the first hint of modified gravity. Based on these insights, we propose the thawing gravity model to explain the nonminimal coupling and phantom crossing indicated by observation, which also fits better to DESI BAO, CMB, and type Ia Supernovae data than .}, archive = {J_PRL}, author = {Gen Ye and Matteo Martinelli and Bin Hu and Alessandra Silvestri}, doi = {10.1103/PhysRevLett.134.181002}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181002}, shortjournal = {Phys. Rev. Lett.}, title = {Hints of nonminimally coupled gravity in DESI 2024 baryon acoustic oscillation measurements}, volume = {134}, year = {2025}, }
• (2025). Enabling strong neutrino self-interaction with an unparticle mediator. PRL, 134(18), 181001. (www)

  @article{ , abstract = {Recent explorations of the cosmic microwave background and the large-scale structure of the universe have indicated a preference for sizable neutrino self-interactions, much stronger than what the standard model offers. When interpreted in the context of simple particle-physics models with a light, neutrinophilic scalar mediator, some of the hints are already in tension with the combination of terrestrial, astrophysical, and cosmological constraints. We take a novel approach by considering neutrino self-interactions through a mediator with a smooth, continuous spectral density function. We consider Georgi’s unparticle with a mass gap as a concrete example and point out two useful effects for mitigating two leading constraints. (i) The Unparticle is “broadband’—it occupies a wide range of masses which allows it to pass the early universe constraint on effective number of extra neutrinos ( ) even if the mass gap lies below the MeV scale. (ii) Scattering involving unparticles is less resonant, which lifts the constraint set by IceCube based on a recent measurement of ultra-high-energy cosmogenic neutrinos. Our analysis shows that an unparticle mediator can open up ample parameter space for strong neutrino self-interactions of interest to cosmology and serves a well-motivated target for upcoming experiments.}, archive = {J_PRL}, author = {Saeid Foroughi-Abari and Kevin J. Kelly and Mudit Rai and Yue Zhang}, doi = {10.1103/PhysRevLett.134.181001}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {181001}, shortjournal = {Phys. Rev. Lett.}, title = {Enabling strong neutrino self-interaction with an unparticle mediator}, volume = {134}, year = {2025}, }
• (2025). Robust approach for time-bin-encoded photonic quantum information protocols. PRL, 134(18), 180802. (www)

  @article{ , abstract = {Quantum states encoded in the time-bin degree of freedom of photons represent a fundamental resource for quantum information protocols. Traditional methods for generating and measuring time-bin-encoded quantum states face severe challenges due to optical instabilities, complex setups, and timing resolution requirements. To circumvent these issues, we leverage an approach based on Hong-Ou-Mandel interference and we propose and demonstrate a robust and scalable protocol to generate and measure arbitrary high-dimensional time-bin quantum states. We experimentally implement the protocol in a photonic setup reaching high-fidelity quantum state tomographies of two- and three-dimensional quantum states encoded in time bins with short temporal separation. We also certify intrasystem polarization-time entanglement of single photons through a nonclassicality test. The demonstrated approach enables access to high-dimensional states and tasks that are practically inaccessible with standard schemes, thereby advancing fundamental quantum information science and opening applications in quantum communication.}, archive = {J_PRL}, author = {Simon J. U. White and Emanuele Polino and Farzad Ghafari and Dominick J. Joch and Luis Villegas-Aguilar and Lynden K. Shalm and Varun B. Verma and Marcus Huber and Nora Tischler}, doi = {10.1103/PhysRevLett.134.180802}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180802}, shortjournal = {Phys. Rev. Lett.}, title = {Robust approach for time-bin-encoded photonic quantum information protocols}, volume = {134}, year = {2025}, }
• (2025). Genuine quantum non-gaussianity and metrological sensitivity of fock states prepared in a mechanical resonator. PRL, 134(18), 180801. (www)

  @article{ , abstract = {Fock states of the quantum harmonic oscillator are fundamental to quantum sensing and information processing, serving as key resources for exploiting bosonic degrees of freedom. Here, we prepare high Fock states in a high-overtone bulk acoustic wave resonator by coupling it to a superconducting qubit and applying microwave pulses designed using quantum optimal control. We characterize the experimentally realized states by employing a criterion for genuine quantum non-Gaussianity (QNG) designed to reveal multiphonon contributions. Although energy relaxation and decoherence limit the achievable fidelities, we demonstrate genuine QNG features compatible with a Fock state , confirming that the prepared states cannot be generated through Gaussian operations on states with up to Fock state contributions. We further investigate the robustness of these QNG features to losses and their utility in sensing displacement amplitudes. In particular, we introduce a hierarchy based on the quantum Fisher information and show that, despite decoherence and measurement imperfections, the prepared states achieve a displacement sensitivity surpassing that of an ideal Fock state . Our results have immediate applications in quantum sensing and simulations with high-overtone bulk acoustic wave resonator devices.}, archive = {J_PRL}, author = {Q. Rumman Rahman and Igor Kladarić and Max-Emanuel Kern and Lukáš Lachman and Yiwen Chu and Radim Filip and Matteo Fadel}, doi = {10.1103/PhysRevLett.134.180801}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180801}, shortjournal = {Phys. Rev. Lett.}, title = {Genuine quantum non-gaussianity and metrological sensitivity of fock states prepared in a mechanical resonator}, volume = {134}, year = {2025}, }
• (2025). Quantum dynamic programming. PRL, 134(18), 180602. (www)

  @article{ , abstract = {We introduce a quantum extension of dynamic programming, a fundamental computational method that efficiently solves recursive problems using memory. Our innovation lies in showing how to coherently generate recursion step unitaries by using memorized intermediate quantum states. Quantum dynamic programming achieves an exponential reduction in circuit depth for a broad class of fixed-point quantum recursions, though this comes at the cost of increased circuit width. Interestingly, the trade-off becomes more favorable when the initial state is pure. By hybridizing our approach with a conventional memoryless one, we can flexibly balance circuit depth and width to optimize performance on quantum devices with fixed hardware constraints. Finally, we showcase applications of quantum dynamic programming to several quantum recursions, including a variant of Grover’s search, quantum imaginary-time evolution, and a new protocol for obliviously preparing a quantum state in its Schmidt basis.}, archive = {J_PRL}, author = {Jeongrak Son and Marek Gluza and Ryuji Takagi and Nelly H. Y. Ng}, doi = {10.1103/PhysRevLett.134.180602}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180602}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum dynamic programming}, volume = {134}, year = {2025}, }
• (2025). Energy barrier of hypergraph product codes. PRL, 134(18), 180601. (www)

  @article{ , abstract = {A macroscopic energy barrier is a necessary condition for self-correcting quantum memory. In this Letter, we prove tight bounds on the energy barrier applicable to any quantum code obtained from the hypergraph product of two classical codes. If the underlying classical codes are low-density parity-check codes (LDPC), the energy barrier of the quantum code is shown to be the minimum energy barrier of the underlying classical codes (and their transposes) up to an additive O ( 1 ) constant.}, archive = {J_PRL}, author = {Guangqi Zhao and Andrew C. Doherty and Isaac H. Kim}, doi = {10.1103/PhysRevLett.134.180601}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180601}, shortjournal = {Phys. Rev. Lett.}, title = {Energy barrier of hypergraph product codes}, volume = {134}, year = {2025}, }
• (2025). Unveiling eigenstate thermalization for non-hermitian systems. PRL, 134(18), 180405. (www)

  @article{ , abstract = {The eigenstate thermalization hypothesis (ETH) has been highly influential in explaining thermodynamic behavior of closed quantum systems. As of yet, it is unclear whether and how the ETH applies to non-Hermitian systems. Here, we introduce a framework that extends the ETH to non-Hermitian systems, within which expectation values of local operators reproduce statistical and scaling predictions known from Hermitian ETH. We illustrate the validity of the framework on non-Hermitian random-matrix and Sachdev-Ye-Kitaev models. Further, we show numerically how the static ETH predictions become imprinted onto the dynamics of local observables. Finally, we present a prescription for observing both ETH-obeying and ETH-violating regimes in an optical-lattice experiment that implements a disordered interacting Hatano-Nelson model. Our results generalize the celebrated ETH to the non-Hermitian setting, and they show how it affects the system dynamics, and how the salient signatures can be observed in present-day cold-atom experiments.}, archive = {J_PRL}, author = {Sudipto Singha Roy and Soumik Bandyopadhyay and Ricardo Costa de Almeida and Philipp Hauke}, doi = {10.1103/PhysRevLett.134.180405}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180405}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling eigenstate thermalization for non-hermitian systems}, volume = {134}, year = {2025}, }
• (2025). Unitary designs of symmetric local random circuits. PRL, 134(18), 180404. (www)

  @article{ , abstract = {We have established the method of characterizing the unitary design generated by a symmetric local random circuit. Concretely, we have shown that the necessary and sufficient condition for the circuit asymptotically forming a -design is given by simple integer optimization for general symmetry and locality. By using the result, we explicitly give the maximal order of unitary design under the , U(1), and SU(2) symmetries for general locality. This work reveals the relation between the fundamental notions of symmetry and locality in terms of randomness.}, archive = {J_PRL}, author = {Yosuke Mitsuhashi and Ryotaro Suzuki and Tomohiro Soejima and Nobuyuki Yoshioka}, doi = {10.1103/PhysRevLett.134.180404}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180404}, shortjournal = {Phys. Rev. Lett.}, title = {Unitary designs of symmetric local random circuits}, volume = {134}, year = {2025}, }
• (2025). Optimal conversion from classical to quantum randomness via quantum chaos. PRL, 134(18), 180403. (www)

  @article{ , abstract = {Quantum many-body systems provide a unique platform for exploring the rich interplay between chaos, randomness, and complexity. In a recently proposed paradigm known as deep thermalization, random quantum states of system A are generated by performing projective measurements on system B following chaotic Hamiltonian evolution acting jointly on A B . In this scheme, the randomness of the projected state ensemble arises from the intrinsic randomness of the outcomes when B is measured. Here, we propose a modified scheme in which classical randomness injected during the protocol is converted by quantum chaos into quantum randomness of the resulting state ensemble. We show that for generic chaotic systems this conversion is optimal in that each bit of injected classical entropy generates as much additional quantum randomness as adding an extra qubit to B . This significantly enhances the randomness of the projected ensemble without imposing additional demands on the quantum hardware. Our scheme can be easily implemented on typical analog quantum simulators, providing a more scalable route for generating quantum randomness valuable for many applications. In particular, we demonstrate that the accuracy of a shadow tomography protocol can be substantially improved.}, archive = {J_PRL}, author = {Wai-Keong Mok and Tobias Haug and Adam L. Shaw and Manuel Endres and John Preskill}, doi = {10.1103/PhysRevLett.134.180403}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180403}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal conversion from classical to quantum randomness via quantum chaos}, volume = {134}, year = {2025}, }
• (2025). Strict area law entanglement versus chirality. PRL, 134(18), 180402. (www)

  @article{ , abstract = {Chirality is a property of a gapped phase of matter in two spatial dimensions that can be manifested through nonzero thermal or electrical Hall conductance. In this Letter, we prove two no-go theorems that forbid such chirality for a quantum state in a finite dimensional local Hilbert space with strict area law entanglement entropies. We also show that the finite dimensional local Hilbert space condition can be relaxed to the condition that the state has finite local entanglement entropies. As a crucial ingredient in the proofs, we introduce a new quantum information-theoretic primitive called instantaneous modular flow , which has many other potential applications.}, archive = {J_PRL}, author = {Xiang Li and Ting-Chun Lin and John McGreevy and Bowen Shi}, doi = {10.1103/PhysRevLett.134.180402}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180402}, shortjournal = {Phys. Rev. Lett.}, title = {Strict area law entanglement versus chirality}, volume = {134}, year = {2025}, }
• (2025). Topological quantum batteries. PRL, 134(18), 180401. (www)

  @article{ , abstract = {We propose an innovative design for quantum batteries (QBs) that involves coupling two-level systems to a topological photonic waveguide. Employing the resolvent method, we analytically explore the thermodynamic performance of QBs. First, we demonstrate that in the long-time limit, only bound states significantly contribute to the stored energy of QBs. We observe that near-perfect energy transfer can occur in the topologically nontrivial phase. Moreover, the maximum stored energy exhibits singular behavior at the phase boundaries, where the number of bound states undergoes a transition. Second, when a quantum charger and a quantum battery are coupled at the same sublattice within a unit cell, the ergotropy becomes immune to dissipation at that location, facilitated by a dark state and a topologically robust dressed bound state. Third, we show that as dissipation intensifies along with the emergence of the quantum Zeno effect, the charging power of QBs experiences a temporary boost. Our findings offer valuable guidance for improving quantum battery performance in realistic conditions through structured reservoir engineering.}, archive = {J_PRL}, author = {Zhi-Guang Lu and Guoqing Tian and Xin-You Lü and Cheng Shang}, doi = {10.1103/PhysRevLett.134.180401}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180401}, shortjournal = {Phys. Rev. Lett.}, title = {Topological quantum batteries}, volume = {134}, year = {2025}, }
• (2025). Active optical intensity interferometry. PRL, 134(18), 180201. (www)

  @article{ , abstract = {Long baseline diffraction-limited optical aperture synthesis technology by interferometry plays an important role in scientific study and practical application. In contrast to amplitude (phase) interferometry, intensity interferometry—which exploits the second-order coherence of thermal light—is robust against atmospheric turbulence and optical defects. However, a thermal light source typically has a broadband spectrum, a low average photon number per mode, and a wide divergence angle, forestalling extended applications. Here, we propose and demonstrate active intensity interferometry for optical synthetic aperture imaging over the kilometer range. Our scheme employs multiple phase-independent laser emitters to generate thermal illumination and utilizes a flexible computational algorithm for image reconstruction. Through outdoor experiments, we have successfully imaged millimeter-scale targets located at 1.36 km away, achieving a resolution enhancement by about 14 times over the diffraction limit of a single telescope. The application of long-baseline active intensity interferometry holds promise for advancing high-resolution optical imaging and sensing.}, archive = {J_PRL}, author = {Lu-Chuan Liu and Cheng Wu and Wei Li and Yu-Ao Chen and Xiao-Peng Shao and Frank Wilczek and Feihu Xu and Qiang Zhang and Jian-Wei Pan}, doi = {10.1103/PhysRevLett.134.180201}, journal = {Physical Review Letters}, month = {5}, number = {18}, pages = {180201}, shortjournal = {Phys. Rev. Lett.}, title = {Active optical intensity interferometry}, volume = {134}, year = {2025}, }
• (2025). Ergodicity breaking and scaling relations for finite-time first-order phase transition. PRL, 134(17), 177101. (www)

  @article{ , abstract = {Hysteresis and metastable states are typical features associated with ergodicity breaking in the first-order phase transition. We explore the scaling relations of nonequilibrium thermodynamics in finite-time first-order phase transitions. Using the Curie-Weiss model as an example, for large systems we find the excess work scales as when the magnetic field is quenched at a finite rate across the phase transition. We further reveal a crossover in the scaling of the excess work from to when downsizing the system. Our study elucidates the interplay between the finite-time dynamics and the finite-size effect, which leads to different scaling behaviors of the excess work with or without ergodicity breaking.}, archive = {J_PRL}, author = {Yu-Xin Wu and Jin-Fu Chen and H. T. Quan}, doi = {10.1103/PhysRevLett.134.177101}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {177101}, shortjournal = {Phys. Rev. Lett.}, title = {Ergodicity breaking and scaling relations for finite-time first-order phase transition}, volume = {134}, year = {2025}, }
• (2025). Attosecond control of solid-state high harmonic generation using ω−3ω fields. PRL, 134(17), 176903. (www)

  @article{ , abstract = {High harmonic spectra generated in condensed matter carry the fingerprints of subcycle electronic motion and the energy structure of the studied system. Here, we show that tailoring the waveform of midinfrared driving light by using a coherent combination with its third harmonic frequency allows one to control the time of electron tunneling to the conduction band within each half-cycle of the fundamental wave with attosecond precision. We introduce an experimental scheme in which we simultaneously monitor the modulation of amplitude and emission delays of high harmonic radiation and the excited electron population generated in crystalline silicon as a function of the relative phase between the fields. We observe that the mutual phase required for the maximum yield of high harmonic generation is shifted by approximately with respect to the phase leading to maximal generated carrier population. The observed emission delays of high harmonic photons of up to few hundred attoseconds scale with the time delay and with the ratio between the electric field amplitudes of the two-color fields. These results reveal the connection between electron tunneling and high harmonic emission processes in solids.}, archive = {J_PRL}, author = {Adam Gindl and Pawan Suthar and František Trojánek and Petr Malý and Thibault J.-Y. Derrien and Martin Kozák}, doi = {10.1103/PhysRevLett.134.176903}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {176903}, shortjournal = {Phys. Rev. Lett.}, title = {Attosecond control of solid-state high harmonic generation using ω−3ω fields}, volume = {134}, year = {2025}, }
• (2025). Experimental observation of vortex gyration excited by surface acoustic waves. PRL, 134(17), 176704. (www)

  @article{ , abstract = {We report experiments using magnetic resonance force microscopy to investigate the dynamics of magnetic vortices in submicrometer CoFeB disks grown on a piezoelectric substrate. We compare the vortex gyration excited inductively by microwave magnetic fields and through magnetoelastic coupling via surface acoustic waves (SAWs). Based on the device geometry and modeling performed, we find that the dominant mechanism for SAW-driven excitation is through lattice rotations, which generate an effective field localized at the vortex core. This contrasts with the magnetoelastic strains typically assumed in similar experiments. Moreover, we demonstrate that this magnetorotation torque can be tuned by applying a perpendicular magnetic field. Unlike spin wave excitations, nontrivial spin textures, such as vortices, effectively couple to magnetorotation torques, making them valuable probes for studying such phenomena.}, archive = {J_PRL}, author = {R. Lopes Seeger and F. Millo and G. Soares and J.-V. Kim and A. Solignac and G. de Loubens and T. Devolder}, doi = {10.1103/PhysRevLett.134.176704}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {176704}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental observation of vortex gyration excited by surface acoustic waves}, volume = {134}, year = {2025}, }
• (2025). Entangling color centers via magnon-antimagnon pair creation. PRL, 134(17), 176703. (www)

  @article{ , abstract = {We present how entanglement between a spatially separated pair of color centers can be created by letting them weakly interact with the quantum fluctuations of a nonequilibrium magnetic environment. To this end, we consider two coupled ferromagnets, one in the ground state and one in an inverted state with respect to an applied magnetic field. The resulting energetic instability leads to a quantum spin current in the vacuum state that is sustained by the creation of magnon-antimagnon pairs at the interface. We show that these quantum fluctuations imprint a steady-state entanglement onto the two dipole-coupled color centers through nonlocal dissipation. We derive conditions for establishing a maximally entangled Bell state. This entanglement is absent in thermal equilibrium.}, archive = {J_PRL}, author = {Eric Kleinherbers and Shane P. Kelly and Yaroslav Tserkovnyak}, doi = {10.1103/PhysRevLett.134.176703}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {176703}, shortjournal = {Phys. Rev. Lett.}, title = {Entangling color centers via magnon-antimagnon pair creation}, volume = {134}, year = {2025}, }
• (2025). Half-integer quantum hall states in two-dimensional graphite. PRL, 134(17), 176302. (www)

  @article{ , abstract = {Non-Abelian fractionalized quasiparticles in half-integer quantum Hall states have been proposed as a platform for the realization of topologically protected fault-tolerant qubits. We observe half-integer quantum Hall states out to remarkably large Landau level filling factors larger than 30 in dual-gated -thick graphite devices. We identify most as single-component states stabilized by fractional correlations in exterior bilayers. Multicomponent (3,3,1) states with strong correlations between opposite-valley states on opposite sides of the graphite interior also appear. The facile integration of graphite with top and bottom surface gates makes thin film graphite an attractive platform to explore the physics of non-Abelian fractionalized quasiparticles.}, archive = {J_PRL}, author = {Nicholas Mazzucca and Bishoy M. Kousa and Kenji Watanabe and Takashi Taniguchi and Allan H. MacDonald and Marc W. Bockrath}, doi = {10.1103/PhysRevLett.134.176302}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {176302}, shortjournal = {Phys. Rev. Lett.}, title = {Half-integer quantum hall states in two-dimensional graphite}, volume = {134}, year = {2025}, }
• (2025). Inverse design of kirigami through shape programming of rotating units. PRL, 134(17), 176103. (www)

  @article{ , abstract = {Kirigami metamaterials have enabled a plethora of morphing patterns across art and engineering. However, the inverse design of kirigami for complex shapes remains a puzzle that so far cannot be solved without relying on complex numerical methods. Here, we present a purely geometric design method to overcome the reliance on sophisticated numerical algorithms and showcase how to leverage it for three distinct types of morphing targets, i.e., the contracted shape, the deployed shape, and the internal trajectories of the rotating units in kirigami specimens. Our results unveil the fundamental relations between the kirigami deformation and the shape of its rotating units and enable us to establish the underpinning physics through theoretical investigations validated via numerical simulations. This work brings ground-rule insights into morphing matter with rotating units and offers an intuitive, firsthand geometric route for the swift design of complex kirigami.}, archive = {J_PRL}, author = {Chuan Qiao and Shijun Chen and Yu Chen and Zhihong Zhou and Wentao Jiang and Qingyuan Wang and Xiaobao Tian and Damiano Pasini}, doi = {10.1103/PhysRevLett.134.176103}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {176103}, shortjournal = {Phys. Rev. Lett.}, title = {Inverse design of kirigami through shape programming of rotating units}, volume = {134}, year = {2025}, }
• (2025). Transverse josephson diode effect in tilted dirac systems. PRL, 134(17), 176002. (www)

  @article{ , abstract = {We theoretically study the transverse charge transport in Josephson junctions based on the tilted Dirac materials with valley-dependent gaps. It is shown that a finite tilt-assisted transverse Josephson Hall current is present under broken time-reversal symmetry. This transverse current is driven by the superconducting phase difference across the junction and exhibits a nonsinusoidal current-phase relation, leading to the transverse Josephson diode effect (TJDE), where the critical currents flowing oppositely along the transverse direction are asymmetric. Compared to the conventional longitudinal Josephson diode effect, the predicted TJDE supports a fully polarized diode efficiency with a 100% quality factor and can completely decouple the input signal path from the output, suggesting potential applications for nonreciprocal superconducting devices.}, archive = {J_PRL}, author = {W. Zeng}, doi = {10.1103/PhysRevLett.134.176002}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {176002}, shortjournal = {Phys. Rev. Lett.}, title = {Transverse josephson diode effect in tilted dirac systems}, volume = {134}, year = {2025}, }
• (2025). Anomalous radiation reaction in a circularly polarized field. PRL, 134(17), 175001. (www)

  @article{ , abstract = {Quantum corrections to electron dynamics in a circularly polarized electromagnetic field are found within the Floquet theory of periodically driven quantum systems. It is demonstrated that emission of photons by an electron rotating under the field leads to the quantum recoil force acting on the electron perpendicularly to the velocity of its forward movement, which differs crucially from the known classical recoil force directed oppositely to the velocity. Physically, such an anomalous radiation reaction arises from the one-loop QED correction to the photon emission and has no analog within the classical electrodynamics. Possible manifestations of this macroscopic QED effect are discussed for electrons in strong laser fields.}, archive = {J_PRL}, author = {O. V. Kibis}, doi = {10.1103/PhysRevLett.134.175001}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {175001}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous radiation reaction in a circularly polarized field}, volume = {134}, year = {2025}, }
• (2025). Evidence for electron spin-torsion coupling in the rotational spectrum of the CH3CO radical. PRL, 134(17), 173001. (www)

  @article{ , abstract = {Open-shell nonrigid molecular systems exhibiting an internal rotation are likely candidates for a coupling between the spin angular momentum of the unpaired electron and the torsional motion. This electron spin-torsion coupling lacked both an experimental validation and a theoretical modeling. Here, the first experimental observation of the electron spin-torsion coupling is reported analyzing the pure rotational spectrum at millimeter wavelengths of the radical, a open-shell molecule displaying an internal rotation of its methyl group. To account for this coupling, a specific Hamiltonian incorporating the rotational, torsional, and electronic degrees of freedom is developed and allows us to reproduce the experimental spectrum. The present demonstration of the electron spin-torsion coupling will undoubtedly be key to future investigations of large open-shell molecules exhibiting a complex internal dynamics.}, archive = {J_PRL}, author = {Laurent H. Coudert and Olivier Pirali and Marie-Aline Martin-Drumel and Rosemonde Chahbazian and Luyao Zou and Roman A. Motiyenko and Laurent Margulès}, doi = {10.1103/PhysRevLett.134.173001}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {173001}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for electron spin-torsion coupling in the rotational spectrum of the CH3CO radical}, volume = {134}, year = {2025}, }
• (2025). Impact of newly measured β-delayed neutron emitters around ni78 on light element nucleosynthesis in the neutrino wind following a neutron star merger. PRL, 134(17), 172701. (www)

  @article{ , abstract = {Neutron emission probabilities and half-lives of 37 -delayed neutron emitters from to were measured at the RIKEN Nishina Center in Japan, including 11 one-neutron and 13 two-neutron emission probabilities and six half-lives for the first time that supersede theoretical estimates. These nuclei lie in the path of the weak process occurring in neutrino-driven winds from the accretion disk formed after the merger of two neutron stars synthesizing elements in the abundance peak. The presence of such elements dominates the accompanying kilonova emission over the first few days and have been identified in the AT2017gfo event, associated to the gravitational wave detection GW170817. Abundance calculations based on over 17 000 simulated trajectories describing the evolution of matter properties in the merger outflows show that the new data lead to an increase of 50%–70% in the abundance of Y, Zr, Nb, and Mo. This enhancement is large compared to the scatter of relative abundances observed in old very metal poor stars and thus is significant in the comparison with other possible astrophysical processes contributing to the light-element production. These results underline the importance of including experimental decay data for very neutron-rich -delayed neutron emitters into -process models.}, archive = {J_PRL}, author = {A. Tolosa-Delgado and J. L. Tain and M. Reichert and A. Arcones and M. Eichler and B. C. Rasco and N. T. Brewer and K. P. Rykaczewski and R. Yokoyama and R. Grzywacz and I. Dillmann and J. Agramunt and D. S. Ahn and A. Algora and H. Baba and S. Bae and C. G. Bruno and R. Caballero Folch and F. Calvino and P. J. Coleman-Smith and G. Cortes and T. Davinson and C. Domingo-Pardo and A. Estrade and N. Fukuda and S. Go and C. J. Griffin and J. Ha and O. Hall and L. Harkness-Brennan and T. Isobe and D. Kahl and M. Karny and L. H. Khiem and G. G. Kiss and M. Kogimtzis and A. Korgul and S. Kubono and M. Labiche and I. Lazarus and J. Liang and J. Lee and J. Liu and G. Lorusso and K. Matsui and K. Miernik and F. Montes and B. Moon and A. I. Morales and N. Nepal and S. Nishimura and R. D. Page and M. Piersa-Siłkowska and V. H. Phong and Zs. Podolyák and V. F. E. Pucknell and P. H. Regan and B. Rubio and Y. Saito and H. Sakurai and Y. Shimizu and J. Simpson and P.-A. Söderström and D. W. Stracener and T. Sumikama and R. Surman and H. Suzuki and M. Takechi and H. Takeda and A. Tarifeño-Saldivia and S. L. Thomas and M. Wolińska-Cichocka and P. J. Woods and X. X. Xu}, doi = {10.1103/PhysRevLett.134.172701}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {172701}, shortjournal = {Phys. Rev. Lett.}, title = {Impact of newly measured β-delayed neutron emitters around ni78 on light element nucleosynthesis in the neutrino wind following a neutron star merger}, volume = {134}, year = {2025}, }
• (2025). NuSTAR bounds on radiatively decaying particles from m82. PRL, 134(17), 171004. (www)

  @article{ , abstract = {Axions and other putative feebly interacting particles with a mass of tens to several hundreds of keVs can be produced in stellar cores with a Lorentz boost factor . Thus, starburst galaxies such as M82 are efficient factories of slow axions. Their decay would produce a large flux of x-ray photons, peaking around 100 keV and spread around the Galaxy by an angle that can be relatively large. We use observations of the Nuclear Spectroscopic Telescope Array mission to show that the absence of these features can constrain 30–500 keV axion masses into uncharted regions for axion-photon coupling of . Our argument can be applied to other heavy feebly interacting particles and astrophysical sources that are hot enough to produce them, yet cold enough to avoid large boost factors which slow down the decay.}, archive = {J_PRL}, author = {Francisco R. Candón and Damiano F. G. Fiorillo and Giuseppe Lucente and Edoardo Vitagliano and Julia K. Vogel}, doi = {10.1103/PhysRevLett.134.171004}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {171004}, shortjournal = {Phys. Rev. Lett.}, title = {NuSTAR bounds on radiatively decaying particles from m82}, volume = {134}, year = {2025}, }
• (2025). Leading axion-photon sensitivity with NuSTAR observations of m82 and m87. PRL, 134(17), 171003. (www)

  @article{ , abstract = {We perform one of the most sensitive searches to date for the existence of ultralight axions using data from the NuSTAR telescope. We search for stellar axion production in the M82 starburst galaxy and the M87 central galaxy of the Virgo cluster and then the subsequent conversion into hard x-rays in the surrounding magnetic fields. We sum over the full stellar populations in these galaxies when computing the axion luminosity, and we account for the conversion of axions to photons by using magnetic field profiles in simulated IllustrisTNG analog galaxies. We show that analyzing NuSTAR data toward these targets between roughly 30 and 70 keV shows no evidence for axions and leads to robust constraints on the axion-photon coupling at the level of for at 95% confidence.}, archive = {J_PRL}, author = {Orion Ning and Benjamin R. Safdi}, doi = {10.1103/PhysRevLett.134.171003}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {171003}, shortjournal = {Phys. Rev. Lett.}, title = {Leading axion-photon sensitivity with NuSTAR observations of m82 and m87}, volume = {134}, year = {2025}, }
• (2025). Simulating sparse hamiltonians on 2D lattices. PRL, 134(17), 170602. (www)

  @article{ , abstract = {Systems with sparse, yet long-range interactions, form a rich class capable of exhibiting various interesting physics, including good error correction. In this Letter we show how to simulate any sparse Pauli Hamiltonian with a 2D nearest neighbor Hamiltonian, using fewer resources than previous techniques. As an application we demonstrate how to simulate a good quantum code Hamiltonian, effectively approximating a code in two dimensions.}, archive = {J_PRL}, author = {Harriet Apel and Nouédyn Baspin}, doi = {10.1103/PhysRevLett.134.170602}, journal = {Physical Review Letters}, month = {5}, number = {17}, pages = {170602}, shortjournal = {Phys. Rev. Lett.}, title = {Simulating sparse hamiltonians on 2D lattices}, volume = {134}, year = {2025}, }
• (2025). Erratum: Measurement of the cross sections of Ξc0 and Ξc+ baryons and of the branching-fraction ratio BR(Ξc0→Ξ−e+νe)/BR(Ξc0→Ξ−π+) in pp collisions at s=13 TeV [Phys. rev. lett. 127, 272001 (2021)]. PRL, 134(17), 179902. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 179902 (2025)}, archive = {J_PRL}, author = {ALICE Collaboration and S. Acharya and et al}, doi = {10.1103/PhysRevLett.134.179902}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {179902}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Measurement of the cross sections of Ξc0 and Ξc+ baryons and of the branching-fraction ratio BR(Ξc0→Ξ−e+νe)/BR(Ξc0→Ξ−π+) in pp collisions at s=13 TeV [Phys. rev. lett. 127, 272001 (2021)]}, volume = {134}, year = {2025}, }
• (2025). Erratum: Evidence for CP violation in B+→pp¯K+ decays [Phys. rev. lett. 113, 141801 (2014)]. PRL, 134(17), 179901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 179901 (2025)}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and et al}, doi = {10.1103/PhysRevLett.134.179901}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {179901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Evidence for CP violation in B+→pp¯K+ decays [Phys. rev. lett. 113, 141801 (2014)]}, volume = {134}, year = {2025}, }
• (2025). Integer defects, flow localization, and bistability on curved active surfaces. PRL, 134(17), 178401. (www)

  @article{ , abstract = {Biological surfaces, such as developing epithelial tissues, exhibit in-plane polar or nematic order and can be strongly curved. Recently, integer ( + 1 ) topological defects have been identified as morphogenetic hotspots in living systems. Yet, while + 1 defects in active matter on flat surfaces are well understood, the general principles governing curved active defects remain unknown. Here, we study the dynamics of integer defects in an extensile or contractile polar fluid on two types of morphogenetically relevant substrates: (i) a cylinder terminated by a spherical cap, and (ii) a bump on an otherwise flat surface. Because the Frank elastic energy on a curved surface generically induces a coupling to deviatoric curvature, D (difference between squared principal curvatures), a + 1 defect is induced on both surface types. We find that D leads to surprising effects including localization of orientation gradients and active flows, and particularly for contractility, to hysteresis and bistability between quiescent and flowing defect states.}, archive = {J_PRL}, author = {Rushikesh Shinde and Raphaël Voituriez and Andrew Callan-Jones}, doi = {10.1103/PhysRevLett.134.178401}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {178401}, shortjournal = {Phys. Rev. Lett.}, title = {Integer defects, flow localization, and bistability on curved active surfaces}, volume = {134}, year = {2025}, }
• (2025). Self-organization and memory in a disordered solid subject to random driving. PRL, 134(17), 178203. (www)

  @article{ , abstract = {We consider self-organization and memory formation in a mesoscopic model of an amorphous solid subject to a protocol of random shear confined to a strain range ± ϵ max . We develop proper readout protocols to show that the response of the driven system self-organizes to retain a memory of the strain range, which can be subsequently retrieved. Our findings generalize previous results obtained upon oscillatory driving and suggest that self-organization and memory formation of disordered materials can emerge under more general conditions, such as a disordered system interacting with its fluctuating environment. Self-organization results in a correlation between the dynamics of the system and its environment, providing thereby an elementary mechanism for sensing. We conclude by discussing our results and their potential relevance for the adaptation of simple organisms lacking a brain to changing environments.}, archive = {J_PRL}, author = {Muhittin Mungan and Dheeraj Kumar and Sylvain Patinet and Damien Vandembroucq}, doi = {10.1103/PhysRevLett.134.178203}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {178203}, shortjournal = {Phys. Rev. Lett.}, title = {Self-organization and memory in a disordered solid subject to random driving}, volume = {134}, year = {2025}, }
• (2025). Heterogeneous dynamics in shear thickening colloids revealed by intrinsic heterodyne correlation spectroscopy. PRL, 134(17), 178202. (www)

  @article{ , abstract = {Shear induced frictional networks have been proposed to be responsible for the emergence of discontinuous shear thickening (DST) in complex fluids. However, little experimental evidence exists to support this model directly. Here, using x-ray photon correlation spectroscopy (XPCS), we show the existence of an intrinsic heterodyne feature during shear cessation, which originates from the relative motion of mobile particles against an aggregated or jammed network induced by shear thickening. Upon removing the shear, the shear stress dissipates rather quickly in a two-step fashion, whereas the heterogeneous particle dynamics persist much longer with the relative velocity decaying slowly with time as . More importantly, both continuous shear thickening (CST) and DST show similar heterodyne features, indicating the intrinsic mechanisms causing shear thickening are similar in nature.}, archive = {J_PRL}, author = {James P. Horwath and Hongrui He and Jonghun Lee and Zhang Jiang and Suman Chakraborty and Qingteng Zhang and Eric M. Dufresne and Mark Sutton and Alec Sandy and Suresh Narayanan and Xiao-Min Lin}, doi = {10.1103/PhysRevLett.134.178202}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {178202}, shortjournal = {Phys. Rev. Lett.}, title = {Heterogeneous dynamics in shear thickening colloids revealed by intrinsic heterodyne correlation spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Long-range angular correlations of particle displacements at a plastic-to-elastic transition in jammed amorphous solids. PRL, 134(17), 178201. (www)

  @article{ , abstract = {Understanding how a fluid turns into an amorphous solid is a fundamental challenge in statistical physics, during which no apparent structural ordering appears. In the athermal limit, the two states are connected by a well-defined jamming transition, near which the solid is marginally stable. A recent mechanical response screening theory proposes an additional transition above jamming, called a plastic-to-elastic transition here, separating anomalous and quasielastic mechanical behavior. Through numerical inflation simulations in two dimensions, we show that the onsets of long-range radial and angular correlations of particle displacements decouple, occurring, respectively, at the jamming and plastic-to-elastic transitions. The latter is characterized by a power-law diverging correlation angle and a power-law spectrum of the displacements along a circle. This work establishes two-step transitions on the mechanical properties during “decompression melting” of an athermal overjammed amorphous solid, reminiscent of the two-step structural melting of a crystal in two dimensions. In contradistinction with the latter, the plastic-to-elastic transition exists also in three dimensions.}, archive = {J_PRL}, author = {Yang Fu and Yuliang Jin and Deng Pan and Itamar Procaccia}, doi = {10.1103/PhysRevLett.134.178201}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {178201}, shortjournal = {Phys. Rev. Lett.}, title = {Long-range angular correlations of particle displacements at a plastic-to-elastic transition in jammed amorphous solids}, volume = {134}, year = {2025}, }
• (2025). Critical clusters in liquid crystals: Fractal geometry and conformal invariance. PRL, 134(17), 178101. (www)

  @article{ , abstract = {We study the two-dimensional domain morphology of twisted nematic liquid crystals during their phase-ordering kinetics [R. A. L. Almeida, Phys. Rev. Lett. 131 , 268101 (2023) ], which is a physical candidate to self-generate critical clusters in the percolation universality class. Here, we present experimental evidence that large clusters and their hulls are indeed both fractals with dimensions of the corresponding figures in critical percolation models. The asymptotic decay of a crossing probability, from a region in the vicinity of the origin to the boundary of disks, is described by the Lawler-Schramm-Werner theorem provided that a microscopic length in the original formulation is replaced by the coarsening length of the liquid crystal. Furthermore, the behavior for the winding angle of large loops is, at certain scales, compatible with that of Schramm-Loewner evolution curves with diffusivity κ = 6 . These results show an experimental realization of critical clusters in phase ordering.}, archive = {J_PRL}, author = {Renan A. L. Almeida and Jeferson J. Arenzon}, doi = {10.1103/PhysRevLett.134.178101}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {178101}, shortjournal = {Phys. Rev. Lett.}, title = {Critical clusters in liquid crystals: Fractal geometry and conformal invariance}, volume = {134}, year = {2025}, }
• (2025). Quantum delocalization enables water dissociation on ru(0001). PRL, 134(17), 178001. (www)

  @article{ , abstract = {We revisit the long-standing question of whether water molecules dissociate on the Ru(0001) surface through nanosecond-scale path-integral molecular dynamics simulations on a sizable supercell. This is made possible through the development of an efficient and reliable machine-learning potential with near first-principles accuracy, overcoming the limitations of previous ab initio studies. We show that the quantum delocalization associated with nuclear quantum effects enables rapid and frequent proton transfers between water molecules, thereby facilitating the water dissociation on Ru(0001). This work provides the direct theoretical evidence of water dissociation on Ru(0001), resolving the enduring issue in surface sciences and offering crucial atomistic insights into water-metal interfaces.}, archive = {J_PRL}, author = {Yu Cao and Jiantao Wang and Mingfeng Liu and Yan Liu and Hui Ma and Cesare Franchini and Yan Sun and Georg Kresse and Xing-Qiu Chen and Peitao Liu}, doi = {10.1103/PhysRevLett.134.178001}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {178001}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum delocalization enables water dissociation on ru(0001)}, volume = {134}, year = {2025}, }
• (2025). Statistical mechanics of transfer learning in fully connected networks in the proportional limit. PRL, 134(17), 177301. (www)

  @article{ , abstract = {Transfer learning (TL) is a well-established machine learning technique to boost the generalization performance on a specific (target) task using information gained from a related (source) task, and it crucially depends on the ability of a network to learn useful features. Leveraging recent analytical progress in the proportional regime of deep learning theory (i.e., the limit where the size of the training set and the size of the hidden layers are taken to infinity keeping their ratio finite), in this Letter we develop a novel single-instance Franz-Parisi formalism that yields an effective theory for TL in fully connected neural networks. Unlike the (lazy-training) infinite-width limit, where TL is ineffective, we demonstrate that in the proportional limit TL occurs due to a renormalized source-target kernel that quantifies their relatedness and determines whether TL is beneficial for generalization.}, archive = {J_PRL}, author = {Alessandro Ingrosso and Rosalba Pacelli and Pietro Rotondo and Federica Gerace}, doi = {10.1103/PhysRevLett.134.177301}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {177301}, shortjournal = {Phys. Rev. Lett.}, title = {Statistical mechanics of transfer learning in fully connected networks in the proportional limit}, volume = {134}, year = {2025}, }
• (2025). Contrasting light-induced spin torque in antiferromagnetic and altermagnetic systems. PRL, 134(17), 176902. (www)

  @article{ , abstract = {Light-matter interaction has become one of the promising routes to manipulating various physical features of quantum materials in an ultrafast kinetics. In this Letter, we focus on the nonlinear optical effects of the spintronic behavior in antiferromagnetic (AFM) and altermagnetic (AM) systems with compensated magnetic moments, which has been extensively attractive for their potential applications. With vanishing net magnetic moments, one of the main concerns is how to distinguish and disentangle AFMs and AMs in experiments, as they usually behave similarly in many susceptibility measurements. To address this challenge, we propose that linearly polarized light could trigger contrasting nonequilibrium local spin torques in these systems, unraveling hidden light-induced spintronic behaviors. In general, one could achieve light-induced spin canting in AMs, but only Néel vector torques in AFMs. We scrutinize and enumerate their symmetry constraints of all 122 magnetic point groups. We also adopt low energy Hamiltonian models and first-principles calculations on two representative materials to illustrate our theory. Our work provides a new perspective for the design and optimization of spintronic devices.}, archive = {J_PRL}, author = {Jian Zhou and Chunmei Zhang}, doi = {10.1103/PhysRevLett.134.176902}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176902}, shortjournal = {Phys. Rev. Lett.}, title = {Contrasting light-induced spin torque in antiferromagnetic and altermagnetic systems}, volume = {134}, year = {2025}, }
• (2025). Collective optical properties of moiré excitons. PRL, 134(17), 176901. (www)

  @article{ , abstract = {We propose that excitons in moiré transition metal dichalcogenide bilayers offer a promising platform for investigating collective radiative properties. While some of these optical properties resemble those of cold atom arrays, moiré excitons extend to the deep subwavelength limit, beyond the reach of current optical lattice experiments. Remarkably, we show that the collective optical properties can be exploited to probe certain correlated electron states without requiring subwavelength spatial resolution. Specifically, we illustrate that the Wigner crystal states of electrons doped into these bilayers act as an emergent periodic potential for excitons. Moreover, the collective dissipative excitonic bands and their associated Berry curvature can reveal various charge orders that emerge at the corresponding electronic doping. Our Letter provides a promising pathway for future research on the interplay between collective effects and strong correlations involving moiré excitons.}, archive = {J_PRL}, author = {Tsung-Sheng Huang and Yu-Xin Wang (王语馨 and Yan-Qi Wang and Darrick Chang and Mohammad Hafezi and Andrey Grankin}, doi = {10.1103/PhysRevLett.134.176901}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176901}, shortjournal = {Phys. Rev. Lett.}, title = {Collective optical properties of moiré excitons}, volume = {134}, year = {2025}, }
• (2025). Adiabatic pumping of orbital magnetization by spin precession. PRL, 134(17), 176702. (www)

  @article{ , abstract = {We propose adiabatic pumping of orbital magnetization driven by coherent spin precession, which enables rectification by converting periodic oscillations into a static signal. The orbital magnetization originates from the adiabatic evolution of valence electrons with a topological bulk contribution expressed as a Chern-Simons form. When the precession cone angle of spin is small, the resulting magnetization is proportional to and contributes to the magnon Zeeman effect, the energy shift induced by a magnetic field. With a large cone angle, the magnetization can reach its natural unit, in an antiferromagnetic topological insulator with as the elementary charge and as the precession period. This significant magnetization is related to the global properties of the electronic geometric phases in the parameter space spanned by and momentum . When the pumped magnetization is inhomogeneous, induced by spin textures or electronic topological phase domains, a dissipationless charge current is also pumped. At last, we discuss the boundary contributions from the spin-driving edge states, which are intricately linked to the gauge-dependent quantum uncertainty of the Chern-Simons form.}, archive = {J_PRL}, author = {Yafei Ren and Wenqin Chen and Chong Wang and Ting Cao and Di Xiao}, doi = {10.1103/PhysRevLett.134.176702}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176702}, shortjournal = {Phys. Rev. Lett.}, title = {Adiabatic pumping of orbital magnetization by spin precession}, volume = {134}, year = {2025}, }
• (2025). Current-driven collective control of helical spin texture in van der waals antiferromagnet. PRL, 134(17), 176701. (www)

  @article{ , abstract = {Electrical control of quantum magnetic states is essential in spintronic science. Initial studies on the ferromagnetic state control were extended to collinear antiferromagnets and, more recently, noncollinear antiferromagnets. However, electrical control mechanisms of such exotic magnetic states remain poorly understood. Here, we report the first experimental and theoretical example of the current control of helical antiferromagnets, arising from the competition between collinear antiferromagnetic exchange and interlayer Dzyaloshinskii-Moriya interaction in new van der Waals (vdW) material . Due to the intrinsic broken inversion symmetry, an in-plane current generates spin-orbit torque that, in turn, interacts directly with the helical antiferromagnetic order. Our theoretical analyses indicate that a weak ferromagnetic order coexists due to the Dzyaloshinskii-Moriya interaction, mediating the spin-orbit torque to collectively rotate the helical antiferromagnetic order. Our nanodevice experiments produce current-dependent resistance change consistent with the theoretical prediction. This Letter widens our understanding of the electrical control of helical antiferromagnets and promotes vdW quantum magnets as interesting material platforms for electrical control.}, archive = {J_PRL}, author = {Kai-Xuan Zhang and Suik Cheon and Hyuncheol Kim and Pyeongjae Park and Yeochan An and Suhan Son and Jingyuan Cui and Jihoon Keum and Joonyoung Choi and Younjung Jo and Hwiin Ju and Jong-Seok Lee and Youjin Lee and Maxim Avdeev and Armin Kleibert and Hyun-Woo Lee and Je-Geun Park}, doi = {10.1103/PhysRevLett.134.176701}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176701}, shortjournal = {Phys. Rev. Lett.}, title = {Current-driven collective control of helical spin texture in van der waals antiferromagnet}, volume = {134}, year = {2025}, }
• (2025). Emergence of ferroelectric topological insulator as verified by quantum hall effect of surface states in (Sn,Pb,In)Te films. PRL, 134(17), 176602. (www)

  @article{ , abstract = {Emergent phenomena arising from nontrivial band structures based on topology and symmetry have been attracting keen interest in contemporary condensed-matter physics. Materials such as SnTe and PbTe are one such example, which demonstrate a topological phase transition while showing ferroelectric instability derived from their rock-salt structure. The ferroelectricity can lift the valley degeneracy, enabling the emergence of the topological insulator phase, although its observation in transport phenomena remains elusive. Here, we report magnetotransport properties of ferroelectric (Sn, Pb)Te thin films with finely controlled Fermi levels via In doping. We identified the ferroelectric topological insulator phase from the observations of the quantum Hall states with filling factors of , 2, and 3 with both spin- and valley-degeneracy lifting. The electronic states are two-dimensional, indicating the ferroelectricity-induced topological surface states with a single Dirac cone. The finding of the new topological state with ferroelectricity will further expand the field of topological physics and advance the development of functional properties, such as topological nonlinear photonics and nonreciprocal transport with memory effect.}, archive = {J_PRL}, author = {Ryutaro Yoshimi and Ryosuke Kurihara and Yoshihiro Okamura and Hikaru Handa and Naoki Ogawa and Minoru Kawamura and Atsushi Tsukazaki and Kei S. Takahashi and Masashi Kawasaki and Youtarou Takahashi and Masashi Tokunaga and Yoshinori Tokura}, doi = {10.1103/PhysRevLett.134.176602}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176602}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of ferroelectric topological insulator as verified by quantum hall effect of surface states in (Sn,Pb,In)Te films}, volume = {134}, year = {2025}, }
• (2025). Hybrid-order skin effect from loss-induced nonreciprocity. PRL, 134(17), 176601. (www)

  @article{ , abstract = {Skin effects, the phenomena of the bulk states collapsing toward open boundaries, have mostly been revealed in non-Hermitian systems hosting nonreciprocity. Either the first-order or the higher-order of skin effects have been observed. Here, we report our first discovery of a hybrid-order of skin effects, of which the utilized two-dimensional system exhibits not only the first-order skin modes, but also the second-order skin modes respectively on the edges and the corners, the different type of open boundaries. We propose a universal approach to achieving nonreciprocal couplings by virtue of the loss and bilayer degree of freedom, as the critical role it plays. Our models are implemented in square- and diamond-shaped phononic crystals, and the hybrid order of acoustic skin modes is evidenced in experiment. Our Letter may foster the development of non-Hermitian physics.}, archive = {J_PRL}, author = {Jien Wu and Yejian Hu and Zhaojian He and Ke Deng and Xueqin Huang and Manzhu Ke and Weiyin Deng and Jiuyang Lu and Zhengyou Liu}, doi = {10.1103/PhysRevLett.134.176601}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176601}, shortjournal = {Phys. Rev. Lett.}, title = {Hybrid-order skin effect from loss-induced nonreciprocity}, volume = {134}, year = {2025}, }
• (2025). Describing landau level mixing in fractional quantum hall states with deep learning. PRL, 134(17), 176503. (www)

  @article{ , abstract = {Strong correlation brings a rich array of emergent phenomena, as well as a daunting challenge to theoretical physics study. In condensed matter physics, the fractional quantum Hall effect is a prominent example of strong correlation, with Landau level mixing being one of the most challenging aspects to address using traditional computational methods. Deep learning real-space neural network wave function methods have emerged as promising architectures to describe electron correlations in molecules and materials, but their power has not been fully tested for exotic quantum states. In this work, we employ real-space neural network wave function techniques to investigate fractional quantum Hall systems. On both and filling systems, we achieve energies consistently lower than exact diagonalization results which only consider the lowest Landau level. We also demonstrate that the real-space neural network wave function can naturally capture the extent of Landau level mixing up to a very high level, overcoming the limitations of traditional methods. Our work underscores the potential of neural networks for future studies of strongly correlated systems and opens new avenues for exploring the rich physics of the fractional quantum Hall effect.}, archive = {J_PRL}, author = {Yubing Qian and Tongzhou Zhao and Jianxiao Zhang and Tao Xiang and Xiang Li and Ji Chen}, doi = {10.1103/PhysRevLett.134.176503}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176503}, shortjournal = {Phys. Rev. Lett.}, title = {Describing landau level mixing in fractional quantum hall states with deep learning}, volume = {134}, year = {2025}, }
• (2025). Taming spin susceptibilities in frustrated quantum magnets: Mean-field form and approximate nature of the quantum-to-classical correspondence. PRL, 134(17), 176502. (www)

  @article{ , abstract = {In frustrated magnetism, the empirically found quantum-to-classical correspondence (QCC) matches the real-space static susceptibility pattern of a quantum spin- model with its classical counterpart computed at a certain elevated temperature. This puzzling relation was observed via bold line diagrammatic Monte Carlo simulations in dimensions two and three. The matching was within error bars and seemed valid down to the lowest accessible temperatures about an order of magnitude smaller than the exchange coupling . Here, we employ resummed spin diagrammatic perturbation theory to show analytically that the QCC breaks weakly at fourth order in and provide the approximate mapping between classical and quantum temperatures. Our treatment further reveals that QCC is an indication of the surprising accuracy with which static correlators can be approximated by a simple renormalized mean-field form. We illustrate this for all models discussed in the context of QCC so far, including a recent example of the material . The success of the mean-field form is traced back to partial diagrammatic cancellations.}, archive = {J_PRL}, author = {Benedikt Schneider and Björn Sbierski}, doi = {10.1103/PhysRevLett.134.176502}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176502}, shortjournal = {Phys. Rev. Lett.}, title = {Taming spin susceptibilities in frustrated quantum magnets: Mean-field form and approximate nature of the quantum-to-classical correspondence}, volume = {134}, year = {2025}, }
• (2025). Compressible quantum liquid with vanishing drude weight. PRL, 134(17), 176501. (www)

  @article{ , abstract = {We explore the possibility of quantum liquids that are compressible but have vanishing dc conductivity in the absence of disorder. We show that the composite Fermi liquid emerging from strong interaction in a generic Chern band has zero Drude weight, in stark contrast to normal Fermi liquids. Our Letter establishes the absence of Drude weight as the defining property of the composite Fermi liquid phase, which distinguishes it from the Fermi liquid or other types of non-Fermi liquids. Our findings point to a possibly wide class of gapless quantum phases with unexpected transport and optical properties.}, archive = {J_PRL}, author = {Ahmed Abouelkomsan and Nisarga Paul and Ady Stern and Liang Fu}, doi = {10.1103/PhysRevLett.134.176501}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176501}, shortjournal = {Phys. Rev. Lett.}, title = {Compressible quantum liquid with vanishing drude weight}, volume = {134}, year = {2025}, }
• (2025). Spin-transfer torque in altermagnets with magnetic textures. PRL, 134(17), 176401. (www)

  @article{ , abstract = {We predict the existence of anisotropic spin-transfer torque effect in textured altermagnets. To this end, we generalize the Zhang-Li torque to incorporate the symmetry associated with prototypical 𝑑 -wave altermagnets and identify the spin-splitter adiabatic and nonadiabatic torques. Applying our results to domain wall dynamics induced by spin-transfer torque, we find that, in certain regimes, the spin-splitter adiabatic torque can induce domain wall precession, significantly slowing down domain wall motion. The response of the domain wall also becomes anisotropic, reflecting the 𝑑 -wave symmetry of the altermagnet. Furthermore, we observe that the spin-splitter adiabatic torque modifies skyrmion dynamics, inducing anisotropic skyrmion Hall effect. The above phenomena can serve as a hallmark of altermagnetism in textured magnets, distinguishing it from the behavior of ordinary antiferromagnets.}, archive = {J_PRL}, author = {Hamed Vakili and Edward Schwartz and Alexey A. Kovalev}, doi = {10.1103/PhysRevLett.134.176401}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176401}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-transfer torque in altermagnets with magnetic textures}, volume = {134}, year = {2025}, }
• (2025). Unified one-parameter scaling function for anderson localization transitions in nonreciprocal non-hermitian systems. PRL, 134(17), 176301. (www)

  @article{ , abstract = {Using dimensionless conductances as scaling variables, the conventional one-parameter scaling theory of localization fails for nonreciprocal non-Hermitian systems such as the Hatano-Nelson model. Here, we propose a one-parameter scaling function using the participation ratio as the scaling variable. Employing a highly accurate numerical procedure based on exact diagonalization, we demonstrate that this one-parameter scaling function can describe Anderson localization transitions of nonreciprocal non-Hermitian systems in one and two dimensions of symmetry classes AI and A. The critical exponents of correlation lengths depend on symmetries and dimensionality only, a typical feature of universality. Then, we derive a complex-gap equation based on the self-consistent Born approximation to determine the critical disorder at which the point gap closes. The obtained critical disorders perfectly match those given by the one-parameter scaling function. Moreover, we propose a one-parameter function that can describe the critical properties of such Anderson localization transitions. Finally, we show that the one-parameter scaling function is also valid for Anderson localization transitions in reciprocal non-Hermitian systems such as the two-dimensional class and can, thus, serve as a unified scaling function for disordered non-Hermitian systems.}, archive = {J_PRL}, author = {C. Wang and Wenxue He and X. R. Wang and Hechen Ren}, doi = {10.1103/PhysRevLett.134.176301}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176301}, shortjournal = {Phys. Rev. Lett.}, title = {Unified one-parameter scaling function for anderson localization transitions in nonreciprocal non-hermitian systems}, volume = {134}, year = {2025}, }
• (2025). Interplay between interface diffusion and boundary slip underlying graphite-lubricated metal nanoforming. PRL, 134(17), 176204. (www)

  @article{ , abstract = {By designing carbon nanotube based nanochannels and exploiting the recent developed thermomechanical nanomolding technique, we reveal that the interface diffusion and boundary slip mechanisms play a key role in metal nanoforming. The former dominates the matter transport at the atomic scale and is significantly affected by surface defects, while the latter is closely related to the flow units at the continuum scale, and more sensitive to the apparent interfacial adhesion work than atomic scale defects. In particular, the excellent lubrication of graphitic materials maintained at high temperatures and in air is uncovered from the defect-insensitive boundary slip mechanism. Our findings not only clarify the fundamental physical processes behind metal nanoforming, but also provide new insights into nanofriction and lubrication.}, archive = {J_PRL}, author = {Jun-Xiang Xiang and Yuanpeng Yao and Hui Fang and Cai Lu and Ze Liu}, doi = {10.1103/PhysRevLett.134.176204}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176204}, shortjournal = {Phys. Rev. Lett.}, title = {Interplay between interface diffusion and boundary slip underlying graphite-lubricated metal nanoforming}, volume = {134}, year = {2025}, }
• (2025). Substrate polarization alters the jahn-teller effect in a single molecule. PRL, 134(17), 176203. (www)

  @article{ , abstract = {Charge-state transitions of a single Cu-phthalocyanine molecule adsorbed on an insulating layer of NaCl on Cu(111) are probed by means of alternate charging scanning tunneling microscopy. Real-space imaging of the electronic transitions reveals the Jahn-Teller distortion occurring upon formation of the first and second anionic charge states. The experimental findings are rationalized by a theoretical many-body model that highlights the crucial role played by the substrate. The latter enhances and stabilizes the intrinsic Jahn-Teller distortion of the negatively charged molecule hosting a degenerate pair of single-particle frontier orbitals. Consequently, two excess electrons are found to occupy, in the ground state, the same localized orbital, despite a larger Coulomb repulsion than the one for the competing delocalized electronic configuration. Control over the charging sequence by varying the applied bias voltage is also predicted.}, archive = {J_PRL}, author = {Moritz Frankerl and Laerte L. Patera and Felix Giselbrecht and Thomas Frederiksen and Jascha Repp and Andrea Donarini}, doi = {10.1103/PhysRevLett.134.176203}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176203}, shortjournal = {Phys. Rev. Lett.}, title = {Substrate polarization alters the jahn-teller effect in a single molecule}, volume = {134}, year = {2025}, }
• (2025). Decrease of static friction coefficient with interface growth from single to multiasperity contact. PRL, 134(17), 176202. (www)

  @article{ , abstract = {The key parameter for describing frictional strength at the onset of sliding is the static friction coefficient. Yet, how the static friction coefficient emerges at the macroscale from contacting asperities at the microscale is still an open problem. Here, we present friction experiments in which the normal load was varied over more than 3 orders of magnitude, so that a transition from a single asperity contact at low loads to multiasperity contacts at high loads was achieved. We find a remarkable reduction in the friction drop (the ratio of the static friction force to the dynamic friction force) with increasing normal load. Using a simple stick-slip transition model we identify the presence of presliding and subcritical contact points as the cause of smaller static friction coefficient at increased normal loads. Our measurements and model bridge the gap between friction behavior commonly observed in atomic force microscopy experiments at microscopic forces, and industrially relevant multiasperity contact interfaces loaded with macroscopic forces.}, archive = {J_PRL}, author = {Liang Peng and Thibault Roch and Daniel Bonn and Bart Weber}, doi = {10.1103/PhysRevLett.134.176202}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176202}, shortjournal = {Phys. Rev. Lett.}, title = {Decrease of static friction coefficient with interface growth from single to multiasperity contact}, volume = {134}, year = {2025}, }
• (2025). Site-selective polar compensation of mott electrons in a double-perovskite heterointerface. PRL, 134(17), 176201. (www)

  @article{ , abstract = {Double-perovskite oxides (DPOs) with two transition metal ions ( ) offer a fascinating platform for exploring exotic physics and practical applications. Studying these DPOs as ultrathin epitaxial films on single crystalline substrates can add another dimension to engineering electronic, magnetic, and topological phenomena. Understanding the consequence of polarity mismatch between the substrate and the DPO would be the first step toward this broad goal. We investigate this by studying the interface between a prototypical insulating DPO and a wide band gap insulator . The interface is found to be insulating in nature. By combining several experimental techniques and density functional theory, we establish a site-selective charge compensation process that occurs explicitly at the Mn site of the film, leaving the Ni sites inert. We further demonstrate that such surprising selectivity, which cannot be explained by existing mechanisms of polarity compensation, is directly associated with their electronic correlation energy scales. This study establishes the crucial role of Mott physics in polar compensation process and paves the way for designer doping strategies in complex oxides.}, archive = {J_PRL}, author = {Nandana Bhattacharya and Arpita Sen and Ke Qu and Arijit Sinha and Ranjan Kumar Patel and Siddharth Kumar and Jianwei Zhang and Prithwijit Mandal and Suresh Chandra Joshi and Shashank Kumar Ojha and Jyotirmay Maity and Zhan Zhang and Hua Zhou and Fanny Rodolakis and Padraic Shafer and Christoph Klewe and John William Freeland and Zhenzhong Yang and Umesh Waghmare and Srimanta Middey}, doi = {10.1103/PhysRevLett.134.176201}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176201}, shortjournal = {Phys. Rev. Lett.}, title = {Site-selective polar compensation of mott electrons in a double-perovskite heterointerface}, volume = {134}, year = {2025}, }
• (2025). Isostructural phase transition of Fe2O3 under laser shock compression. PRL, 134(17), 176102. (www)

  @article{ , abstract = {We present in situ x-ray diffraction and velocity measurements of under laser shock compression at pressures between 38–122 GPa. None of the high-pressure phases reported by static compression studies were observed. Instead, we observed an isostructural phase transition from to a new phase at a pressure of 50–62 GPa. The phase differs from by an 11% volume drop and a different unit cell compressibility. We further observed a two-wave structure in the velocity profile, which can be related to an intermediate regime where both and phases coexist. Density functional theory calculations with a Hubbard parameter indicate that the observed unit cell volume drop can be associated with a spin transition following a magnetic collapse.}, archive = {J_PRL}, author = {A. Amouretti and C. Crépisson and S. Azadi and F. Brisset and D. Cabaret and T. Campbell and D. A. Chin and G. W. Collins and L. Hansen and G. Fiquet and A. Forte and T. Gawne and F. Guyot and P. Heighway and E. Heriprë and E. Cunningham and H. J. Lee and D. McGonegle and B. Nagler and J. Pintor and D. N. Polsin and G. Rousse and Y. Shi and E. Smith and J. S. Wark and S. M. Vinko and M. Harmand}, doi = {10.1103/PhysRevLett.134.176102}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176102}, shortjournal = {Phys. Rev. Lett.}, title = {Isostructural phase transition of Fe2O3 under laser shock compression}, volume = {134}, year = {2025}, }
• (2025). Strongly hybridized phonons in one-dimensional van der waals crystals. PRL, 134(17), 176101. (www)

  @article{ , abstract = {The phenomena of pronounced electron-electron and electron-phonon interactions in one-dimensional (1D) systems are ubiquitous, which are well described by frameworks of Luttinger liquid, Peierls instability, and concomitant charge density wave. However, the experimental observation of strongly hybridized phonons in 1D was not demonstrated. Herein we report the first observation of strongly hybridized phonons in 1D condensed matters by using double-walled carbon nanotubes (DWNTs), representative 1D van der Waals crystals, by combining the spectroscopic and microscopic tools as well as the ab initio density functional theory (DFT) calculations. We observe uncharted phonon modes in one commensurate and three incommensurate DWNT crystals, three of which concurrently exhibit strongly reconstructed electronic band structures. Our DFT calculations for the experimentally observed commensurate DWNT (7, 7) @ (12, 12) reveal that this new phonon mode originates from a (nearly) degenerate coupling between two transverse acoustic modes (ZA modes) of constituent inner and outer nanotubes having approximately trigonal and pentagonal rotational symmetry along the nanotube circumferences. Such coupling strongly hybridizes the two phonon modes in different shells and leads to the formation of a unique lattice motion featuring evenly distributed vibrational amplitudes over inner and outer nanotubes, distinct from any known phonon modes in 1D systems. All four DWNTs that exhibit the pronounced new phonon modes show small chiral angle twists, closely matched diameter ratios of 3 5 and decreased frequencies of new phonon modes with increased diameters, all supporting the uncovered coupling mechanism. Our discovery of strongly hybridized phonons in DWNTs opens new opportunities for engineering phonons and exploring novel phonon-related phenomena in 1D condensed matters.}, archive = {J_PRL}, author = {Shaoqi Sun and Qingyun Lin and Yihuan Li and Daichi Kozawa and Huizhen Wu and Shigeo Maruyama and Pilkyung Moon and Toshikaze Kariyado and Ryo Kitaura and Sihan Zhao}, doi = {10.1103/PhysRevLett.134.176101}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176101}, shortjournal = {Phys. Rev. Lett.}, title = {Strongly hybridized phonons in one-dimensional van der waals crystals}, volume = {134}, year = {2025}, }
• (2025). Quantum geometric kohn-luttinger superconductivity. PRL, 134(17), 176001. (www)

  @article{ , abstract = {Coulomb repulsion can, counterintuitively, mediate Cooper pairing via the Kohn-Luttinger mechanism. However, it is commonly believed that observability of the effect requires special circumstances, e.g., vicinity of the Fermi level to Van Hove singularities, significant lattice-induced band distortions, or nontrivial Fermi surface topologies. Here, we establish that quantum geometric properties of the constituent electrons can dramatically promote pairing from repulsion via dependence of screening on the quantum metric. We demonstrate quantum-geometry-enhanced superconductivity in two microscopic models with tunable quantum geometry, highlighting the crucial roles of quantum metric anisotropy and inhomogeneity. Our analysis provides an experimentally accessible figure of merit for the importance of quantum geometry to inducing unconventional superconductivity, indicating its relevance to graphene multilayers.}, archive = {J_PRL}, author = {Gal Shavit and Jason Alicea}, doi = {10.1103/PhysRevLett.134.176001}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {176001}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum geometric kohn-luttinger superconductivity}, volume = {134}, year = {2025}, }
• (2025). Nonperturbative guiding center model for magnetized plasmas. PRL, 134(17), 175101. (www)

  @article{ , abstract = {Perturbative guiding center theory adequately describes the slow drift motion of charged particles in the strongly magnetized regime characteristic of thermal particle populations in various magnetic fusion devices. However, it breaks down for particles with large-enough energy. We report on a data-driven method for learning a nonperturbative guiding center model from full-orbit particle simulation data. We show the data-driven model significantly outperforms traditional asymptotic theory in magnetization regimes appropriate for fusion-born particles in stellarators, thus opening the door to nonperturbative guiding center calculations.}, archive = {J_PRL}, author = {J. W. Burby and I. A. Maldonado and M. Ruth and D. A. Messenger and L. Carbajal}, doi = {10.1103/PhysRevLett.134.175101}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {175101}, shortjournal = {Phys. Rev. Lett.}, title = {Nonperturbative guiding center model for magnetized plasmas}, volume = {134}, year = {2025}, }
• (2025). Effects of retardation on many-body superradiance in chiral waveguide QED. PRL, 134(17), 173601. (www)

  @article{ , abstract = {We study the superradiant decay of a chain of atoms coupled to a chiral waveguide, focusing on the regime of non-negligible photon propagation time. Using an exact master equation description that accounts for delay effects, we obtain evidence to suggest that competition between collective decay and retardation leads to the emergence of an effective maximum number of atoms able to contribute to the superradiant dynamics, resulting in a plateau of the peak emission rate. To develop this analysis further, we investigate the interatomic correlations to find features consistent with the formation of individual superradiant domains. Moreover, we find that retardation can also result in persistent oscillatory atomic dynamics accompanied by a periodic sequence of emission bursts.}, archive = {J_PRL}, author = {Bennet Windt and Miguel Bello and Daniel Malz and J. Ignacio Cirac}, doi = {10.1103/PhysRevLett.134.173601}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {173601}, shortjournal = {Phys. Rev. Lett.}, title = {Effects of retardation on many-body superradiance in chiral waveguide QED}, volume = {134}, year = {2025}, }
• (2025). Ultralow qβ value for the allowed decay of ag110m confirmed via mass measurements. PRL, 134(17), 172501. (www)

  @article{ , abstract = {The mass of the electron-antineutrino can be determined in dedicated measurements of the spectral shape near the end point of a transition, with a low value enhancing the sensitivity of the measurement. One such low value candidate is the transition between the isomer of and the state in ( ). To reduce the uncertainty of the value, we have used the phase-imaging ion-cyclotron-resonance technique with the JYFLTRAP double Penning trap and performed a high-precision atomic mass measurement of with as a reference. Combined with the known spectroscopic data, we obtain a reevaluated value for the transition. This represents the lowest value for any allowed transition observed to date. In order to estimate the partial half-life ( ) and branching ratio (Br) of the transition, nuclear shell model calculations were performed using the Hamiltonian in combination with state-of-the-art atomic calculations. The computed values of and , along with the thermal-neutron capture on stable as a viable production method, make a promising candidate for future antineutrino mass measurements.}, archive = {J_PRL}, author = {J. Ruotsalainen and M. Stryjczyk and M. Ramalho and T. Eronen and Z. Ge and A. Kankainen and M. Mougeot and J. Suhonen}, doi = {10.1103/PhysRevLett.134.172501}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {172501}, shortjournal = {Phys. Rev. Lett.}, title = {Ultralow qβ value for the allowed decay of ag110m confirmed via mass measurements}, volume = {134}, year = {2025}, }
• (2025). Heavy-flavor angular correlations as a direct probe of the glasma. PRL, 134(17), 172301. (www)

  @article{ , abstract = {We use classical equations of motion for heavy quarks to show that the preequilibrium glasma phase of a heavy ion collision has an extremely strong effect on heavy quark angular correlations. At the same time the effect on the single inclusive spectrum is much more moderate. This suggests that meson angular correlations in future LHC measurements could provide a direct experimental access to the physics of the preequilibrium stage.}, archive = {J_PRL}, author = {Dana Avramescu and Vincenzo Greco and Tuomas Lappi and Heikki Mäntysaari and David Müller}, doi = {10.1103/PhysRevLett.134.172301}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {172301}, shortjournal = {Phys. Rev. Lett.}, title = {Heavy-flavor angular correlations as a direct probe of the glasma}, volume = {134}, year = {2025}, }
• (2025). Lattice QCD study of pion electroproduction and weak production from a nucleon. PRL, 134(17), 171904. (www)

  @article{ , abstract = {Quantum fluctuations in QCD influence nucleon structure and interactions, with pion production serving as a key probe of chiral dynamics. In this Letter, we present a lattice QCD calculation of multipole amplitudes at threshold, related to both pion electroproduction and weak production from a nucleon, using two gauge ensembles near the physical pion mass. We develop a technique for spin projection and construct multiple operators for analyzing the generalized eigenvalue problem in both the nucleon-pion system in the center-of-mass frame and the nucleon system with nonzero momentum. The numerical lattice results are then compared with those extracted from experimental data and predicted by low-energy theorems incorporating one-loop corrections.}, archive = {J_PRL}, author = {Yu-Sheng Gao and Zhao-Long Zhang and Xu Feng and Lu-Chang Jin and Chuan Liu and Ulf-G. Meißner}, doi = {10.1103/PhysRevLett.134.171904}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171904}, shortjournal = {Phys. Rev. Lett.}, title = {Lattice QCD study of pion electroproduction and weak production from a nucleon}, volume = {134}, year = {2025}, }
• (2025). Berry curvature and spin-one color superconductivity. PRL, 134(17), 171903. (www)

  @article{ , abstract = {We explore the interplay between Berry curvature and topological properties in single-flavor color superconductors, where quarks form spin-one Cooper pairs. By deriving a new relation, we connect the topological nodal structure of the gap function in momentum space to the (non-Abelian) Berry flux associated with paired quarks. This generalizes the early work by Li and Haldane [ Phys. Rev. Lett. 120 , 067003 (2018) ] to systems with additional internal quantum numbers, such as color. In the ultrarelativistic limit, we uncover rich topological structures driven by the interplay of spin, chirality, and color. Specifically, we identify chirality-induced topological nodes in the transverse (opposite chirality pairing) polar and phases. In contrast, the color-spin-locking phase lacks these nodes due to a nontrivial color Berry flux, which in turn induces gapless excitations with total Berry monopole charges of —differing from conventional Weyl fermions. Our findings can be potentially extended to other fermionic systems carrying additional internal degrees of freedom.}, archive = {J_PRL}, author = {Noriyuki Sogabe and Yi Yin}, doi = {10.1103/PhysRevLett.134.171903}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171903}, shortjournal = {Phys. Rev. Lett.}, title = {Berry curvature and spin-one color superconductivity}, volume = {134}, year = {2025}, }
• (2025). Precision evaluation of the η- and η′-pole contributions to hadronic light-by-light scattering in the anomalous magnetic moment of the muon. PRL, 134(17), 171902. (www)

  @article{ , abstract = {Next to the pole, and intermediate states give rise to the leading singularities of the hadronic light-by-light tensor, resulting in sizable contributions to the anomalous magnetic moment of the muon . The strength of the poles is determined by the respective transition form factors (TFFs) to two (virtual) photons. We present a calculation of these TFFs that implements a number of low- and high-energy constraints, including the decay widths, spectra, chiral symmetry for the amplitudes, vector-meson couplings, and asymptotic limits. Crucially, we investigate the role of the leading left-hand singularity generated by the exchange of the tensor meson, yielding, for the first time, an estimate of the associated factorization-breaking corrections. Our final results, and , conclude a dedicated effort to evaluate the pseudoscalar-pole contributions to hadronic light-by-light scattering using dispersion relations, amounting to a combined .}, archive = {J_PRL}, author = {Simon Holz and Martin Hoferichter and Bai-Long Hoid and Bastian Kubis}, doi = {10.1103/PhysRevLett.134.171902}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171902}, shortjournal = {Phys. Rev. Lett.}, title = {Precision evaluation of the η- and η′-pole contributions to hadronic light-by-light scattering in the anomalous magnetic moment of the muon}, volume = {134}, year = {2025}, }
• (2025). Precise predictions for event shapes in diphoton production at the LHC. PRL, 134(17), 171901. (www)

  @article{ , abstract = {Photon pair production is an important benchmark process at the LHC, entering Higgs boson studies and new physics searches. It has been measured to high accuracy, allowing for detailed studies of event shapes in diphoton final states. To enable precision physics with diphoton event shapes, we compute the second-order QCD corrections, to them and study their phenomenological impact.}, archive = {J_PRL}, author = {Federico Buccioni and Xuan Chen and Wei-Jie Feng and Thomas Gehrmann and Alexander Huss and Matteo Marcoli}, doi = {10.1103/PhysRevLett.134.171901}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171901}, shortjournal = {Phys. Rev. Lett.}, title = {Precise predictions for event shapes in diphoton production at the LHC}, volume = {134}, year = {2025}, }
• (2025). Surface kinematics and the canonical yang-mills all-loop integrand. PRL, 134(17), 171601. (www)

  @article{ , abstract = {It has been a long-standing challenge to define a canonical loop integrand for nonsupersymmetric gluon scattering amplitudes in the planar limit. Naive integrands are inflicted with ambiguities associated with tadpoles and massless external bubbles, which destroy integrand-level gauge invariance as well as consistent on-shell factorization on single loop cuts. In this Letter, we show that this essentially kinematical obstruction to defining “the” integrand for Yang-Mills theory has a structural solution, handed to us by the formulation of gluon amplitudes in terms of curves on surfaces. This defines “surface kinematics” generalizing momenta, making it possible to define the integrand satisfying both a (surface generalized) notion of gauge-invariance and consistent loop cuts. The integrand also vanishes at infinity in appropriate directions, allowing it to be recursively computed for nonsupersymmetric Yang-Mills theory in any number of dimensions. We illustrate these ideas through one loop for all multiplicity, and for the simplest two-loop integrand.}, archive = {J_PRL}, author = {Nima Arkani-Hamed and Qu Cao (曹趣 and Jin Dong (董晋 and Carolina Figueiredo and Song He (何颂}, doi = {10.1103/PhysRevLett.134.171601}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171601}, shortjournal = {Phys. Rev. Lett.}, title = {Surface kinematics and the canonical yang-mills all-loop integrand}, volume = {134}, year = {2025}, }
• (2025). Analytic solution for the motion of spinning particles in kerr spacetime. PRL, 134(17), 171401. (www)

  @article{ , abstract = {The equations of motion of massive test particles near Kerr black holes are separable in Boyer-Lindquist coordinates, as established by Carter. This separability, however, is lost when the particles are endowed with classical spin. We show that separability of the equations of motion can be recovered to linear order in spin by a shift of the worldline derived with the use of the hidden symmetry of Kerr spacetime. Consequently, the closed-form solution of the motion is expressed in a way closely analogous to the solution for spinless particles. This finding enriches the understanding of separability and integrability properties of the dynamics of test particles and fields in Kerr spacetime and is particularly valuable for modeling inspirals of rotating compact objects into massive black holes.}, archive = {J_PRL}, author = {Viktor Skoupý and Vojtěch Witzany}, doi = {10.1103/PhysRevLett.134.171401}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171401}, shortjournal = {Phys. Rev. Lett.}, title = {Analytic solution for the motion of spinning particles in kerr spacetime}, volume = {134}, year = {2025}, }
• (2025). Extended TeV halos may commonly exist around middle-aged pulsars. PRL, 134(17), 171005. (www)

  @article{ , abstract = {Extended gamma-ray emission around isolated pulsars at TeV energies, also known as TeV halos, have been found around a handful of middle-aged pulsars. The halos are significantly more extended than their pulsar wind nebulae but much smaller than the particle diffusion length in the interstellar medium. The origin of TeV halos is unknown. Interpretations invoke either local effects related to the environment of a pulsar or generic particle transport behaviors. The latter scenario predicts that TeV halos would be a universal phenomena for all pulsars. We searched for extended gamma-ray emission around 36 isolated middle-aged pulsars identified by radio and gamma-ray facilities using 2321 days of data from the High-Altitude Water Cherenkov (HAWC) Observatory. Through a stacking analysis comparing TeV flux models against a background-only hypothesis, we identified TeV halolike emission at a significance level of . Our results imply that extended TeV gamma-ray halos may commonly exist around middle-aged pulsars. This reveals a previously unknown feature about pulsars and opens a new window to identify the pulsar population that is invisible to radio, x-ray, and GeV gamma-ray observations.}, archive = {J_PRL}, author = {A. Albert and R. Alfaro and C. Alvarez and J. C. Arteaga-Velázquez and D. Avila Rojas and H. A. Ayala Solares and R. Babu and E. Belmont-Moreno and A. Bernal and K. S. Caballero-Mora and T. Capistrán and A. Carramiñana and S. Casanova and U. Cotti and J. Cotzomi and S. Coutiño de León and E. De la Fuente and C. de León and D. Depaoli and P. Desiati and N. Di Lalla and R. Diaz Hernandez and B. L. Dingus and M. A. DuVernois and J. C. Díaz-Vélez and K. Engel and C. Espinoza and K. L. Fan and K. Fang and N. Fraija and J. A. García-González and F. Garfias and H. Goksu and M. M. González and J. A. Goodman and S. Groetsch and J. P. Harding and S. Hernández-Cadena and I. Herzog and D. Huang and F. Hueyotl-Zahuantitla and A. Iriarte and S. Kaufmann and D. Kieda and J. Lee and H. León Vargas and J. T. Linnemann and A. L. Longinotti and G. Luis-Raya and K. Malone and O. Martinez and J. Martínez-Castro and J. A. Matthews and P. Miranda-Romagnoli and J. A. Morales-Soto and E. Moreno and M. Mostafá and L. Nellen and M. U. Nisa and N. Omodei and Y. Pérez Araujo and E. G. Pérez-Pérez and C. D. Rho and D. Rosa-González and E. Ruiz-Velasco and H. Salazar and D. Salazar-Gallegos and A. Sandoval and M. Schneider and J. Serna-Franco and Y. Son and R. W. Springer and O. Tibolla and K. Tollefson and I. Torres and R. Torres-Escobedo and R. Turner and F. Ureña-Mena and E. Varela and L. Villaseñor and X. Wang and E. Willox and H. Wu and H. Zhou}, doi = {10.1103/PhysRevLett.134.171005}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171005}, shortjournal = {Phys. Rev. Lett.}, title = {Extended TeV halos may commonly exist around middle-aged pulsars}, volume = {134}, year = {2025}, }
• (2025). First axionlike particle results from a broadband search for wavelike dark matter in the 44 to 52 μeV range with a coaxial dish antenna. PRL, 134(17), 171002. (www)

  @article{ , abstract = {We present the results from the first axionlike particle search conducted using a dish antenna. The experiment was conducted at room temperature and sensitive to axionlike particles in the range (10.7–12.5 GHz). The novel dish antenna geometry was proposed by the BREAD Collaboration and previously used to conduct a dark photon search in the same mass range. To allow for axionlike particle sensitivity, the BREAD dish antenna was placed in a 3.9 T solenoid magnet at Argonne National Laboratory. In the presence of a magnetic field, axionlike dark matter converts to photons at the conductive surface of the reflector. The signal is focused onto a custom coaxial horn antenna and read out with a low-noise radio-frequency receiver. No evidence of axionlike dark matter was observed in this mass range and we place the most stringent laboratory constraints on the axion-photon coupling strength, in this mass range at 90% confidence.}, archive = {J_PRL}, author = {GigaBREAD Collaboration and Gabe Hoshino and Stefan Knirck and Mohamed H. Awida and Gustavo I. Cancelo and Simon Corrodi and Martin Di Federico and Benjamin Knepper and Alex Lapuente and Mira Littmann and David W. Miller and Donald V. Mitchell and Derrick Rodriguez and Mark K. Ruschman and Chiara P. Salemi and Matthew A. Sawtell and Leandro Stefanazzi and Andrew Sonnenschein and Gary W. Teafoe and Peter Winter}, doi = {10.1103/PhysRevLett.134.171002}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171002}, shortjournal = {Phys. Rev. Lett.}, title = {First axionlike particle results from a broadband search for wavelike dark matter in the 44 to 52 μeV range with a coaxial dish antenna}, volume = {134}, year = {2025}, }
• (2025). In situ measurements of dark photon dark matter using parker solar probe: Going beyond the radio window. PRL, 134(17), 171001. (www)

  @article{ , abstract = {Dark photon dark matter (DPDM) emerges as a compelling candidate for ultralight bosonic dark matter, detectable through resonant conversion into photons within a plasma environment. This Letter employs in situ measurements from the Parker Solar Probe (PSP), the first spacecraft to venture into the solar corona, to probe for DPDM signatures. The PSP in situ measurements go beyond the traditional radio window, spanning frequencies between about 10 kHz and 20 MHz, a challenging range inaccessible to Earth-based radio astronomy. Additionally, the proximity of PSP to the resonant conversion location enhances the signal flux, providing a distinct advantage over ground-based observations. As a result, the PSP data establishes the most stringent constraints on the kinetic mixing parameter for DPDM frequencies between 70 kHz and 20 MHz, with values of . Investigating the data from STEREO satellites resulted in weaker constraints compared to those obtained from PSP. By utilizing state-of-the-art solar observations from space, we have surpassed the cosmic microwave background limits derived from early-universe observations.}, archive = {J_PRL}, author = {Haipeng An and Shuailiang Ge and Jia Liu and Mingzhe Liu}, doi = {10.1103/PhysRevLett.134.171001}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {171001}, shortjournal = {Phys. Rev. Lett.}, title = {In situ measurements of dark photon dark matter using parker solar probe: Going beyond the radio window}, volume = {134}, year = {2025}, }
• (2025). Random distillation protocols in long baseline telescopy. PRL, 134(17), 170801. (www)

  @article{ , abstract = {In quantum-enhanced astronomical imaging, multiple distant apertures work together by utilizing quantum resources distributed from a central server. Our findings suggest that preprocessing the stellar light received by all telescopes can improve imaging performance without increasing resource consumption. The preprocessing leverages weak quantum measurements and modifies random-party entanglement distillation protocols from quantum information science. Intuitively, this approach allows us to collapse the stellar light that is originally coherent between all telescopes to one pair of telescopes with probability arbitrarily close to one. The central server can then distribute entanglement solely to the pair of telescopes receiving a photon, thereby enhancing the efficiency of resource utilization. We discuss two types of resources that benefit from this preprocessing: shared entanglement and a shared reference frame.}, archive = {J_PRL}, author = {Yunkai Wang and Eric Chitambar}, doi = {10.1103/PhysRevLett.134.170801}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {170801}, shortjournal = {Phys. Rev. Lett.}, title = {Random distillation protocols in long baseline telescopy}, volume = {134}, year = {2025}, }
• (2025). Variational LOCC-assisted quantum circuits for long-range entangled states. PRL, 134(17), 170601. (www)

  @article{ , abstract = {Long-range entanglement is an important quantum resource, particularly for topological orders and quantum error correction. In reality, preparing long-range entangled states requires a deep unitary circuit, which poses significant experimental challenges. A promising avenue is offered by replacing some quantum resources with local operations and classical communication (LOCC). With these classical components, one can communicate outcomes of midcircuit measurements in distant subsystems, substantially reducing circuit depth in many important cases. However, to prepare general long-range entangled states, finding LOCC-assisted circuits of a short depth remains an open question. Here, to address this challenge, we propose a quantum-classical hybrid algorithm to find optimal LOCC protocols for preparing ground states of given Hamiltonians. In our algorithm, we introduce an efficient way to estimate parameter gradients and use such gradients for variational optimization. Theoretically, we establish the conditions for the absence of barren plateaus, ensuring trainability at a large system size. Numerically, the algorithm accurately solves the ground state of long-range entangled models, such as the perturbed Greenberger–Horne–Zeilinger state and surface code. Our results demonstrate the advantage of our method over conventional unitary variational circuits: the practical advantage in the accuracy of estimated ground-state energy and the theoretical advantage in creating long-range entanglement.}, archive = {J_PRL}, author = {Yuxuan Yan and Muzhou Ma and You Zhou and Xiongfeng Ma}, doi = {10.1103/PhysRevLett.134.170601}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {170601}, shortjournal = {Phys. Rev. Lett.}, title = {Variational LOCC-assisted quantum circuits for long-range entangled states}, volume = {134}, year = {2025}, }
• (2025). Gibbs-preserving operations requiring infinite amount of quantum coherence. PRL, 134(17), 170201. (www)

  @article{ , abstract = {Gibbs-preserving operations have been studied as one of the standard free processes in quantum thermodynamics. Although they admit a simple mathematical structure, their operational significance has been unclear due to the potential hidden cost to implement them using an operationally motivated class of operations, such as thermal operations. Here, we show that this hidden cost can be infinite—we present a family of Gibbs-preserving operations that cannot be implemented by thermal operations aided by any finite amount of quantum coherence. Our result implies that there are uncountably many Gibbs-preserving operations that require unbounded thermodynamic resources to implement, raising a question about employing Gibbs-preserving operations as available thermodynamics processes. This finding is a consequence of the general lower bounds we provide for the coherence cost of approximately implementing a certain class of Gibbs-preserving operations with a desired accuracy. We find that our lower bound is almost tight, identifying a quantity—related to the energy change caused by the channel to implement—as a fundamental quantifier characterizing the coherence cost for the approximate implementation of Gibbs-preserving operations.}, archive = {J_PRL}, author = {Hiroyasu Tajima and Ryuji Takagi}, doi = {10.1103/PhysRevLett.134.170201}, journal = {Physical Review Letters}, month = {4}, number = {17}, pages = {170201}, shortjournal = {Phys. Rev. Lett.}, title = {Gibbs-preserving operations requiring infinite amount of quantum coherence}, volume = {134}, year = {2025}, }
• (2025). Erratum: Dynamical signatures of quasiparticle interactions in quantum spin chains [Phys. rev. lett. 125, 187201 (2020)]. PRL, 134(16), 169901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 169901 (2025)}, archive = {J_PRL}, author = {Anna Keselman and Leon Balents and Oleg A. Starykh}, doi = {10.1103/PhysRevLett.134.169901}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {169901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Dynamical signatures of quasiparticle interactions in quantum spin chains [Phys. rev. lett. 125, 187201 (2020)]}, volume = {134}, year = {2025}, }
• (2025). Differential elasticity affects lineage segregation of embryonic stem cells. PRL, 134(16), 168401. (www)

  @article{ , abstract = {The question of what guides lineage segregation is central to development, where cellular differentiation leads to segregated cell populations destined for specialized functions. Here, using optical tweezers measurements of mouse embryonic stem cells, we reveal a mechanical mechanism based on differential elasticity in the second lineage segregation of the embryonic inner cell mass into epiblast (EPI) cells, which will develop into the fetus, and primitive endoderm (PrE), which will form extraembryonic structures such as the yolk sac. Remarkably, we find that these mechanical differences already occur during priming, not just after a cell has committed to differentiation. Specifically, we show that PrE-primed cells exhibit significantly higher elasticity than EPI-primed cells, characterized by lower power spectrum scaling exponents, higher Young’s modulus, and lower loss tangent. Using a model of two cell types differing only in elasticity, we show that differential elasticity alone is sufficient to lead to segregation between cell types, suggesting that the mechanical attributes of the cells contribute to the segregation process. Importantly, we find that this process relies on cellular activity. Our findings present differential elasticity as a previously unknown mechanical contributor to lineage segregation during embryo morphogenesis.}, archive = {J_PRL}, author = {Christine M. Ritter and Tianxiang Ma and Natascha Leijnse and Younes Farhangi Barooji and William Hamilton and Joshua M. Brickman and Amin Doostmohammadi and Lene B. Oddershede}, doi = {10.1103/PhysRevLett.134.168401}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {168401}, shortjournal = {Phys. Rev. Lett.}, title = {Differential elasticity affects lineage segregation of embryonic stem cells}, volume = {134}, year = {2025}, }
• (2025). Upsurge of spontaneous knotting in polar diblock active polymers. PRL, 134(16), 168301. (www)

  @article{ , abstract = {Spontaneous formation of knots in long polymers at equilibrium is inevitable but becomes rare in sufficiently short chains. Here, we show that knotting increases by orders of magnitude in diblock polymers having a fraction p of self-propelled monomers. Remarkably, this enhancement is not monotonic in p with an optimal value independent of the monomer’s activity. By monitoring the knot’s size and position we elucidate the mechanisms of its formation, diffusion, and untying and ascribe the nonmonotonic behavior to the competition between the rate of knot formation and the knot’s lifetime. These findings suggest a nonequilibrium mechanism to generate entangled filaments at the nano- and microscales.}, archive = {J_PRL}, author = {Marin Vatin and Enzo Orlandini and Emanuele Locatelli}, doi = {10.1103/PhysRevLett.134.168301}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {168301}, shortjournal = {Phys. Rev. Lett.}, title = {Upsurge of spontaneous knotting in polar diblock active polymers}, volume = {134}, year = {2025}, }
• (2025). Hindered stokesian settling of discs and rods. PRL, 134(16), 168202. (www)

  @article{ , abstract = {We report measurements of the mean settling velocities for suspensions of discs and rods in the Stokes regime for a number of particle aspect ratios. All these shapes display “hindered settling,” namely, a decrease in settling speed as the solid volume fraction is increased. A comparison of our data to spheres reveals that discs and rods show less hindering than spheres at the same relative interparticle separation. The data for all six of our particle shapes may be scaled to collapse on that of spheres, with a scaling factor that depends only on the volume of the particle relative to a sphere. Despite the orientational degrees of freedom available with nonspherical particles, it thus appears that the dominant contribution to the hindered settling emerges from terms that are simply proportional to the volume of the sedimenting particles, enabling prediction of hindered settling of other nonpolar axisymmetric shapes.}, archive = {J_PRL}, author = {Yating Zhang and Narayanan Menon}, doi = {10.1103/PhysRevLett.134.168202}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {168202}, shortjournal = {Phys. Rev. Lett.}, title = {Hindered stokesian settling of discs and rods}, volume = {134}, year = {2025}, }
• (2025). Surfactant exchanges between deformed soap films. PRL, 134(16), 168201. (www)

  @article{ , abstract = {The effective viscosity of liquid foams is controlled by Marangoni forces and therefore by the transport of surfactants. Direct tracking of the latter during foam deformation is out of reach. Besides, the competition between diffusion and convection on the interfaces and in the bulk of complex assemblies of thin films and menisci is still an open problem. These shortcomings severely limit our understanding of foam rheology and stability. In this Letter, we use a comprehensive characterization of in-plane flows in an elementary foam during imposed deformation to determine indirectly the flux of surfactants from a film to its first neighbor. We show that the meniscus connecting the films, despite its potential role as a surfactant reservoir, is not involved in surfactant transport. This information has been identified as a key missing piece in local foam viscosity models of the literature.}, archive = {J_PRL}, author = {Théo Lenavetier and Emmanuel Schaub and Isabelle Cantat}, doi = {10.1103/PhysRevLett.134.168201}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {168201}, shortjournal = {Phys. Rev. Lett.}, title = {Surfactant exchanges between deformed soap films}, volume = {134}, year = {2025}, }
• (2025). Waveform proportionality and taylor’s law induced by synchronization of periodic and chaotic oscillators. PRL, 134(16), 167202. (www)

  @article{ , abstract = {Taylor’s law (TL), the scaling relationship between mean and variance, has been observed in various fields. However, the underlying reasons for the widespread occurrence of TL, the frequent appearance of the TL exponent value close to 2, and the relationship between temporal and spatial TLs are not fully understood. Here, using coupled oscillator models, we analytically and numerically demonstrate that synchronization can induce TL. In particular, we show that strong synchronization leads to waveform proportionality, resulting in temporal and spatial TLs with an exponent 2. Our results can help infer the existence of synchronization solely from the correlation between mean and variance.}, archive = {J_PRL}, author = {Yuzuru Mitsui and Hiroshi Kori}, doi = {10.1103/PhysRevLett.134.167202}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {167202}, shortjournal = {Phys. Rev. Lett.}, title = {Waveform proportionality and taylor’s law induced by synchronization of periodic and chaotic oscillators}, volume = {134}, year = {2025}, }
• (2025). Robust chaos in a totally symmetric network of four phase oscillators. PRL, 134(16), 167201. (www)

  @article{ , abstract = {The Kuramoto model and its generalizations are universal models of collective behavior in oscillatory networks. We provide conditions on the coupling function such that the Kuramoto system with four globally coupled identical oscillators has chaotic attractors: a pair of Lorenz attractors or a four-winged analog of the Lorenz attractor. The attractors emerge near the triple instability threshold of the splay-phase synchronization state of the oscillators. We provide theoretical arguments and verify numerically, based on the pseudohyperbolicity test, that the chaotic dynamics are robust with respect to small, e.g., time-dependent, perturbations of the system. The robust chaoticity should also be inherited by any network of weakly interacting systems with such attractors.}, archive = {J_PRL}, author = {Efrosiniia Karatetskaia and Alexey Kazakov and Klim Safonov and Dmitry Turaev}, doi = {10.1103/PhysRevLett.134.167201}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {167201}, shortjournal = {Phys. Rev. Lett.}, title = {Robust chaos in a totally symmetric network of four phase oscillators}, volume = {134}, year = {2025}, }
• (2025). Nonreciprocal interactions reshape topological defect annihilation. PRL, 134(16), 167101. (www)

  @article{ , abstract = {We show how nonreciprocal ferromagnetic interactions between neighboring planar spins in two dimensions, affect the behavior of topological defects. Nonreciprocity is introduced by weighting the coupling strength of the two-dimensional XY model by an anisotropic kernel. As a consequence, in addition to the topological charge q , the actual shape of the defects becomes crucial to faithfully describe their dynamics. Nonreciprocal coupling twists the spin field, selecting specific defect shapes, dramatically altering the pair annihilation process. Defect annihilation can either be enhanced or hindered, depending on the shape of the defects concerned and the degree of nonreciprocity in the system. We introduce a continuous description—for which the phenomenological coefficients can be explicitly written in terms of the microscopic ones—that captures the behavior of the lattice model.}, archive = {J_PRL}, author = {Ylann Rouzaire and Daniel J. G. Pearce and Ignacio Pagonabarraga and Demian Levis}, doi = {10.1103/PhysRevLett.134.167101}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {167101}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal interactions reshape topological defect annihilation}, volume = {134}, year = {2025}, }
• (2025). Quadrupolar and dipolar excitons in bilayer 2H−MoSe2. PRL, 134(16), 166901. (www)

  @article{ , abstract = {We report the experimental observation of quadrupolar exciton states in the reflectance contrast spectrum of 2 H -stacked bilayer MoSe 2 . The application of a vertical electric field results in a quadratic energy redshift of these quadrupolar excitons, in contrast to the linear energy splitting observed in the coexisting dipolar excitons within the bilayer MoSe 2 . We perform helicity-resolved reflectance contrast measurements to investigate the spin and valley configurations of the quadrupolar exciton states as a function of applied vertical electric and magnetic fields. Comparing our results with a phenomenological coupled-oscillator model indicates that the electric- and magnetic-field dependence of the quadrupolar exciton states can be attributed to the intra- and intervalley hybridization of spin-triplet interlayer excitons with opposite permanent dipole moments, mediated by interlayer hole tunneling. These results position naturally stacked MoSe 2 bilayers as a promising platform to explore electric-field-tunable many-body exciton phenomena.}, archive = {J_PRL}, author = {Shun Feng and Aidan J. Campbell and Bibi Mary Francis and Hyeonjun Baek and Takashi Taniguchi and Kenji Watanabe and Iann C. Gerber and Brian D. Gerardot and Mauro Brotons-Gisbert}, doi = {10.1103/PhysRevLett.134.166901}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166901}, shortjournal = {Phys. Rev. Lett.}, title = {Quadrupolar and dipolar excitons in bilayer 2H−MoSe2}, volume = {134}, year = {2025}, }
• (2025). Design of altermagnetic models from spin clusters. PRL, 134(16), 166701. (www)

  @article{ , abstract = {Altermagnetism, a new class of collinear compensated magnetic phase, has garnered tremendous interest because of its rich physics and promising applications. Physical models and verified material candidates for altermagnetism remain limited. Here, we propose a general scheme to construct altermagnetic models, which explicitly exhibits the blend of ferromagnetic and antiferromagnetic correlations in real space via the design of spin clusters, echoing the observation that properties of altermagnets resemble a mixture of ferromagnets and antiferromagnets. We show that in some of our models, the desired altermagnetic order can be spontaneously realized by electron-electron interaction in a broad range of the phase diagram. This development facilitates the study of fascinating physics of altermagnetism and sheds light on the discovery of new altermagnetic materials.}, archive = {J_PRL}, author = {Xingchuan Zhu and Xingmin Huo and Shiping Feng and Song-Bo Zhang and Shengyuan A. Yang and Huaiming Guo}, doi = {10.1103/PhysRevLett.134.166701}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166701}, shortjournal = {Phys. Rev. Lett.}, title = {Design of altermagnetic models from spin clusters}, volume = {134}, year = {2025}, }
• (2025). Moiré kramers-weyl fermions with ideal radial spin texture from structural chirality. PRL, 134(16), 166401. (www)

  @article{ , abstract = {We demonstrate that two-dimensional Kramers-Weyl fermions can be engineered in spin-orbit coupled twisted bilayers, where the chiral structure of these moiré systems breaks all mirror symmetries, confining Kramers-Weyl fermions to high-symmetry points in the Brillouin zone under time reversal symmetry. Our theoretical analysis reveals a symmetry-enforced, Weyl-like spinful interlayer moiré coupling that universally ensures an ideal radial spin-texture at arbitrary twist angles, under C n z symmetry with n > 2 . First principles density functional calculation confirm the realization of these fermions in twisted α − In 2 Se 3 homobilayers, where flat bands and out-of-plane ferroelectric polarization in each layer guarantee two-dimensional Kramers-Weyl physics with ideal radial spin textures.}, archive = {J_PRL}, author = {D. J. P. de Sousa and Seungjun Lee and Tony Low}, doi = {10.1103/PhysRevLett.134.166401}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166401}, shortjournal = {Phys. Rev. Lett.}, title = {Moiré kramers-weyl fermions with ideal radial spin texture from structural chirality}, volume = {134}, year = {2025}, }
• (2025). Sensing quantum vacuum fluctuations with non-gaussian electronic noise. PRL, 134(16), 166301. (www)

  @article{ , abstract = {The statistics of electron transport in a quantum conductor is affected by fluctuations of its voltage bias. Here, we show experimentally how a third order correlation in the electromagnetic field arises from the noise of a tunnel junction in the microwave domain being modulated by the vacuum fluctuations generated by a resistor at ultralow temperature. This provides a way to measure the vacuum fluctuations experienced by the junction, not offset by the unavoidable noise added by the detection setup.}, archive = {J_PRL}, author = {Clovis Farley and Edouard Pinsolle and Bertrand Reulet}, doi = {10.1103/PhysRevLett.134.166301}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166301}, shortjournal = {Phys. Rev. Lett.}, title = {Sensing quantum vacuum fluctuations with non-gaussian electronic noise}, volume = {134}, year = {2025}, }
• (2025). Full-scaling friction and wear laws of nanotwinned metals. PRL, 134(16), 166201. (www)

  @article{ , abstract = {Ultrastrong nanotwinned (NT) metals hold promise for mitigating friction and wear—essential for enhancing the energy efficiency and longevity of all moving systems. However, optimizing their tribological performance has long suffered from the absence of friction and wear laws across varying tribological loading scales. Here, we have discovered full-scaling twin lamella spacing ( λ )-dependent friction and wear laws in NT pure nickel and identified critical deformation mechanisms for reducing friction and wear. Nanoscale friction initially increases with decreasing λ , peaking at 20 nm, and then decreases due to a transition from dislocation-twin boundary interactions to detwinning. Under microscale loading, friction and wear reduce linearly with decreasing λ , attributed to an unforeseen phase transition from face-centered cubic to hexagonal close-packed structures. Furthermore, under macroscale loading, the formation of a durable oxide layer and a stable gradient nanostructure in nanotwinned nickel with λ exceeding 20 nm aids in mitigating wear loss.}, archive = {J_PRL}, author = {Yan Lin and Ziyue Zhang and Fenghui Duan and Fangming Wang and Fei Liang and Qicheng Zhang and Yong Li and Jie Pan and Keke Chang and Yonghao Zhao and Yuntian Zhu and Xiang Chen}, doi = {10.1103/PhysRevLett.134.166201}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166201}, shortjournal = {Phys. Rev. Lett.}, title = {Full-scaling friction and wear laws of nanotwinned metals}, volume = {134}, year = {2025}, }
• (2025). Corrugation-dominated mechanical softening of defect-engineered graphene. PRL, 134(16), 166102. (www)

  @article{ , abstract = {We measure the two-dimensional elastic modulus E 2 D of atomically clean defect-engineered graphene with a known vacancy distribution and density in correlated ultrahigh vacuum experiments. The vacancies are introduced via low-energy ( < 200 eV ) Ar ion irradiation, and the atomic structure is obtained via semiautonomous scanning transmission electron microscopy and image analysis. Based on atomic force microscopy nanoindentation measurements, a decrease of E 2 D from 286 to 158 N / m is observed when measuring the same graphene membrane before and after introducing vacancies at a density of 1.0 × 10 13 cm − 2 . This decrease is significantly greater than what is predicted by most theoretical studies and in stark contrast to some measurements presented in the literature. With the assistance of atomistic simulations, we show that this softening is mostly due to corrugations caused by local strain at vacancies with two or more missing atoms, while the influence of single vacancies is negligible. We further demonstrate that the opposite effect can be measured when surface contamination is not removed before defect engineering.}, archive = {J_PRL}, author = {Wael Joudi and Rika Saskia Windisch and Alberto Trentino and Diana Propst and Jacob Madsen and Toma Susi and Clemens Mangler and Kimmo Mustonen and Florian Libisch and Jani Kotakoski}, doi = {10.1103/PhysRevLett.134.166102}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166102}, shortjournal = {Phys. Rev. Lett.}, title = {Corrugation-dominated mechanical softening of defect-engineered graphene}, volume = {134}, year = {2025}, }
• (2025). Negative gradient energy facilitates charged domain walls in HfO2. PRL, 134(16), 166101. (www)

  @article{ , abstract = {Charged domain walls (CDWs) in ferroelectrics are often characterized as excited states, even after full bound charge compensation at domain walls (DWs). Here, we propose a mechanism where negative gradient energy ( E grad ) counteracts the large positive electrostatic energy ( E el ) induced by bound charge at DWs, stabilizing the CDWs over the bulk state, even with partial or no bound charge compensation. As proof of scheme, we demonstrate that negative E grad of modes, which reverse their sign during the formation of CDWs in HfO 2 , partially offsets E el . Their corresponding remaining E el can be neutralized by partial bound charge compensation. Exceeding this partial compensation, achieved through the substitution of Nb 5 + at tail-to-tail and Y 3 + at head-to-head DWs for Hf 4 + , CDWs exhibit unprecedented stability over the bulk state. The 1.33 eV band gap of the most stable CDW is particularly suitable for photovoltaic applications due to their potential for efficient electron-hole separation. We further reveal that negative phonon band curvatures are useful descriptors to uncover the origin of negative E grad in such CDWs, which can be estimated simply by phonon band fitting, making our scheme easy to implement for realizing CDWs beyond HfO 2 .}, archive = {J_PRL}, author = {Pawan Kumar and Dipti Gupta and Jun Hee Lee}, doi = {10.1103/PhysRevLett.134.166101}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166101}, shortjournal = {Phys. Rev. Lett.}, title = {Negative gradient energy facilitates charged domain walls in HfO2}, volume = {134}, year = {2025}, }
• (2025). Refractive contribution to the mass of an elementary excitation in a dilute bose-einstein condensate. PRL, 134(16), 166001. (www)

  @article{ , abstract = {Since the pioneering works of Landau and Feynman, the origin of a roton minimum in the excitation spectrum of a quantum Bose liquid has been debated. A consensus has been reached on relation of the roton to eventual solidification, but this viewpoint still remains to be connected to the polaronic concept of an impurity pushing through a dense medium. The diagrammatic theory allows one to approach the problem qualitatively from a dilute limit. We revisit the equation for the elementary excitation spectrum obtained in the ladder approximation and argue that polaronic renormalization of the quasiparticle mass has a contribution due to matter-wave refraction. At low energies attenuation of the quasiparticle wave turns out to be dramatically suppressed by the condensate. Refractive correction to the mass is enhanced by Bose statistics at high momenta and produces autolocalization of an elementary excitation upon increasing the density.}, archive = {J_PRL}, author = {S. V. Andreev}, doi = {10.1103/PhysRevLett.134.166001}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {166001}, shortjournal = {Phys. Rev. Lett.}, title = {Refractive contribution to the mass of an elementary excitation in a dilute bose-einstein condensate}, volume = {134}, year = {2025}, }
• (2025). Ion acoustic instability resulting from suprathermal electrons generated by stimulated raman scattering in laser-plasma interactions. PRL, 134(16), 165102. (www)

  @article{ , abstract = {Using space-time-resolved Thomson scattering, we investigate experimentally the development of electrostatic waves in a preformed undercritical helium plasma driven by a 1.059 μ m laser pulse of ∼ 1.5 ps duration and ∼ 10 15 – 16 W cm − 2 mean intensity. We observe the excitation of intense ion plasma waves (IAWs) over a broad wave number range, distinct from what is expected from stimulated Brillouin scattering or Langmuir decay instability. These IAWs are correlated with the occurrence of backward stimulated Raman scattering (B-SRS) at earlier times but persist much longer than the B-SRS-driven electron plasma waves. Particle-in-cell modeling reveals that they result from an ion acoustic instability triggered by the bulk electrons drifting against the ions to neutralize the current carried by the B-SRS-generated hot electrons. The properties of the simulated unstable IAWs match well with the measurements.}, archive = {J_PRL}, author = {C. Rousseaux and S. D. Baton and K. Glize and L. Lancia and D. Bénisti and G. Sary and L. Gremillet}, doi = {10.1103/PhysRevLett.134.165102}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {165102}, shortjournal = {Phys. Rev. Lett.}, title = {Ion acoustic instability resulting from suprathermal electrons generated by stimulated raman scattering in laser-plasma interactions}, volume = {134}, year = {2025}, }
• (2025). Direct evidence of multispecies hydrodynamics in ignition-scale hohlraums. PRL, 134(16), 165101. (www)

  @article{ , abstract = {A targeted experiment at the National Ignition Facility (NIF) confirms the presence of multispecies hydrodynamics in inertial confinement fusion hohlraums relevant to ignition. The effects are identified by filling the gold hohlraum with a deuterium-tritium (DT) gas mixture instead of helium. As the hohlraum is heated by the NIF lasers, it implodes inward, compressing and heating the DT, which leads to fusion. The resulting DT-fusion neutrons are measured in space, time, yield, angle, and energy. A distinct, peaked, triangular shape in the radial neutron emission profile provides evidence of a “leaky piston” effect caused by the interpenetration of DT into the expanding gold. This process reduces the reversibility of DT compression and decreases neutron generation on the temporal trailing edge compared to the leading edge. These results are well described by multispecies hydrodynamics simulations, which reproduce the observed spatial and temporal features, as well as the total neutron yield and angularly resolved energy spectra. In contrast, conventional simulations that use only single-species physics fail to match the experimental data. They overpredict the neutron yield, produce a flatter-than-observed spatial profile, and show excessive emission at late times compared to the experimental measurements.}, archive = {J_PRL}, author = {Drew P. Higginson and N. Izumi and M. D. Rosen and P. Volegov and T. Chapman and D. N. Fittinghoff and K. D. Hahn and B. M. Haines and J. Jeet and A. J. Kemp and S. Kerr and O. L. Landen and S. MacLaren and A. J. MacKinnon and J. D. Moody and A. S. Moore and B. L. Reichelt and W. M. Riedel and D. J. Schlossberg and D. J. Strozzi and A. E. Youmans and G. Zimmerman and W. A. Farmer and J. S. Ross and D. E. Hinkel}, doi = {10.1103/PhysRevLett.134.165101}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {165101}, shortjournal = {Phys. Rev. Lett.}, title = {Direct evidence of multispecies hydrodynamics in ignition-scale hohlraums}, volume = {134}, year = {2025}, }
• (2025). Synthetic non-abelian electric fields and spin-orbit coupling in photonic synthetic dimensions. PRL, 134(16), 163803. (www)

  @article{ , abstract = {We theoretically propose a scheme to synthesize photonic non-Abelian electric field and spin-orbit coupling (SOC) in the synthetic frequency dimension based on a polarization-multiplexed time-modulated ring resonator. Inside the ring resonator, the cascade of polarization-dependent phase modulation, polarization rotation, and phase retardation enables a photonic realization of minimal SOC with Peierls substitution composed of equal Rashba and Dresselhaus coupling. The synthetic bands and associated spin textures can be effectively probed by the continuous-wave polarization- and time-resolved band structure measurements. Meanwhile, the pulse dynamics in the frequency dimension can be manipulated by both synthetic Abelian and non-Abelian electric fields, leading to Bloch oscillation, Zitterbewegung, and their interplay dynamics. Our proposed setup can be realized with free-space optics, fibers, and integrated photonics, and provides pseudospin control knobs for large-scale synthetic lattices based on frequency combs.}, archive = {J_PRL}, author = {Bengy Tsz Tsun Wong and Shu Yang and Zehai Pang and Yi Yang}, doi = {10.1103/PhysRevLett.134.163803}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163803}, shortjournal = {Phys. Rev. Lett.}, title = {Synthetic non-abelian electric fields and spin-orbit coupling in photonic synthetic dimensions}, volume = {134}, year = {2025}, }
• (2025). Construction of various time-varying hamiltonians on thin-film lithium niobate chip. PRL, 134(16), 163802. (www)

  @article{ , abstract = {Integrated photonics provides an important platform for simulating physical models with high-performance chip-scale devices, where the lattice size and the time dependence of a model are key ingredients for further enriching the functionality of a photonic chip. Here, we propose and demonstrate the construction of various time-varying Hamiltonian models using a single microresonator on thin-film lithium niobate chip. Such an integrated microresonator holds high-quality factor to 10 6 , and supports the construction of the synthetic frequency lattice with effective lattice sites up to 221 under efficient integrated electro-optic modulation. By further applying different bichromatic modulations composed of two radio-frequency signals oppositely detuned from the resonant frequency in the microresonator, we successfully build various time-varying Hamiltonian models, where the temporal features of the dynamic band structures are captured from experimental measurements, highlighting great flexibility and tunability of this integrated chip. Our work presents a photonic chip for simulating versatile time-varying Hamiltonians, which pushes forward quantum simulations and future photonic applications.}, archive = {J_PRL}, author = {Rui Ye and Guangzhen Li and Shuai Wan and Xiaotian Xue and Pi-Yu Wang and Xin Qiao and Luojia Wang and Hao Li and Shijie Liu and Jiayu Wang and Rui Ma and Fang Bo and Yuanlin Zheng and Chun-Hua Dong and Luqi Yuan and Xianfeng Chen}, doi = {10.1103/PhysRevLett.134.163802}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163802}, shortjournal = {Phys. Rev. Lett.}, title = {Construction of various time-varying hamiltonians on thin-film lithium niobate chip}, volume = {134}, year = {2025}, }
• (2025). Probing bulk band topology from time boundary effect in synthetic dimension. PRL, 134(16), 163801. (www)

  @article{ , abstract = {An incident wave at a temporal interface, created by an abrupt change in system parameters, generates time-refracted and time-reflected waves. We find topological characteristics associated with the temporal interface that separates distinct spatial topologies and report a novel bulk-boundary correspondence for the temporal interface. The vanishing of either time refraction or time reflection records a topological phase transition across the temporal interface, and the difference of bulk band topology predicts nontrivial braiding hidden in the time refraction and time reflection coefficients. These findings, which are insensitive to spatial boundary conditions and robust against disorder, are demonstrated in a synthetic frequency lattice with rich topological phases engendered by long-range couplings. Our work reveals the topological aspect of temporal interface and paves the way for using the time boundary effect to probe topological phase transitions and topological invariants.}, archive = {J_PRL}, author = {Huisheng Xu and Zhaohui Dong and Luqi Yuan and Liang Jin}, doi = {10.1103/PhysRevLett.134.163801}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163801}, shortjournal = {Phys. Rev. Lett.}, title = {Probing bulk band topology from time boundary effect in synthetic dimension}, volume = {134}, year = {2025}, }
• (2025). Dynamically enhanced two-photon spectroscopy. PRL, 134(16), 163601. (www)

  @article{ , abstract = {A novel quantum control protocol utilizing two-photon processes with trigonometric pulse modulation is developed, enabling the intermediate state population’s dynamic elimination (DE). The proposed DE technique excels at single-photon resonance in contrast to the well-known adiabatic elimination (AE) regime, which requires large single-photon detuning and strong pulses. The DE approach outperforms AE in efficiency and exhibits enhanced resilience to one-photon detuning since the key control parameter, the effective two-photon Rabi frequency, inversely proportional to the modulation frequency, does not depend on the one-photon detuning. The comprehensive analysis of population transfer and Ramsey interferometry demonstrates the protocol’s superiority, achieving enhanced signal-to-noise ratios and higher fidelities with respect to existing two-photon methods.}, archive = {J_PRL}, author = {Sebastian C. Carrasco and Sean Lourette and Ignacio Sola and Vladimir S. Malinovsky}, doi = {10.1103/PhysRevLett.134.163601}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163601}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamically enhanced two-photon spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Unveiling supersolid order via vortex trajectory correlations. PRL, 134(16), 163401. (www)

  @article{ , abstract = {The task of experimentally investigating the inherently dual properties of a supersolid, a simultaneous superfluid and solid, has become more critical following the recent experimental exploration of supersolid regimes in dipolar Bose-Einstein condensates (BECs) of Dy 164 . We introduce a supersolid order parameter that uses vortex-vortex trajectory correlations to simultaneously reveal the periodic density of the underlying solid and superfluidity in a single measure. We propose experiments using existing technology to optically create and image trajectories of vortex dipoles in dipolar BECs that is applicable to large system sizes. We numerically test our observable and find that vortex-vortex correlations reveal the supersolid lattice structure while distinguishing it from superfluidity even in the presence of dissipation. Our method sets the stage for experiments to use vortex trajectory correlations to investigate fundamental properties of supersolids arising from their dynamics and phase transitions as experimental system sizes are increased.}, archive = {J_PRL}, author = {Subrata Das and Vito W. Scarola}, doi = {10.1103/PhysRevLett.134.163401}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163401}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling supersolid order via vortex trajectory correlations}, volume = {134}, year = {2025}, }
• (2025). Photoelectron spin texture in tunneling ionization induced by a linearly polarized laser pulse. PRL, 134(16), 163201. (www)

  @article{ , abstract = {The spin polarization of photoelectrons in tunneling ionization is investigated using numerical solutions of the time-dependent Schrödinger equation in companion with our analytic treatment via the spin-resolved strong-field approximation and classical trajectory Monte Carlo simulations. We demonstrate a nontrivial spin texture of photoelectrons in momentum space, exhibiting a vortex structure relative to the laser polarization axis. The momentum-resolved polarization stems from the emergence of spin-correlated quantum orbits in the continuum. For direct electrons in few-cycle pulses, the nonvanishing initial transverse velocity of the electron is responsible for the polarization, while in long pulses, the spin texture is essentially shaped by recollisions. Furthermore, the interference between direct and rescattering ionization leads to spin-polarized electron holography, offering an alternative method to extract atomic fine structural information.}, archive = {J_PRL}, author = {Pei-Lun He and Zhao-Han Zhang and Karen Z. Hatsagortsyan and Christoph H. Keitel}, doi = {10.1103/PhysRevLett.134.163201}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163201}, shortjournal = {Phys. Rev. Lett.}, title = {Photoelectron spin texture in tunneling ionization induced by a linearly polarized laser pulse}, volume = {134}, year = {2025}, }
• (2025). Nondestructive control of the rovibrational ground state of a single molecular hydrogen ion in a penning trap. PRL, 134(16), 163001. (www)

  @article{ , abstract = {In this work, we demonstrate a new method for quantum state control and nondestructive internal quantum state readout of a single HD + ion in the rovibrational ground state in a Penning trap. Furthermore, we demonstrate a measurement of the magnetic trapping field with the same ion to sub-ppb uncertainty. This could enable nondestructive, high-precision spectroscopy of the hyperfine, Zeeman, and rovibrational level structure of single molecular ions. In particular, this technique can be applied to H 2 + as well as to its antimatter equivalent, H ¯ 2 − , with the potential for high-precision tests of charge-parity-time reversal symmetry beyond current sensitivities [ Phys. Scr. T 1995 , 423 (1995) , Phys. Rev. A 98 , 010101 (2018) ].}, archive = {J_PRL}, author = {Charlotte M. König and Fabian Heiße and Jonathan Morgner and Tim Sailer and Bingsheng Tu and Dimitar Bakalov and Klaus Blaum and Stephan Schiller and Sven Sturm}, doi = {10.1103/PhysRevLett.134.163001}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {163001}, shortjournal = {Phys. Rev. Lett.}, title = {Nondestructive control of the rovibrational ground state of a single molecular hydrogen ion in a penning trap}, volume = {134}, year = {2025}, }
• (2025). Probing exotic cross-shell interactions at n=28 with single-neutron transfer on k47. PRL, 134(16), 162504. (www)

  @article{ , abstract = {We present the first measurement of the K 47 ( d , p γ ) K 48 transfer reaction, performed in inverse kinematics using a reaccelerated beam of K 47 . The level scheme of K 48 has been greatly extended, with nine new bound excited states identified and spectroscopic factors deduced. Uniquely, the K 47 ( d , p ) reaction gives access to nuclear states that are sensitive to the interaction of protons and neutrons in the widely spaced 1 s and f p orbitals, respectively. Detailed comparisons with SDPF-U and SDPF-MU shell-model calculations reveal a number of discrepancies between theory and experiment. Intriguingly, a systematic overestimation of spectroscopic factors and a poor reproduction of the energies for 1 − states suggests that the mixing between the π s 1 / 2 1 d 3 / 2 4 and π s 1 / 2 2 d 3 / 2 3 proton configurations in K 48 is not correctly described using current interactions, challenging our description of light nuclei around the N = 28 island of inversion.}, archive = {J_PRL}, author = {C. J. Paxman and A. Matta and W. N. Catford and G. Lotay and M. Assié and E. Clément and A. Lemasson and D. Ramos and N. A. Orr and F. Galtarossa and V. Girard-Alcindor and J. Dudouet and N. L. Achouri and D. Ackermann and D. Barrientos and D. Beaumel and P. Bednarczyk and G. Benzoni and A. Bracco and L. Canete and B. Cederwall and M. Ciemala and P. Delahaye and D. T. Doherty and C. Domingo-Pardo and B. Fernández-Domínguez and D. Fernández and F. Flavigny and C. Fougères and G. de France and S. Franchoo and A. Gadea and J. Gibelin and V. González and A. Gottardo and N. Goyal and F. Hammache and L. J. Harkness-Brennan and D. S. Harrouz and B. Jacquot and D. S. Judson and A. Jungclaus and A. Kaşkaş and W. Korten and M. Labiche and L. Lalanne and C. Lenain and S. Leoni and J. Ljungvall and J. Lois-Fuentes and T. Lokotko and A. Lopez-Martens and A. Maj and F. M. Marqués and I. Martel and R. Menegazzo and D. Mengoni and B. Million and J. Nyberg and R. M. Pérez-Vidal and L. Plagnol and Zs. Podolyák and A. Pullia and B. Quintana and D. Regueira-Castro and P. Reiter and M. Rejmund and K. Rezynkina and E. Sanchis and M. Şenyiğit and N. de Séréville and M. Siciliano and D. Sohler and O. Stezowski and J.-C. Thomas and A. Utepov and J. J. Valiente-Dobón and D. Verney and M. Zielińska}, doi = {10.1103/PhysRevLett.134.162504}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {162504}, shortjournal = {Phys. Rev. Lett.}, title = {Probing exotic cross-shell interactions at n=28 with single-neutron transfer on k47}, volume = {134}, year = {2025}, }
• (2025). Ab initio study of the beryllium isotopes be7 to be12. PRL, 134(16), 162503. (www)

  @article{ , abstract = {We present a systematic ab initio study of the low-lying states in beryllium isotopes from Be 7 to Be 12 using nuclear lattice effective field theory with the N 3 LO interaction. Our calculations achieve good agreement with experimental data for energies, radii, and electromagnetic properties. We introduce a novel, model-independent method to quantify nuclear shapes, uncovering a distinct pattern in the interplay between positive and negative parity states across the isotopic chain. By combining Monte Carlo sampling of the many-body density operator with a novel nucleon-grouping algorithm, the prominent two-center cluster structures, the emergence of one-neutron halo, complex nuclear molecular dynamics such as π orbital and σ orbital, emerge naturally.}, archive = {J_PRL}, author = {Shihang Shen and Serdar Elhatisari and Dean Lee and Ulf-G. Meißner and Zhengxue Ren}, doi = {10.1103/PhysRevLett.134.162503}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {162503}, shortjournal = {Phys. Rev. Lett.}, title = {Ab initio study of the beryllium isotopes be7 to be12}, volume = {134}, year = {2025}, }
• (2025). Isospin symmetry breaking in the kr71 and br71 mirror system. PRL, 134(16), 162502. (www)

  @article{ , abstract = {Isospin symmetry is a fundamental concept in nuclear physics. Even though isospin symmetry is partially broken, it holds approximately for most nuclear systems, which makes exceptions very interesting from the nuclear structure perspective. In this framework, it is expected that the spins and parities of the ground states of mirror nuclei should be the same, in particular for the simplest systems where a proton is exchanged with a neutron or vice versa. In this Letter, we present evidence that this assumption is broken in the mirror pair Br 71 and Kr 71 system. Our conclusions are based on a high-statistics β decay study of Kr 71 and on state-of-the-art shell model calculations. In our work, we also found evidence of a new state in Se 70 , populated in the β -delayed proton emission process which can be interpreted as the long sought coexisting 0 + state.}, archive = {J_PRL}, author = {A. Algora and A. Vitéz-Sveiczer and A. Poves and G. G. Kiss and B. Rubio and G. de Angelis and F. Recchia and S. Nishimura and T. Rodriguez and P. Sarriguren and J. Agramunt and V. Guadilla and A. Montaner-Pizá and A. I. Morales and S. E. A. Orrigo and D. Napoli and S. M. Lenzi and A. Boso and V. H. Phong and J. Wu and P.-A. Söderström and T. Sumikama and H. Suzuki and H. Takeda and D. S. Ahn and H. Baba and P. Doornenbal and N. Fukuda and N. Inabe and T. Isobe and T. Kubo and S. Kubono and H. Sakurai and Y. Shimizu and S. Chen and B. Blank and P. Ascher and M. Gerbaux and T. Goigoux and J. Giovinazzo and S. Grévy and T. Kurtukián Nieto and C. Magron and W. Gelletly and Zs. Dombrádi and Y. Fujita and M. Tanaka and P. Aguilera and F. Molina and J. Eberth and F. Diel and D. Lubos and C. Borcea and E. Ganioglu and D. Nishimura and H. Oikawa and Y. Takei and S. Yagi and W. Korten and G. de France and P. Davies and J. Liu and J. Lee and T. Lokotko and I. Kojouharov and N. Kurz and H. Schaffner and A. T. Kruppa}, doi = {10.1103/PhysRevLett.134.162502}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {162502}, shortjournal = {Phys. Rev. Lett.}, title = {Isospin symmetry breaking in the kr71 and br71 mirror system}, volume = {134}, year = {2025}, }
• (2025). Measurement of h6 ground state energy in an electron scattering experiment at MAMI-a1. PRL, 134(16), 162501. (www)

  @article{ , abstract = {For the first time the neutron-rich hydrogen isotope H 6 was produced in an electron scattering experiment in the reaction Li 7 ( e , e ′ p π + ) 6 H using the spectrometer facility of the A1 Collaboration at the Mainz Microtron accelerator. By measuring the triple coincidence between the scattered electron, the produced proton, and π + , the missing mass spectrum of H 6 was obtained. A clear peak above H 3 + n + n + n energy threshold was seen resulting in a ground state energy of H 6 at 2.3 ± 0.5 ( stat . ) ± 0.4 ( syst . ) MeV with a width of 1.9 ± 1.0 ( stat . ) ± 0.4 ( syst . ) MeV . This Letter challenges the understandings of multinucleon interactions and presents a new method to study light neutron-rich nuclei with electron scattering experiments.}, archive = {J_PRL}, author = {A1 Collaboration and Tianhao Shao and Jinhui Chen and Josef Pochodzalla and Patrick Achenbach and Mirco Christmann and Michael O. Distler and Luca Doria and Anselm Esser and Julian Geratz and Christian Helmel and Matthias Hoek and Ryoko Kino and Pascal Klag and Yu-Gang Ma and David Markus and Harald Merkel and Miha Mihovilovič and Ulrich Müller and Sho Nagao and Satoshi N. Nakamura and Kotaro Nishi and Ken Nishida and Fumiya Oura and Jonas Pätschke and Björn Sören Schlimme and Concettina Sfienti and Daniel Steger and Marcell Steinen and Michaela Thiel and Andrzej Wilczek and Luca Wilhelm}, doi = {10.1103/PhysRevLett.134.162501}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {162501}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of h6 ground state energy in an electron scattering experiment at MAMI-a1}, volume = {134}, year = {2025}, }
• (2025). Locating critical points using ratios of lee-yang zeros. PRL, 134(16), 162302. (www)

  @article{ , abstract = {We propose a method to numerically determine the location of a critical point in general systems using the finite-size scaling of Lee-Yang zeros. This method makes use of the fact that the ratios of Lee-Yang zeros on various spatial volumes intersect at the critical point. While the method is similar to the Binder-cumulant analysis, it is advantageous in suppressing the finite-volume effects arising from the mixing of variables in general systems. We show that the method works successfully for numerically locating the critical point in the three-dimensional three-state Potts model with a nonzero external field.}, archive = {J_PRL}, author = {Tatsuya Wada and Masakiyo Kitazawa and Kazuyuki Kanaya}, doi = {10.1103/PhysRevLett.134.162302}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {162302}, shortjournal = {Phys. Rev. Lett.}, title = {Locating critical points using ratios of lee-yang zeros}, volume = {134}, year = {2025}, }
• (2025). First measurement of a=4 hypernuclei and antihypernuclei at the LHC. PRL, 134(16), 162301. (www)

  @article{ , abstract = {In this Letter, the first evidence of the He ¯ Λ ¯ 4 antihypernucleus is presented, along with the first measurement at the LHC of the production of (anti)hypernuclei with mass number A = 4 , specifically ( anti ) H Λ 4 and ( anti ) He Λ 4 . In addition, the antiparticle-to-particle ratios for both hypernuclei ( H ¯ Λ ¯ 4 / H Λ 4 and He ¯ Λ ¯ 4 / He Λ 4 ) are shown, which are sensitive to the baryochemical potential of the strongly interacting matter created in heavy-ion collisions. The results are obtained from a data sample of central Pb-Pb collisions, collected during the 2018 LHC data taking at a center-of-mass energy per nucleon pair of s NN = 5.02 TeV . The yields measured for the average of the charge-conjugated states are found to be [ 0.78 ± 0.19 ( stat ) ± 0.17 ( syst ) ] × 10 − 6 for the ( anti ) H Λ 4 and [ 1.08 ± 0.34 ( stat ) ± 0.20 ( syst ) ] × 10 − 6 for the ( anti ) He Λ 4 , and the measured antiparticle-to-particle ratios are in agreement with unity. The presence of ( anti ) H Λ 4 and ( anti ) He Λ 4 excited states is expected to strongly enhance the production yield of these hypernuclei. The yield values exhibit a combined deviation of 3.3 σ from the theoretical ground-state-only expectation, while the inclusion of the excited states in the calculations leads to an agreement within 0.6 σ with the present measurements. Additionally, the measured ( anti ) H Λ 4 and ( anti ) He Λ 4 masses are compatible with the world-average values within the uncertainties.}, archive = {J_PRL}, author = {ALICE Collaboration and S. Acharya and A. Agarwal and G. Aglieri Rinella and L. Aglietta and M. Agnello and N. Agrawal and Z. Ahammed and S. Ahmad and S. U. Ahn and I. Ahuja and A. Akindinov and V. Akishina and M. Al-Turany and D. Aleksandrov and B. Alessandro and H. M. Alfanda and R. Alfaro Molina and B. Ali and A. Alici and N. Alizadehvandchali and A. Alkin and J. Alme and G. Alocco and T. Alt and A. R. Altamura and I. Altsybeev and J. R. Alvarado and C. O. R. Alvarez and M. N. Anaam and C. Andrei and N. Andreou and A. Andronic and E. Andronov and V. Anguelov and F. Antinori and P. Antonioli and N. Apadula and L. Aphecetche and H. Appelshäuser and C. Arata and S. Arcelli and R. Arnaldi and J. G. M. C. A. Arneiro and I. C. Arsene and M. Arslandok and A. Augustinus and R. Averbeck and D. Averyanov and M. D. Azmi and H. Baba and A. Badalà and J. Bae and Y. W. Baek and X. Bai and R. Bailhache and Y. Bailung and R. Bala and A. Balbino and A. Baldisseri and B. Balis and Z. Banoo and V. Barbasova and F. Barile and L. Barioglio and M. Barlou and B. Barman and G. G. Barnaföldi and L. S. Barnby and E. Barreau and V. Barret and L. Barreto and C. Bartels and K. Barth and E. Bartsch and N. Bastid and S. Basu and G. Batigne and D. Battistini and B. Batyunya and D. Bauri and J. L. Bazo Alba and I. G. Bearden and C. Beattie and P. Becht and D. Behera and I. Belikov and A. D. C. Bell Hechavarria and F. Bellini and R. Bellwied and S. Belokurova and L. G. E. Beltran and Y. A. V. Beltran and G. Bencedi and A. Bensaoula and S. Beole and Y. Berdnikov and A. Berdnikova and L. Bergmann and M. G. Besoiu and L. Betev and P. P. Bhaduri and A. Bhasin and B. Bhattacharjee and L. Bianchi and J. Bielčík and J. Bielčíková and A. P. Bigot and A. Bilandzic and G. Biro and S. Biswas and N. Bize and J. T. Blair and D. Blau and M. B. Blidaru and N. Bluhme and C. Blume and G. Boca and F. Bock and T. Bodova and J. Bok and L. Boldizsár and M. Bombara and P. M. Bond and G. Bonomi and H. Borel and A. Borissov and A. G. Borquez Carcamo and E. Botta and Y. E. M. Bouziani and L. Bratrud and P. Braun-Munzinger and M. Bregant and M. Broz and G. E. Bruno and V. D. Buchakchiev and M. D. Buckland and D. Budnikov and H. Buesching and S. Bufalino and P. Buhler and N. Burmasov and Z. Buthelezi and A. Bylinkin and S. A. Bysiak and J. C. Cabanillas Noris and M. F. T. Cabrera and M. Cai and H. Caines and A. Caliva and E. Calvo Villar and J. M. M. Camacho and P. Camerini and F. D. M. Canedo and S. L. Cantway and M. Carabas and A. A. Carballo and F. Carnesecchi and R. Caron and L. A. D. Carvalho and J. Castillo Castellanos and M. Castoldi and F. Catalano and S. Cattaruzzi and R. Cerri and I. Chakaberia and P. Chakraborty and S. Chandra and S. Chapeland and M. Chartier and S. Chattopadhay and S. Chattopadhyay and M. Chen and T. Cheng and C. Cheshkov and V. Chibante Barroso and D. D. Chinellato and E. S. Chizzali and J. Cho and S. Cho and P. Chochula and Z. A. Chochulska and D. Choudhury and P. Christakoglou and C. H. Christensen and P. Christiansen and T. Chujo and M. Ciacco and C. Cicalo and M. R. Ciupek and G. Clai and F. Colamaria and J. S. Colburn and D. Colella and A. Colelli and M. Colocci and M. Concas and G. Conesa Balbastre and Z. Conesa del Valle and G. Contin and J. G. Contreras and M. L. Coquet and P. Cortese and M. R. Cosentino and F. Costa and S. Costanza and C. Cot and P. Crochet and M. M. Czarnynoga and A. Dainese and G. Dange and M. C. Danisch and A. Danu and P. Das and S. Das and A. R. Dash and S. Dash and A. De Caro and G. de Cataldo and J. de Cuveland and A. De Falco and D. De Gruttola and N. De Marco and C. De Martin and S. De Pasquale and R. Deb and R. Del Grande and L. Dello Stritto and W. Deng and K. C. Devereaux and P. Dhankher and D. Di Bari and A. Di Mauro and B. Di Ruzza and B. Diab and R. A. Diaz and T. Dietel and Y. Ding and J. Ditzel and R. Divià and Ø. Djuvsland and U. Dmitrieva and A. Dobrin and B. Dönigus and J. M. Dubinski and A. Dubla and P. Dupieux and N. Dzalaiova and T. M. Eder and R. J. Ehlers and F. Eisenhut and R. Ejima and D. Elia and B. Erazmus and F. Ercolessi and B. Espagnon and G. Eulisse and D. Evans and S. Evdokimov and L. Fabbietti and M. Faggin and J. Faivre and F. Fan and W. Fan and A. Fantoni and M. Fasel and A. Feliciello and G. Feofilov and A. Fernández Téllez and L. Ferrandi and M. B. Ferrer and A. Ferrero and C. Ferrero and A. Ferretti and V. J. G. Feuillard and V. Filova and D. Finogeev and F. M. Fionda and E. Flatland and F. Flor and A. N. Flores and S. Foertsch and I. Fokin and S. Fokin and U. Follo and E. Fragiacomo and E. Frajna and U. Fuchs and N. Funicello and C. Furget and A. Furs and T. Fusayasu and J. J. Gaardhøje and M. Gagliardi and A. M. Gago and T. Gahlaut and C. D. Galvan and S. Gami and D. R. Gangadharan and P. Ganoti and C. Garabatos and J. M. Garcia and T. García Chávez and E. Garcia-Solis and C. Gargiulo and P. Gasik and H. M. Gaur and A. Gautam and M. B. Gay Ducati and M. Germain and R. A. Gernhaeuser and C. Ghosh and M. Giacalone and G. Gioachin and S. K. Giri and P. Giubellino and P. Giubilato and A. M. C. Glaenzer and P. Glässel and E. Glimos and D. J. Q. Goh and V. Gonzalez and P. Gordeev and M. Gorgon and K. Goswami and S. Gotovac and V. Grabski and L. K. Graczykowski and E. Grecka and A. Grelli and C. Grigoras and V. Grigoriev and S. Grigoryan and F. Grosa and J. F. Grosse-Oetringhaus and R. Grosso and D. Grund and N. A. Grunwald and G. G. Guardiano and R. Guernane and M. Guilbaud and K. Gulbrandsen and J. J. W. K. Gumprecht and T. Gündem and T. Gunji and W. Guo and A. Gupta and R. Gupta and K. Gwizdziel and L. Gyulai and C. Hadjidakis and F. U. Haider and S. Haidlova and M. Haldar and H. Hamagaki and Y. Han and B. G. Hanley and R. Hannigan and J. Hansen and M. R. Haque and J. W. Harris and A. Harton and M. V. Hartung and H. Hassan and D. Hatzifotiadou and P. Hauer and L. B. Havener and E. Hellbär and H. Helstrup and M. Hemmer and T. Herman and S. G. Hernandez and G. Herrera Corral and S. Herrmann and K. F. Hetland and B. Heybeck and H. Hillemanns and B. Hippolyte and I. P. M. Hobus and F. W. Hoffmann and B. Hofman and G. H. Hong and M. Horst and A. Horzyk and Y. Hou and P. Hristov and P. Huhn and L. M. Huhta and T. J. Humanic and A. Hutson and D. Hutter and M. C. Hwang and R. Ilkaev and M. Inaba and G. M. Innocenti and M. Ippolitov and A. Isakov and T. Isidori and M. S. Islam and S. Iurchenko and M. Ivanov and V. Ivanov and K. E. Iversen and M. Jablonski and B. Jacak and N. Jacazio and P. M. Jacobs and S. Jadlovska and J. Jadlovsky and S. Jaelani and C. Jahnke and M. J. Jakubowska and M. A. Janik and T. Janson and S. Ji and S. Jia and T. Jiang and A. A. P. Jimenez and F. Jonas and D. M. Jones and J. M. Jowett and J. Jung and M. Jung and A. Junique and A. Jusko and J. Kaewjai and P. Kalinak and A. Kalweit and A. Karasu Uysal and D. Karatovic and N. Karatzenis and O. Karavichev and T. Karavicheva and E. Karpechev and M. J. Karwowska and U. Kebschull and M. Keil and B. Ketzer and J. Keul and S. S. Khade and A. M. Khan and S. Khan and A. Khanzadeev and Y. Kharlov and A. Khatun and A. Khuntia and Z. Khuranova and B. Kileng and B. Kim and C. Kim and D. J. Kim and E. J. Kim and J. Kim and M. Kim and S. Kim and T. Kim and K. Kimura and A. Kirkova and S. Kirsch and I. Kisel and S. Kiselev and A. Kisiel and J. P. Kitowski and J. L. Klay and J. Klein and S. Klein and C. Klein-Bösing and M. Kleiner and T. Klemenz and A. Kluge and C. Kobdaj and R. Kohara and T. Kollegger and A. Kondratyev and N. Kondratyeva and J. Konig and S. A. Konigstorfer and P. J. Konopka and G. Kornakov and M. Korwieser and S. D. Koryciak and C. Koster and A. Kotliarov and N. Kovacic and V. Kovalenko and M. Kowalski and V. Kozhuharov and G. Kozlov and I. Králik and A. Kravčáková and L. Krcal and M. Krivda and F. Krizek and K. Krizkova Gajdosova and C. Krug and M. Krüger and D. M. Krupova and E. Kryshen and V. Kučera and C. Kuhn and P. G. Kuijer and T. Kumaoka and D. Kumar and L. Kumar and N. Kumar and S. Kumar and S. Kundu and P. Kurashvili and A. B. Kurepin and A. Kuryakin and S. Kushpil and V. Kuskov and M. Kutyla and A. Kuznetsov and M. J. Kweon and Y. Kwon and S. L. La Pointe and P. La Rocca and A. Lakrathok and M. Lamanna and A. R. Landou and R. Langoy and P. Larionov and E. Laudi and L. Lautner and R. A. N. Laveaga and R. Lavicka and R. Lea and H. Lee and I. Legrand and G. Legras and J. Lehrbach and A. M. Lejeune and T. M. Lelek and R. C. Lemmon and I. León Monzón and M. M. Lesch and E. D. Lesser and P. Lévai and M. Li and P. Li and X. Li and B. E. Liang-gilman and J. Lien and R. Lietava and I. Likmeta and B. Lim and S. H. Lim and V. Lindenstruth and C. Lippmann and D. H. Liu and J. Liu and G. S. S. Liveraro and I. M. Lofnes and C. Loizides and S. Lokos and J. Lömker and X. Lopez and E. López Torres and C. Lotteau and P. Lu and Z. Lu and F. V. Lugo and J. R. Luhder and M. Lunardon and G. Luparello and Y. G. Ma and M. Mager and A. Maire and E. M. Majerz and M. V. Makariev and M. Malaev and G. Malfattore and N. M. Malik and S. K. Malik and L. Malinina and D. Mallick and N. Mallick and G. Mandaglio and S. K. Mandal and A. Manea and V. Manko and F. Manso and V. Manzari and Y. Mao and R. W. Marcjan and G. V. Margagliotti and A. Margotti and A. Marín and C. Markert and C. F. B. Marquez and P. Martinengo and M. I. Martínez and G. Martínez García and M. P. P. Martins and S. Masciocchi and M. Masera and A. Masoni and L. Massacrier and O. Massen and A. Mastroserio and S. Mattiazzo and A. Matyja and F. Mazzaschi and M. Mazzilli and Y. Melikyan and M. Melo and A. Menchaca-Rocha and J. E. M. Mendez and E. Meninno and A. S. Menon and M. W. Menzel and M. Meres and Y. Miake and L. Micheletti and D. Mihai and D. L. Mihaylov and K. Mikhaylov and N. Minafra and D. Miśkowiec and A. Modak and B. Mohanty and M. Mohisin Khan and M. A. Molander and S. Monira and C. Mordasini and D. A. Moreira De Godoy and I. Morozov and A. Morsch and T. Mrnjavac and V. Muccifora and S. Muhuri and J. D. Mulligan and A. Mulliri and M. G. Munhoz and R. H. Munzer and H. Murakami and S. Murray and L. Musa and J. Musinsky and J. W. Myrcha and B. Naik and A. I. Nambrath and B. K. Nandi and R. Nania and E. Nappi and A. F. Nassirpour and V. Nastase and A. Nath and S. Nath and C. Nattrass and M. N. Naydenov and A. Neagu and A. Negru and E. Nekrasova and L. Nellen and R. Nepeivoda and S. Nese and N. Nicassio and B. S. Nielsen and E. G. Nielsen and S. Nikolaev and S. Nikulin and V. Nikulin and F. Noferini and S. Noh and P. Nomokonov and J. Norman and N. Novitzky and P. Nowakowski and A. Nyanin and J. Nystrand and S. Oh and A. Ohlson and V. A. Okorokov and J. Oleniacz and A. Onnerstad and C. Oppedisano and A. Ortiz Velasquez and J. Otwinowski and M. Oya and K. Oyama and Y. Pachmayer and S. Padhan and D. Pagano and G. Paić and S. Paisano-Guzmán and A. Palasciano and I. Panasenko and S. Panebianco and C. Pantouvakis and H. Park and J. Park and J. E. Parkkila and Y. Patley and R. N. Patra and B. Paul and H. Pei and T. Peitzmann and X. Peng and M. Pennisi and S. Perciballi and D. Peresunko and G. M. Perez and Y. Pestov and M. T. Petersen and V. Petrov and M. Petrovici and S. Piano and M. Pikna and P. Pillot and O. Pinazza and L. Pinsky and C. Pinto and S. Pisano and M. Płoskoń and M. Planinic and F. Pliquett and D. K. Plociennik and M. G. Poghosyan and B. Polichtchouk and S. Politano and N. Poljak and A. Pop and S. Porteboeuf-Houssais and V. Pozdniakov and I. Y. Pozos and K. K. Pradhan and S. K. Prasad and S. Prasad and R. Preghenella and F. Prino and C. A. Pruneau and I. Pshenichnov and M. Puccio and S. Pucillo and S. Qiu and L. Quaglia and A. M. K. Radhakrishnan and S. Ragoni and A. Rai and A. Rakotozafindrabe and L. Ramello and F. Rami and M. Rasa and S. S. Räsänen and R. Rath and M. P. Rauch and I. Ravasenga and K. F. Read and C. Reckziegel and A. R. Redelbach and K. Redlich and C. A. Reetz and H. D. Regules-Medel and A. Rehman and F. Reidt and H. A. Reme-Ness and K. Reygers and A. Riabov and V. Riabov and R. Ricci and M. Richter and A. A. Riedel and W. Riegler and A. G. Riffero and M. Rignanese and C. Ripoli and C. Ristea and M. V. Rodriguez and M. Rodríguez Cahuantzi and S. A. Rodríguez Ramírez and K. Røed and R. Rogalev and E. Rogochaya and T. S. Rogoschinski and D. Rohr and D. Röhrich and S. Rojas Torres and P. S. Rokita and G. Romanenko and F. Ronchetti and E. D. Rosas and K. Roslon and A. Rossi and A. Roy and S. Roy and N. Rubini and J. A. Rudolph and D. Ruggiano and R. Rui and P. G. Russek and R. Russo and A. Rustamov and E. Ryabinkin and Y. Ryabov and A. Rybicki and J. Ryu and W. Rzesa and B. Sabiu and S. Sadovsky and J. Saetre and S. Saha and B. Sahoo and R. Sahoo and S. Sahoo and D. Sahu and P. K. Sahu and J. Saini and K. Sajdakova and S. Sakai and M. P. Salvan and S. Sambyal and D. Samitz and I. Sanna and T. B. Saramela and D. Sarkar and P. Sarma and V. Sarritzu and V. M. Sarti and M. H. P. Sas and S. Sawan and E. Scapparone and J. Schambach and H. S. Scheid and C. Schiaua and R. Schicker and F. Schlepper and A. Schmah and C. Schmidt and H. R. Schmidt and M. O. Schmidt and M. Schmidt and N. V. Schmidt and A. R. Schmier and R. Schotter and A. Schröter and J. Schukraft and K. Schweda and G. Scioli and E. Scomparin and J. E. Seger and Y. Sekiguchi and D. Sekihata and M. Selina and I. Selyuzhenkov and S. Senyukov and J. J. Seo and D. Serebryakov and L. Serkin and L. Šerkšnytė and A. Sevcenco and T. J. Shaba and A. Shabetai and R. Shahoyan and A. Shangaraev and B. Sharma and D. Sharma and H. Sharma and M. Sharma and S. Sharma and U. Sharma and A. Shatat and O. Sheibani and K. Shigaki and M. Shimomura and J. Shin and S. Shirinkin and Q. Shou and Y. Sibiriak and S. Siddhanta and T. Siemiarczuk and T. F. Silva and D. Silvermyr and T. Simantathammakul and R. Simeonov and B. Singh and K. Singh and R. Singh and S. Singh and V. K. Singh and V. Singhal and T. Sinha and B. Sitar and M. Sitta and T. B. Skaali and G. Skorodumovs and N. Smirnov and R. J. M. Snellings and E. H. Solheim and J. Song and C. Sonnabend and J. M. Sonneveld and F. Soramel and A. B. Soto-hernandez and R. Spijkers and I. Sputowska and J. Staa and J. Stachel and I. Stan and P. J. Steffanic and T. Stellhorn and S. F. Stiefelmaier and D. Stocco and I. Storehaug and N. J. Strangmann and P. Stratmann and S. Strazzi and A. Sturniolo and C. P. Stylianidis and A. A. P. Suaide and C. Suire and M. Sukhanov and M. Suljic and R. Sultanov and V. Sumberia and S. Sumowidagdo and M. Szymkowski and L. H. Tabares and S. F. Taghavi and G. Taillepied and J. Takahashi and G. J. Tambave and S. Tang and Z. Tang and J. D. Tapia Takaki and N. Tapus and L. A. Tarasovicova and M. G. Tarzila and G. F. Tassielli and A. Tauro and A. Tavira García and G. Tejeda Muñoz and L. Terlizzi and C. Terrevoli and S. Thakur and D. Thomas and A. Tikhonov and N. Tiltmann and A. R. Timmins and M. Tkacik and T. Tkacik and A. Toia and R. Tokumoto and S. Tomassini and K. Tomohiro and N. Topilskaya and M. Toppi and V. V. Torres and A. G. Torres Ramos and A. Trifiró and T. Triloki and A. S. Triolo and S. Tripathy and T. Tripathy and S. Trogolo and V. Trubnikov and W. H. Trzaska and T. P. Trzcinski and C. Tsolanta and R. Tu and A. Tumkin and R. Turrisi and T. S. Tveter and K. Ullaland and B. Ulukutlu and S. Upadhyaya and A. Uras and M. Urioni and G. L. Usai and M. Vala and N. Valle and L. V. R. van Doremalen and M. van Leeuwen and C. A. van Veen and R. J. G. van Weelden and P. Vande Vyvre and D. Varga and Z. Varga and P. Vargas Torres and M. Vasileiou and A. Vasiliev and O. Vázquez Doce and O. Vazquez Rueda and V. Vechernin and E. Vercellin and R. Verma and L. Vermunt and R. Vértesi and M. Verweij and L. Vickovic and Z. Vilakazi and O. Villalobos Baillie and A. Villani and A. Vinogradov and T. Virgili and M. M. O. Virta and A. Vodopyanov and B. Volkel and M. A. Völkl and S. A. Voloshin and G. Volpe and B. von Haller and I. Vorobyev and N. Vozniuk and J. Vrláková and J. Wan and C. Wang and D. Wang and Y. Wang and Z. Wang and A. Wegrzynek and F. T. Weiglhofer and S. C. Wenzel and J. P. Wessels and J. Wiechula and J. Wikne and G. Wilk and J. Wilkinson and G. A. Willems and B. Windelband and M. Winn and J. R. Wright and W. Wu and Y. Wu and Z. Xiong and R. Xu and A. Yadav and A. K. Yadav and Y. Yamaguchi and S. Yang and S. Yano and E. R. Yeats and Z. Yin and I.-K. Yoo and J. H. Yoon and H. Yu and S. Yuan and A. Yuncu and V. Zaccolo and C. Zampolli and F. Zanone and N. Zardoshti and A. Zarochentsev and P. Závada and N. Zaviyalov and M. Zhalov and B. Zhang and C. Zhang and L. Zhang and M. Zhang and S. Zhang and X. Zhang and Y. Zhang and Z. Zhang and M. Zhao and V. Zherebchevskii and Y. Zhi and D. Zhou and Y. Zhou and J. Zhu and S. Zhu and Y. Zhu and S. C. Zugravel and N. Zurlo}, doi = {10.1103/PhysRevLett.134.162301}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {162301}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of a=4 hypernuclei and antihypernuclei at the LHC}, volume = {134}, year = {2025}, }
• (2025). B→ρℓν¯ resonance form factors from b→ππℓν¯ in lattice QCD. PRL, 134(16), 161901. (www)

  @article{ , abstract = {The decay B → ρ ℓ ν ¯ is an attractive process for determining the magnitude of the smallest Cabibbo-Kobayashi-Maskawa matrix element, | V u b | , and can provide new insights into the origin of the long-standing exclusive-inclusive discrepancy in determinations of this standard-model parameter. This requires a nonperturbative QCD calculation of the B → ρ form factors V , A 0 , A 1 , and A 12 . The unstable nature of the ρ resonance has prevented precise lattice QCD calculations of these form factors to date. Here, we present the first lattice QCD calculation of the B → ρ form factors in which the ρ is treated properly as a resonance in P -wave π π scattering. To this end, we use the Lellouch-Lüscher finite-volume formalism to compute the B → π π form factors as a function of both momentum transfer and π π invariant mass, and then analytically continue to the ρ resonance pole. This calculation is performed with 2 + 1 dynamical quark flavors at a pion mass of approximately 320 MeV, and demonstrates a clear path toward results at the physical point.}, archive = {J_PRL}, author = {Luka Leskovec and Stefan Meinel and Marcus Petschlies and John Negele and Srijit Paul and Andrew Pochinsky}, doi = {10.1103/PhysRevLett.134.161901}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161901}, shortjournal = {Phys. Rev. Lett.}, title = {B→ρℓν¯ resonance form factors from b→ππℓν¯ in lattice QCD}, volume = {134}, year = {2025}, }
• (2025). First double-differential cross section measurement of neutral-current π0 production in neutrino-argon scattering in the MicroBooNE detector. PRL, 134(16), 161802. (www)

  @article{ , abstract = {We report the first double-differential cross section measurement of neutral-current neutral pion ( NC π 0 ) production in neutrino-argon scattering, as well as single-differential measurements of the same channel in terms of final states with and without protons. The kinematic variables of interest for these measurements are the π 0 momentum and the π 0 scattering angle with respect to the neutrino beam. A total of 4971 candidate NC π 0 events fully contained within the MicroBooNE detector are selected using data collected at a mean neutrino energy of ∼ 0.8 GeV from 6.4 × 10 20 protons on target from the Booster Neutrino Beam at the Fermi National Accelerator Laboratory. After extensive data-driven model validation to ensure unbiased unfolding, the Wiener-singular-value-decomposition method is used to extract nominal flux-averaged cross sections. The results are compared to predictions from commonly used neutrino event generators, which tend to overpredict the measured NC π 0 cross section, especially in the 0.2 – 0.5 GeV / c π 0 momentum range and at forward scattering angles. Events with at least one proton present in the final state are also underestimated. This data will help improve the modeling of NC π 0 production, which represents a major background in measurements of charge-parity violation in the neutrino sector and in searches for new physics beyond the standard model.}, archive = {J_PRL}, author = {MicroBooNE Collaboration and P. Abratenko and O. Alterkait and D. Andrade Aldana and L. Arellano and J. Asaadi and A. Ashkenazi and S. Balasubramanian and B. Baller and A. Barnard and G. Barr and D. Barrow and J. Barrow and V. Basque and J. Bateman and O. Benevides Rodrigues and S. Berkman and A. Bhanderi and A. Bhat and M. Bhattacharya and M. Bishai and A. Blake and B. Bogart and T. Bolton and J. Y. Book and M. B. Brunetti and L. Camilleri and Y. Cao and D. Caratelli and F. Cavanna and G. Cerati and A. Chappell and Y. Chen and J. M. Conrad and M. Convery and L. Cooper-Troendle and J. I. Crespo-Anadón and R. Cross and M. Del Tutto and S. R. Dennis and P. Detje and R. Diurba and Z. Djurcic and R. Dorrill and K. Duffy and S. Dytman and B. Eberly and P. Englezos and A. Ereditato and J. J. Evans and R. Fine and W. Foreman and B. T. Fleming and D. Franco and A. P. Furmanski and F. Gao and D. Garcia-Gamez and S. Gardiner and G. Ge and S. Gollapinni and E. Gramellini and P. Green and H. Greenlee and L. Gu and W. Gu and R. Guenette and P. Guzowski and L. Hagaman and M. Handley and O. Hen and C. Hilgenberg and G. A. Horton-Smith and Z. Imani and B. Irwin and M. S. Ismail and C. James and X. Ji and J. H. Jo and R. A. Johnson and Y.-J. Jwa and D. Kalra and N. Kamp and G. Karagiorgi and W. Ketchum and M. Kirby and T. Kobilarcik and I. Kreslo and N. Lane and I. Lepetic and J.-Y. Li and Y. Li and K. Lin and B. R. Littlejohn and H. Liu and W. C. Louis and X. Luo and C. Mariani and D. Marsden and J. Marshall and N. Martinez and D. A. Martinez Caicedo and S. Martynenko and A. Mastbaum and I. Mawby and N. McConkey and V. Meddage and J. Mendez and J. Micallef and K. Miller and A. Mogan and T. Mohayai and M. Mooney and A. F. Moor and C. D. Moore and L. Mora Lepin and M. M. Moudgalya and S. Mulleriababu and D. Naples and A. Navrer-Agasson and N. Nayak and M. Nebot-Guinot and J. Nowak and N. Oza and O. Palamara and N. Pallat and V. Paolone and A. Papadopoulou and V. Papavassiliou and H. B. Parkinson and S. F. Pate and N. Patel and Z. Pavlovic and E. Piasetzky and K. Pletcher and I. Pophale and X. Qian and J. L. Raaf and V. Radeka and A. Rafique and M. Reggiani-Guzzo and L. Ren and L. Rochester and J. Rodriguez Rondon and M. Rosenberg and M. Ross-Lonergan and I. Safa and G. Scanavini and D. W. Schmitz and A. Schukraft and W. Seligman and M. H. Shaevitz and R. Sharankova and J. Shi and E. L. Snider and M. Soderberg and S. Söldner-Rembold and J. Spitz and M. Stancari and J. St. John and T. Strauss and A. M. Szelc and W. Tang and N. Taniuchi and K. Terao and C. Thorpe and D. Torbunov and D. Totani and M. Toups and A. Trettin and Y.-T. Tsai and J. Tyler and M. A. Uchida and T. Usher and B. Viren and J. Wang and M. Weber and H. Wei and A. J. White and S. Wolbers and T. Wongjirad and M. Wospakrik and K. Wresilo and W. Wu and E. Yandel and T. Yang and L. E. Yates and H. W. Yu and G. P. Zeller and J. Zennamo and C. Zhang}, doi = {10.1103/PhysRevLett.134.161802}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161802}, shortjournal = {Phys. Rev. Lett.}, title = {First double-differential cross section measurement of neutral-current π0 production in neutrino-argon scattering in the MicroBooNE detector}, volume = {134}, year = {2025}, }
• (2025). Discovering dark matter with the MUonE experiment. PRL, 134(16), 161801. (www)

  @article{ , abstract = {The MUonE experiment aims to extract the hadronic contribution to the muon anomalous magnetic moment from a precise measurement of the muon-electron differential scattering cross section. We show that MUonE can also discover thermal relic dark matter using only its nominal experimental setup. Our search strategy is sensitive to models of dark matter in which pairs of pseudo-Dirac fermions are produced in muon-nucleus scattering in the target, and the heavier state decays semivisibly to yield dilepton pairs displaced downstream from the interaction point. This approach can probe sub-GeV thermal-relic dark matter whose cosmological abundance is governed by the same model parameters that set the MUonE signal strength. Furthermore, our results show that the downstream electron calorimeter plays a key role in rejecting backgrounds for this search, thereby providing strong motivation for the MUonE to keep this component in the final experimental design.}, archive = {J_PRL}, author = {Gordan Krnjaic and Duncan Rocha and Isaac R. Wang}, doi = {10.1103/PhysRevLett.134.161801}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161801}, shortjournal = {Phys. Rev. Lett.}, title = {Discovering dark matter with the MUonE experiment}, volume = {134}, year = {2025}, }
• (2025). All five-point kaluza-klein correlators and hidden 8D symmetry in AdS5×S3. PRL, 134(16), 161601. (www)

  @article{ , abstract = {We systematically compute five-point correlators of chiral primary operators with arbitrary Kaluza-Klein charges at tree level in AdS 5 × S 3 and obtain a unified formula. This result serves as the first concrete confirmation for the existence of the hidden eight-dimensional symmetries at the level of five points.}, archive = {J_PRL}, author = {Zhongjie Huang (黄中杰 and Bo Wang (王波 and Ellis Ye Yuan (袁野 and Jiarong Zhang (张家荣}, doi = {10.1103/PhysRevLett.134.161601}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161601}, shortjournal = {Phys. Rev. Lett.}, title = {All five-point kaluza-klein correlators and hidden 8D symmetry in AdS5×S3}, volume = {134}, year = {2025}, }
• (2025). Diagonal approximation for holographic rényi entropies. PRL, 134(16), 161501. (www)

  @article{ , abstract = {Recently, Dong et al. , [A modified cosmic brane proposal for holographic Renyi entropy, J. High Energy Phys. 06 ( 2024 ) 120 ] proposed a modified cosmic brane prescription for computing the Rényi entropy S α of a holographic system in the presence of multiple extremal surfaces. This prescription was found by assuming a diagonal approximation, where the Rényi entropy is computed after first measuring the areas of all extremal surfaces. We derive this diagonal approximation for the case of two extremal surfaces and show that it accurately computes Rényi entropies up to O ( log G ) corrections. For α < 1 , this allows us to derive the modified cosmic brane prescription, which differs from the original cosmic brane prescription at leading order in G . For α > 1 , it leads to the original cosmic brane prescription without needing to assume that replica symmetry is unbroken in the bulk.}, archive = {J_PRL}, author = {Geoff Penington and Pratik Rath}, doi = {10.1103/PhysRevLett.134.161501}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161501}, shortjournal = {Phys. Rev. Lett.}, title = {Diagonal approximation for holographic rényi entropies}, volume = {134}, year = {2025}, }
• (2025). Fully nonlinear gravitational wave simulations from past to future null infinity. PRL, 134(16), 161401. (www)

  @article{ , abstract = {We present the first numerical simulations of asymptotically flat space-times whose computational domain includes past and future null infinity. As an application, we explore the scattering of a gravitational wave in a black hole space-time. The study is conducted in the fully nonlinear regime using an initial boundary value problem formulation of Friedrich’s generalized conformal field equations. We calculate the Bondi energy, Bondi news, and gravitational information at both past and future null infinity and discuss their relationships.}, archive = {J_PRL}, author = {Jörg Frauendiener and Chris Stevens and Sebenele Thwala}, doi = {10.1103/PhysRevLett.134.161401}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161401}, shortjournal = {Phys. Rev. Lett.}, title = {Fully nonlinear gravitational wave simulations from past to future null infinity}, volume = {134}, year = {2025}, }
• (2025). Search for light dark matter in low-energy ionization signals from XENONnT. PRL, 134(16), 161004. (www)

  @article{ , abstract = {We report on a blinded search for dark matter with single- and few-electron signals in the first science run of XENONnT relying on a novel detector response framework that is physics model dependent. We derive 90% confidence upper limits for dark matter-electron interactions. Heavy and light mediator cases are considered for the standard halo model and dark matter up-scattered in the Sun. We set stringent new limits on dark matter-electron scattering via a heavy mediator with a mass within and electron absorption of axionlike particles and dark photons for below .}, archive = {J_PRL}, author = {XENON Collaboration and E. Aprile and J. Aalbers and K. Abe and S. Ahmed Maouloud and L. Althueser and B. Andrieu and E. Angelino and D. Antón Martin and F. Arneodo and L. Baudis and M. Bazyk and L. Bellagamba and R. Biondi and A. Bismark and K. Boese and A. Brown and G. Bruno and R. Budnik and C. Cai and C. Capelli and J. M. R. Cardoso and A. P. Cimental Chávez and A. P. Colijn and J. Conrad and J. J. Cuenca-García and V. D’Andrea and L. C. Daniel Garcia and M. P. Decowski and A. Deisting and C. Di Donato and P. Di Gangi and S. Diglio and K. Eitel and S. el Morabit and A. Elykov and A. D. Ferella and C. Ferrari and H. Fischer and T. Flehmke and M. Flierman and W. Fulgione and C. Fuselli and P. Gaemers and R. Gaior and M. Galloway and F. Gao and S. Ghosh and R. Giacomobono and R. Glade-Beucke and L. Grandi and J. Grigat and H. Guan and M. Guida and P. Gyorgy and R. Hammann and A. Higuera and C. Hils and L. Hoetzsch and N. F. Hood and M. Iacovacci and Y. Itow and J. Jakob and F. Joerg and Y. Kaminaga and M. Kara and P. Kavrigin and S. Kazama and M. Kobayashi and D. Koke and A. Kopec and H. Landsman and R. F. Lang and L. Levinson and I. Li and S. Li and S. Liang and Y.-T. Lin and S. Lindemann and M. Lindner and K. Liu and M. Liu and J. Loizeau and F. Lombardi and J. Long and J. A. M. Lopes and T. Luce and Y. Ma and C. Macolino and J. Mahlstedt and A. Mancuso and L. Manenti and F. Marignetti and T. Marrodán Undagoitia and K. Martens and J. Masbou and E. Masson and S. Mastroianni and A. Melchiorre and J. Merz and M. Messina and A. Michael and K. Miuchi and A. Molinario and S. Moriyama and K. Morå and Y. Mosbacher and M. Murra and J. Müller and K. Ni and U. Oberlack and B. Paetsch and Y. Pan and Q. Pellegrini and R. Peres and C. Peters and J. Pienaar and M. Pierre and G. Plante and T. R. Pollmann and L. Principe and J. Qi and J. Qin and D. Ramírez García and M. Rajado and R. Singh and L. Sanchez and J. M. F. dos Santos and I. Sarnoff and G. Sartorelli and J. Schreiner and P. Schulte and H. Schulze Eißing and M. Schumann and L. Scotto Lavina and M. Selvi and F. Semeria and P. Shagin and S. Shi and J. Shi and M. Silva and H. Simgen and C. Szyszka and A. Takeda and P.-L. Tan and D. Thers and F. Toschi and G. Trinchero and C. D. Tunnell and F. Tönnies and K. Valerius and S. Vecchi and S. Vetter and F. I. Villazon Solar and G. Volta and C. Weinheimer and M. Weiss and D. Wenz and C. Wittweg and V. H. S. Wu and Y. Xing and D. Xu and Z. Xu and M. Yamashita and L. Yang and J. Ye and L. Yuan and G. Zavattini and M. Zhong}, doi = {10.1103/PhysRevLett.134.161004}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161004}, shortjournal = {Phys. Rev. Lett.}, title = {Search for light dark matter in low-energy ionization signals from XENONnT}, volume = {134}, year = {2025}, }
• (2025). Search for solar boosted dark matter particles at the PandaX-4T experiment. PRL, 134(16), 161003. (www)

  @article{ , abstract = {We present a novel constraint on light dark matter utilizing 1.54 metric ton/year of data acquired from the PandaX-4T dual-phase xenon time projection chamber. This constraint is derived through detecting electronic recoil signals resulting from the interaction with solar-enhanced dark matter flux. Low-mass dark matter particles, lighter than a few MeV / c 2 , can scatter with the thermal electrons in the Sun. Consequently, with higher kinetic energy, the boosted dark matter component becomes detectable via contact scattering with xenon electrons, resulting in a few keV energy deposition that exceeds the threshold of PandaX-4T. We calculate the expected recoil energy in PandaX-4T considering the Sun’s acceleration with heavy mediators and the detection capabilities of the xenon detector. The first experimental search results using the xenon detector yield the most stringent upper limits cross section of 3.51 × 10 − 39 cm 2 at 0.08 MeV / c 2 for a solar boosted dark matter mass ranging from 0.02 to 10 MeV / c 2 , achieving a 23-fold improvement compared with earlier experimental studies.}, archive = {J_PRL}, author = {PandaX Collaboration and Guofang Shen and Zihao Bo and Wei Chen and Xun Chen and Yunhua Chen and Zhaokan Cheng and Xiangyi Cui and Yingjie Fan and Deqing Fang and Zhixing Gao and Lisheng Geng and Karl Giboni and Xunan Guo and Xuyuan Guo and Zichao Guo and Chencheng Han and Ke Han and Changda He and Jinrong He and Di Huang and Houqi Huang and Junting Huang and Ruquan Hou and Yu Hou and Xiangdong Ji and Xiangpan Ji and Yonglin Ju and Chenxiang Li and Jiafu Li and Mingchuan Li and Shuaijie Li and Tao Li and Zhiyuan Li and Qing Lin and Jianglai Liu and Congcong Lu and Xiaoying Lu and Lingyin Luo and Yunyang Luo and Wenbo Ma and Yugang Ma and Yajun Mao and Yue Meng and Xuyang Ning and Binyu Pang and Ningchun Qi and Zhicheng Qian and Xiangxiang Ren and Dong Shan and Xiaofeng Shang and Xiyuan Shao and Manbin Shen and Wenliang Sun and Yi Tao and Anqing Wang and Guanbo Wang and Hao Wang and Jiamin Wang and Lei Wang and Meng Wang and Qiuhong Wang and Shaobo Wang and Siguang Wang and Wei Wang and Xiuli Wang and Xu Wang and Zhou Wang and Yuehuan Wei and Weihao Wu and Yuan Wu and Mengjiao Xiao and Xiang Xiao and Kaizhi Xiong and Yifan Xu and Shunyu Yao and Binbin Yan and Xiyu Yan and Yong Yang and Peihua Ye and Chunxu Yu and Ying Yuan and Zhe Yuan and Youhui Yun and Xinning Zeng and Minzhen Zhang and Peng Zhang and Shibo Zhang and Shu Zhang and Tao Zhang and Wei Zhang and Yang Zhang and Yingxin Zhang and Yuanyuan Zhang and Li Zhao and Jifang Zhou and Jiaxu Zhou and Jiayi Zhou and Ning Zhou and Xiaopeng Zhou and Yubo Zhou and Zhizhen Zhou and Haipeng An and Haoming Nie}, doi = {10.1103/PhysRevLett.134.161003}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161003}, shortjournal = {Phys. Rev. Lett.}, title = {Search for solar boosted dark matter particles at the PandaX-4T experiment}, volume = {134}, year = {2025}, }
• (2025). SENSEI at SNOLAB: Single-electron event rate and implications for dark matter. PRL, 134(16), 161002. (www)

  @article{ , abstract = {We present results from data acquired by the SENSEI experiment at SNOLAB after a major upgrade in May 2023, which includes deploying 16 new sensors and replacing the copper trays that house the CCDs with a new light-tight design. We observe a single-electron event rate of ( 1.39 ± 0.11 ) × 10 − 5 e − / pix / day , corresponding to ( 39.8 ± 3.1 ) e − / gram / day . This is an order-of-magnitude improvement compared to the previous lowest single-electron rate in a silicon detector and the lowest for any photon detector in the wavelength range between near-infrared and ultraviolet. We use these data to obtain a 90% confidence level upper bound of 1.53 × 10 − 5 e − / pix / day and to set constraints on sub-GeV dark matter candidates that produce single-electron events. We hypothesize that the data taken at SNOLAB in the previous run, with an older tray design for the sensors, contained a larger rate of single-electron events due to light leaks. We test this hypothesis using data from the SENSEI detector located in the MINOS cavern at Fermilab.}, archive = {J_PRL}, author = {SENSEI Collaboration and Itay M. Bloch and Ana M. Botti and Mariano Cababie and Gustavo Cancelo and Brenda A. Cervantes-Vergara and Miguel Daal and Ansh Desai and Alex Drlica-Wagner and Rouven Essig and Juan Estrada and Erez Etzion and Guillermo Fernandez Moroni and Stephen E. Holland and Jonathan Kehat and Ian Lawson and Steffon Luoma and Aviv Orly and Santiago E. Perez and Dario Rodrigues and Nathan A. Saffold and Silvia Scorza and Miguel Sofo-Haro and Kelly Stifter and Javier Tiffenberg and Sho Uemura and Edgar Marrufo Villalpando and Tomer Volansky and Federico Winkel and Yikai Wu and Tien-Tien Yu}, doi = {10.1103/PhysRevLett.134.161002}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161002}, shortjournal = {Phys. Rev. Lett.}, title = {SENSEI at SNOLAB: Single-electron event rate and implications for dark matter}, volume = {134}, year = {2025}, }
• (2025). New probe of cosmic birefringence using galaxy polarization and shapes. PRL, 134(16), 161001. (www)

  @article{ , abstract = {We propose a novel statistical method to measure cosmic birefringence and demonstrate its power in probing parity violation due to axions. Exploiting an empirical correlation between the integrated radio polarization direction of a spiral galaxy and its apparent shape, we devise an unbiased minimum-variance estimator for the rotation angle, which should achieve an uncertainty of 5°–15° per galaxy. Large galaxy samples from the forthcoming SKA continuum surveys, together with optical shape catalogs, promise a comparable or even lower noise power spectrum for the rotation angle than in the CMB Stage-IV (CMB-S4) experiment, with different systematics.}, archive = {J_PRL}, author = {Weichen Winston Yin (尹維晨 and Liang Dai (戴亮 and Junwu Huang (黄俊午 and Lingyuan Ji (吉聆远 and Simone Ferraro}, doi = {10.1103/PhysRevLett.134.161001}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {161001}, shortjournal = {Phys. Rev. Lett.}, title = {New probe of cosmic birefringence using galaxy polarization and shapes}, volume = {134}, year = {2025}, }
• (2025). Repeater-based quantum communication protocol: Maximizing teleportation fidelity with minimal entanglement. PRL, 134(16), 160803. (www)

  @article{ , abstract = {Transmitting unknown quantum states to distant locations is crucial for distributed quantum information protocols. The seminal quantum teleportation scheme achieves this feat while requiring prior maximal entanglement between the sender and receiver. In scenarios with noisy entangled states, optimal teleportation fidelity characterizes the efficacy of transmitting the state, demanding the proper selection of local operations at the sender’s and receiver’s ends. The complexity escalates further in long-range communication setups, prompting the consideration of a repeater-based approach, which incorporates arrays of nodes with multiple segments to facilitate the efficient transmission of quantum information. The fidelity of the communication line gets degraded even if a single segment is affected by noise. In such cases, the general wisdom employs the standard entanglement swapping protocol involving maximally entangled states across the noiseless segments and applying maximally entangled basis measurement at the corresponding nodes to achieve optimal fidelity. In this Letter, we propose a more efficient protocol for a certain class of noisy states, achieving the same fidelity as the standard protocol while consuming less amount of entanglement. Our approach ensures optimal teleportation fidelity even when the end-to-end state gets noisier, and thus promises efficient utility of quantum resources in repeater-based distributed quantum protocols.}, archive = {J_PRL}, author = {Arkaprabha Ghosal and Jatin Ghai and Tanmay Saha and Sibasish Ghosh and Mir Alimuddin}, doi = {10.1103/PhysRevLett.134.160803}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160803}, shortjournal = {Phys. Rev. Lett.}, title = {Repeater-based quantum communication protocol: Maximizing teleportation fidelity with minimal entanglement}, volume = {134}, year = {2025}, }
• (2025). Faithful quantum teleportation via a nanophotonic nonlinear bell state analyzer. PRL, 134(16), 160802. (www)

  @article{ , abstract = {Quantum networking protocols, including quantum teleportation and entanglement swapping, use linear-optical Bell state measurements for heralding the distribution and transfer of quantum information. However, a linear-optical Bell state measurement requires identical photons and is susceptible to errors caused by multiphoton emission, fundamentally limiting the efficiency and fidelity of quantum networking protocols. Here we show a nonlinear Bell state analyzer for time-bin encoded photons based on a nanophotonic cavity with a sum-frequency generation efficiency of 4 × 10 − 5 to filter multiphoton emissions, and utilize it for faithful quantum teleportation involving spectrally distinct photons with fidelities ≥ 94 % down to the single-photon level. Our result demonstrates that nonlinear-optical entangling operations, empowered by our efficient nanophotonics platform, can realize faithful quantum information protocols without requiring identical photons and without the fundamental limit on the fidelity of a Bell state measurement imposed by linear optics, which facilitates the realization of practical quantum networks.}, archive = {J_PRL}, author = {Joshua Akin and Yunlei Zhao and Paul G. Kwiat and Elizabeth A. Goldschmidt and Kejie Fang}, doi = {10.1103/PhysRevLett.134.160802}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160802}, shortjournal = {Phys. Rev. Lett.}, title = {Faithful quantum teleportation via a nanophotonic nonlinear bell state analyzer}, volume = {134}, year = {2025}, }
• (2025). Qudit shadow estimation based on the clifford group and the power of a single magic gate. PRL, 134(16), 160801. (www)

  @article{ , abstract = {Shadow estimation is a sample-efficient protocol for learning the properties of a quantum system using randomized measurements, but the current understanding of qudit shadow estimation is quite limited compared with the qubit setting. Here, we clarify the sample complexity of qudit shadow estimation based on the Clifford group, where the local dimension d is an odd prime. Notably, we show that the overhead of qudit shadow estimation over the qubit counterpart is only O ( d ) , which is independent of the qudit number n , although the set of stabilizer states may deviate exponentially from a 3-design with respect to the third moment operator. Furthermore, by adding one layer of magic gates, we propose a simple circuit that can significantly boost the efficiency. Actually, a single magic gate can already eliminate the O ( d ) overhead in qudit shadow estimation and bridge the gap from the qubit setting.}, archive = {J_PRL}, author = {Chengsi Mao and Changhao Yi and Huangjun Zhu}, doi = {10.1103/PhysRevLett.134.160801}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160801}, shortjournal = {Phys. Rev. Lett.}, title = {Qudit shadow estimation based on the clifford group and the power of a single magic gate}, volume = {134}, year = {2025}, }
• (2025). Scaling advantage in approximate optimization with quantum annealing. PRL, 134(16), 160601. (www)

  @article{ , abstract = {Quantum annealing is a heuristic optimization algorithm that exploits quantum evolution to find low-energy states. Quantum annealers have scaled up in recent years to tackle increasingly larger and more highly connected discrete optimization and quantum simulation problems. Nevertheless, a computational quantum advantage in exact optimization using quantum annealing hardware has so far remained elusive. Here, we present evidence for a quantum annealing scaling advantage in approximate optimization. The advantage is relative to the top classical heuristic algorithm: parallel tempering with isoenergetic cluster moves (PT-ICM). The setting is a family of 2D spin-glass problems with high-precision spin-spin interactions. To achieve this advantage, we implement quantum annealing correction (QAC): an embedding of a bit-flip error-correcting code with energy penalties that leverages the properties of the D-Wave Advantage quantum annealer to yield over 1,300 error-suppressed logical qubits on a degree-5 interaction graph. We generate random spin-glass instances on this graph and benchmark their time-to-epsilon, a generalization of the time-to-solution metric for low-energy states. We demonstrate that, with QAC, quantum annealing exhibits a scaling advantage over PT-ICM at sampling low-energy states with an optimality gap of at least 1.0%. This amounts to the first demonstration of an algorithmic quantum speedup in approximate optimization.}, archive = {J_PRL}, author = {Humberto Munoz-Bauza and Daniel Lidar}, doi = {10.1103/PhysRevLett.134.160601}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160601}, shortjournal = {Phys. Rev. Lett.}, title = {Scaling advantage in approximate optimization with quantum annealing}, volume = {134}, year = {2025}, }
• (2025). Quantum thermodynamic integrability for canonical and noncanonical statistics. PRL, 134(16), 160404. (www)

  @article{ , abstract = {We extend the Carathéodory principle of the second law to quantum thermodynamics, where energy levels depend on macroscopic variables such as volume and magnetic field. This extension introduces the concept of quantum thermodynamic integrability (QTI), providing an alternative foundation for statistical mechanics. QTI is characterized by the path independence of work and heat within the thermodynamic manifold, locally described by energy levels and specific thermodynamic parameters. Within this framework, temperature naturally emerges as an integrating factor, enabling the derivation of both canonical and noncanonical states from the entropy integrable equations based on QTI. Notably, noncanonical states, which become particularly significant outside the thermodynamic limit, reveal the existence of informational correlations in finite-size thermodynamic systems.}, archive = {J_PRL}, author = {R. X. Zhai (翟若迅 and C. P. Sun (孙昌璞}, doi = {10.1103/PhysRevLett.134.160404}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160404}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum thermodynamic integrability for canonical and noncanonical statistics}, volume = {134}, year = {2025}, }
• (2025). Single-particle universality of the many-body spectral form factor. PRL, 134(16), 160403. (www)

  @article{ , abstract = {We consider systems of fermions evolved by noninteracting unitary circuits with correlated on-site potentials. When these potentials are drawn from the eigenvalue distribution of a circular random matrix ensemble, the single-particle sector exhibits chaotic dynamics. The corresponding many-body spectral form factors (SFFs) can be computed exactly , revealing signatures of single-particle chaos in the many-body spectral statistics. Due to the absence of interactions the SFF grows exponentially in time, a result which we demonstrate through simple arguments, scaling collapses, and closed-form evaluation of the SFF. Upon introducing interactions, the SFF crosses over to a linear growth regime consistent with many-body random matrix universality. Our exact results for the SFF provide a baseline for future studies of the crossover between single-particle and many-body random matrix behavior.}, archive = {J_PRL}, author = {Michael O. Flynn and Lev Vidmar and Tatsuhiko N. Ikeda}, doi = {10.1103/PhysRevLett.134.160403}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160403}, shortjournal = {Phys. Rev. Lett.}, title = {Single-particle universality of the many-body spectral form factor}, volume = {134}, year = {2025}, }
• (2025). Quantum thermodynamics with coherence: Covariant gibbs-preserving operation is characterized by the free energy. PRL, 134(16), 160402. (www)

  @article{ , abstract = {The resource theory with covariant Gibbs-preserving operations, also called enhanced thermal operations, is investigated. We prove that with the help of a correlated catalyst, the state convertibility for any coherent state is fully characterized by the free energy defined with the quantum relative entropy. We can extend this result to general resource theories in the form that imposing the covariant condition to a general resource theory does not change the state convertibility, as long as the initial state is coherent and distillable and this resource theory admits the phase estimation and the phase shift. This means that adding a constraint from the law of energy conservation is irrelevant in the correlated-catalytic framework.}, archive = {J_PRL}, author = {Naoto Shiraishi}, doi = {10.1103/PhysRevLett.134.160402}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160402}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum thermodynamics with coherence: Covariant gibbs-preserving operation is characterized by the free energy}, volume = {134}, year = {2025}, }
• (2025). Quantum many-body scars beyond the PXP model in rydberg simulators. PRL, 134(16), 160401. (www)

  @article{ , abstract = {Persistent revivals recently observed in Rydberg atom simulators have challenged our understanding of thermalization and attracted much interest to the concept of quantum many-body scars (QMBSs). QMBSs are non-thermal highly excited eigenstates that coexist with typical eigenstates in the spectrum of many-body Hamiltonians, and have since been reported in multiple theoretical models, including the so-called PXP model, approximately realized by Rydberg simulators. At the same time, questions of how common QMBSs are and in what models they are physically realized remain open. In this Letter, we demonstrate that QMBSs exist in a broader family of models that includes and generalizes PXP to longer-range constraints and states with different periodicity. We show that in each model, multiple QMBS families can be found. Each of them relies on a different approximate su ( 2 ) algebra, leading to oscillatory dynamics in all cases. However, in contrast to the PXP model, their observation requires launching dynamics from weakly entangled initial states rather than from a product state. QMBSs reported here may be experimentally probed using Rydberg atom simulator in the regime of longer-range Rydberg blockades.}, archive = {J_PRL}, author = {Aron Kerschbaumer and Marko Ljubotina and Maksym Serbyn and Jean-Yves Desaules}, doi = {10.1103/PhysRevLett.134.160401}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160401}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum many-body scars beyond the PXP model in rydberg simulators}, volume = {134}, year = {2025}, }
• (2025). Essay: A path for the construction of a muon collider. PRL, 134(16), 160001. (www)

  @article{ , abstract = {Muons are elementary particles and provide cleaner collision events that can explore higher energies compared to composite particles like protons. Muons are also far heavier than their electron cousins, meaning that they emit less synchrotron radiation that effectively limits the energies of circular electron-positron colliders. These characteristics open up the possibility for a muon collider to surpass the direct energy reach of the Large Hadron Collider while achieving unprecedented precision measurements of standard model processes. In this Essay, after briefly summarizing the progress achieved so far, I identify important missing research and development steps and envision a compelling plan to bring a muon collider to reality in the next two decades. A muon collider could allow for the exploration of physics that is not available with current technologies. For example, it may provide a way to study the Higgs boson directly or probe new particles, including those related to dark matter or other phenomena beyond the standard model.}, archive = {J_PRL}, author = {Diktys Stratakis}, doi = {10.1103/PhysRevLett.134.160001}, journal = {Physical Review Letters}, month = {4}, number = {16}, pages = {160001}, shortjournal = {Phys. Rev. Lett.}, title = {Essay: A path for the construction of a muon collider}, volume = {134}, year = {2025}, }
• (2025). Erratum: Gravitational raman scattering in effective field theory: A scalar tidal matching at O(G3) [Phys. rev. lett. 132, 131401 (2024)]. PRL, 134(15), 159901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 159901 (2025)}, archive = {J_PRL}, author = {Mikhail M. Ivanov and Yue-Zhou Li and Julio Parra-Martinez and Zihan Zhou}, doi = {10.1103/PhysRevLett.134.159901}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {159901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Gravitational raman scattering in effective field theory: A scalar tidal matching at O(G3) [Phys. rev. lett. 132, 131401 (2024)]}, volume = {134}, year = {2025}, }
• (2025). Local clustering and global spreading of receptors for optimal spatial gradient sensing. PRL, 134(15), 158401. (www)

  @article{ , abstract = {Spatial information from cell-surface receptors is crucial for processes that require signal processing and sensing of the environment. Here, we investigate the optimal placement of such receptors through a theoretical model that minimizes uncertainty in gradient estimation. Without requiring a priori knowledge of the physical limits of sensing or biochemical processes, we reproduce the emergence of clusters that closely resemble those observed in real cells. On perfect spherical surfaces, optimally placed receptors spread uniformly. When perturbations break their symmetry, receptors cluster in regions of high curvature, massively reducing estimation uncertainty. This agrees in many scenarios with mechanistic models that minimize elastic preference discrepancies between receptors and cell membranes. We further extend our model to motile receptors responding to cell-shape changes and external fluid flow, demonstrating the biological relevance of our model. Our findings provide a simple and utilitarian explanation for receptor clustering at high-curvature regions when high sensing accuracy is paramount.}, archive = {J_PRL}, author = {Albert Alonso and Robert G. Endres and Julius B. Kirkegaard}, doi = {10.1103/PhysRevLett.134.158401}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {158401}, shortjournal = {Phys. Rev. Lett.}, title = {Local clustering and global spreading of receptors for optimal spatial gradient sensing}, volume = {134}, year = {2025}, }
• (2025). Myosin-independent amoeboid cell motility. PRL, 134(15), 158301. (www)

  @article{ , abstract = {Mammalian cell polarization and motility are important processes involved in many physiological and pathological phenomena, such as embryonic development, wound healing, and cancer metastasis. The traditional view of mammalian cell motility suggests that molecular motors, adhesion, and cell deformation are all necessary components for mammalian cell movement. However, experiments on immune system cells have shown that the inhibition of molecular motors does not significantly affect cell motility. We present a new theory and simulations demonstrating that actin polymerization alone is sufficient to induce spontaneously cell polarity accompanied by the retrograde flow. These findings provide a new understanding of the fundamental mechanisms of cell movement and at the same time provide a simple mechanism for cell motility in diverse configurations, e.g., on an adherent substrate, in a nonadherent matrix, or in liquids.}, archive = {J_PRL}, author = {Winfried Schmidt and Walter Zimmermann and Chaouqi Misbah and Alexander Farutin}, doi = {10.1103/PhysRevLett.134.158301}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {158301}, shortjournal = {Phys. Rev. Lett.}, title = {Myosin-independent amoeboid cell motility}, volume = {134}, year = {2025}, }
• (2025). Micromechanical origin of rate independence of the stress in sheared granular materials. PRL, 134(15), 158201. (www)

  @article{ , abstract = {The stress in slowly sheared granular materials is independent of the shear rate, but individual particles transmit momentum at a rate proportional to the shear rate. How a rate-dependent microscopic momentum flux leads to a rate-independent macroscopic stress is a fundamental, unanswered question. Another prominent feature is the occurrence of large stress fluctuations. Here, we show that the two features are closely related. The fluctuations arise from recurrent jamming-yielding dynamics, with deformation being elastic in the jammed phases and yielding occurring in short bursts. These findings lead to an explanation for the rate independence of the stress.}, archive = {J_PRL}, author = {Ravi Gautam and Prabhu R. Nott}, doi = {10.1103/PhysRevLett.134.158201}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {158201}, shortjournal = {Phys. Rev. Lett.}, title = {Micromechanical origin of rate independence of the stress in sheared granular materials}, volume = {134}, year = {2025}, }
• (2025). Statistical mechanics of heteropolymers from lattice gauge theory. PRL, 134(15), 158101. (www)

  @article{ , abstract = {Lattice models are valuable tools to gain insight into the statistical physics of heteropolymers. We rigorously map the partition function of these models into a vacuum expectation value of a Z 2 lattice gauge theory (LGT), with both fermionic and bosonic degrees of freedom. Because the associated path integral expression is not affected by a sign problem, it is amenable to Monte Carlo (MC) sampling in both the sequence and structure space, unlike conventional polymer field theory. At the same time, since the LGT encoding relies on qubits, it provides a framework for future efforts to capitalize on the development of quantum computing hardware. We discuss two illustrative applications of our formalism: first, we use it to characterize the thermodynamically stable sequences and structures of small heteropolymers consisting of two types of residues. Next, we assess its efficiency to sample ensembles of compact structures, finding that the MC decorrelation time scales only linearly with the chain length.}, archive = {J_PRL}, author = {Veronica Panizza and Alessandro Roggero and Philipp Hauke and Pietro Faccioli}, doi = {10.1103/PhysRevLett.134.158101}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {158101}, shortjournal = {Phys. Rev. Lett.}, title = {Statistical mechanics of heteropolymers from lattice gauge theory}, volume = {134}, year = {2025}, }
• (2025). Dielectric properties of aqueous electrolytes at the nanoscale. PRL, 134(15), 158001. (www)

  @article{ , abstract = {Despite the ubiquity of aqueous electrolytes, the effect of salt on water organization remains controversial. We introduce a nonlocal and nonlinear field theory for the nanoscale polarization of ions and water and derive the electrolyte dielectric response as a function of salt concentration to first order in a loop expansion. By comparison with molecular dynamics simulations, we show that rising salt concentration induces a dielectric permittivity decrement and Debye screening in the longitudinal susceptibility but leaves the water structure remarkably unchanged.}, archive = {J_PRL}, author = {Maximilian R. Becker and Roland R. Netz and Philip Loche and Douwe Jan Bonthuis and Dominique Mouhanna and Hélène Berthoumieux}, doi = {10.1103/PhysRevLett.134.158001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {158001}, shortjournal = {Phys. Rev. Lett.}, title = {Dielectric properties of aqueous electrolytes at the nanoscale}, volume = {134}, year = {2025}, }
• (2025). Shortcuts to adiabaticity across a separatrix. PRL, 134(15), 157201. (www)

  @article{ , abstract = {Shortcuts to adiabaticity are strategies for conserving adiabatic invariants under nonadiabatic (i.e. fast-driving) conditions. Here, we show how to extend classical, Hamiltonian shortcuts to adiabaticity to allow the crossing of a phase-space separatrix—a situation in which a corresponding adiabatic protocol does not exist. Specifically, we show how to construct a time-dependent Hamiltonian that evolves one energy shell to another energy shell across a separatrix. Leveraging this method, we design an erasure procedure whose energy cost bound and fidelity do not depend on the protocol’s duration.}, archive = {J_PRL}, author = {Roi Holtzman and Oren Raz and Christopher Jarzynski}, doi = {10.1103/PhysRevLett.134.157201}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {157201}, shortjournal = {Phys. Rev. Lett.}, title = {Shortcuts to adiabaticity across a separatrix}, volume = {134}, year = {2025}, }
• (2025). Nonequilibrium fluctuation-response relations: From identities to bounds. PRL, 134(15), 157101. (www)

  @article{ , abstract = {In nonequilibrium steady states of Markov jump processes, we derive exact fluctuation-response relations (FRRs) that express the covariance between any pair of currents in terms of static responses in a notably simple form, thus generalizing the fluctuation-dissipation theorem far from equilibrium. We begin by considering perturbations in the symmetric part of the rates. We demonstrate that FRRs imply a hierarchy of thermodynamic bounds. These hierarchies prove the recently conjectured response thermodynamic uncertainty relation, which bounds the ratio between any current’s response and its variance by the entropy production rate (EPR). We furthermore strengthen this bound in two distinct ways, using a partial EPR in one case and a pseudo-EPR in the other. For perturbations in the antisymmetric part of the rates, we show that the ratio between any current’s response and its variance is bounded by traffic, a metric representing the total number of transitions per unit time in the system. As an application, we use FRRs to explain the origin of positive correlations between currents in Coulomb-blockaded systems previously observed in experiments.}, archive = {J_PRL}, author = {Timur Aslyamov and Krzysztof Ptaszyński and Massimiliano Esposito}, doi = {10.1103/PhysRevLett.134.157101}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {157101}, shortjournal = {Phys. Rev. Lett.}, title = {Nonequilibrium fluctuation-response relations: From identities to bounds}, volume = {134}, year = {2025}, }
• (2025). Direct spin-imaging detector based on freestanding magnetic nanomembranes. PRL, 134(15), 157002. (www)

  @article{ , abstract = {An analog of the optical polarizer-analyzer for electrons, a spin filter based on a freestanding ferromagnetic (FM) nanomembrane covering the entrance of the microchannel plate (MCP) was applied for efficient spin filtering and electron amplification in the 2D field of view. To study the spin dependent transmission, we constructed a spin-triode device (spintron), which consists of a compact proximity focused vacuum tube with the Na 2 KSb spin-polarized electron source, the FM-MCP and phosphor screen placed to run parallel to each other. Here, we demonstrate the fabrication of FM nanomembranes consisting of a [ Co / Pt ] superlattice deposited on a freestanding 3 nm SiO 2 layer with a total thickness of 10 nm. The FM-MCP has ∼ 10 6 channels with a single-channel Sherman function S = 0.6 and a transmission of ∼ 1.5 × 10 − 3 in the low electron energy range. The FM-MCP-based device provides a compact optical method for measuring the spin polarization of free electron beams in the imaging mode and is well suited for photoemission spectroscopy and microscopy methods.}, archive = {J_PRL}, author = {O. E. Tereshchenko and V. V. Bakin and S. A. Stepanov and V. A. Golyashov and A. S. Mikaeva and D. A. Kustov and V. S. Rusetsky and S. A. Rozhkov and H. E. Scheibler and A. Yu. Demin}, doi = {10.1103/PhysRevLett.134.157002}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {157002}, shortjournal = {Phys. Rev. Lett.}, title = {Direct spin-imaging detector based on freestanding magnetic nanomembranes}, volume = {134}, year = {2025}, }
• (2025). Multipath signal-selective metasurface: Passive time-varying interlocking mechanism to vary spatial impedance for signals with the same frequency. PRL, 134(15), 157001. (www)

  @article{ , abstract = {Electromagnetic (EM) multipath interference is difficult to address with passive approaches due to two physical restrictions—the shared frequency of the initial and interfering signals and their variable incident angles. Thus, to address multipath interference, the spatial impedance, i.e., the impedance structured in three-dimensional space, must be adjusted in response to the incident angles of multiple signals with the same frequency, which is impossible with classic linear time-invariant (LTI) systems. We present a design concept for metasurface-based spatial filters to overcome LTI behavior and suppress multipath interference signals using a time-varying interlocking mechanism without any active biasing systems. The proposed filters are comprised of metasurface panels and internally coupled circuit elements including MOSFETs, which permit accepting only the first incoming wave, while adjusting the spatial impedance to reject time-delayed waves from different angles. The proposed concept is numerically and experimentally validated to have a shielding effectiveness of more than 10 dB. This Letter opens a new avenue for passive yet time-varying selective EM metasystems, enabling the adjustment of spatially complicated EM waves and fields even at the same frequency.}, archive = {J_PRL}, author = {Kaito Tachi and Kota Suzuki and Kairi Takimoto and Shunsuke Saruwatari and Kiichi Niitsu and Ryo Ikeya and Tayaallen Ramachandran and Atsuko Nagata and Peter Njogu and Hiroki Wakatsuchi}, doi = {10.1103/PhysRevLett.134.157001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {157001}, shortjournal = {Phys. Rev. Lett.}, title = {Multipath signal-selective metasurface: Passive time-varying interlocking mechanism to vary spatial impedance for signals with the same frequency}, volume = {134}, year = {2025}, }
• (2025). Second harmonic generation due to the spatial structure of a radiation beam. PRL, 134(15), 156901. (www)

  @article{ , abstract = {We show that spatially structured radiation generates a second harmonic even in homogeneous and isotropic media. The effect originates from the nonlocality of the electric response to the structured electromagnetic field. We develop an analytical theory of such a second harmonic generation in conducting two-dimensional systems. For the general type of structured radiation, we calculate the emerging electric currents at the double frequency and the emitted second harmonic radiation. The theory applied to twisted light reveals that the angular momentum of light doubles in the second harmonic emission. Our results pave the way for light second harmonic generation and structuring beyond the constraints imposed by crystal symmetry.}, archive = {J_PRL}, author = {A. A. Gunyaga and M. V. Durnev and S. A. Tarasenko}, doi = {10.1103/PhysRevLett.134.156901}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {156901}, shortjournal = {Phys. Rev. Lett.}, title = {Second harmonic generation due to the spatial structure of a radiation beam}, volume = {134}, year = {2025}, }
• (2025). Magnetic vortex dynamics probed by time-resolved magnetic helicoidal dichroism. PRL, 134(15), 156701. (www)

  @article{ , abstract = {The laser excitation of magnetization dynamics without applying external fields is a topic of high interest for its potential applications (e.g., magnetic memories, oscillators, and THz emitters). We explore the use of an ultrashort infrared laser pulse for triggering transient changes in a magnetic vortex, probing the induced dynamics by time-resolved magnetic helicoidal dichroism (MHD) in resonant extreme ultraviolet scattering. MHD describes the optical response of a magnetic sample upon sign reversal of either the light orbital angular momentum or the magnetization and was demonstrated to be sensitive to the sample spin texture. Here, we show that, in addition to the well-known ultrafast demagnetization and remagnetization laser-induced processes, the analysis of the MHD signal, supported by micromagnetic simulations, provides direct evidence of important transient reorganizations of the spin texture. In particular, we find that an ultrafast laser pulse of sufficient intensity can induce a surface transient magnetic texture where the vortex curling direction is reversed with respect to the bulk. This result provides insight into the preparation of metastable complex spin states in magnetic films by optical methods without applying an external field, which is of relevance for novel applications in data storage and manipulation.}, archive = {J_PRL}, author = {Mauro Fanciulli and Matteo Pancaldi and Anda-Elena Stanciu and Matthieu Guer and Emanuele Pedersoli and Dario De Angelis and Primož Rebernik Ribič and David Bresteau and Martin Luttmann and Pietro Carrara and Arun Ravindran and Benedikt Rösner and Christian David and Carlo Spezzani and Michele Manfredda and Ricardo Sousa and Laurent Vila and Ioan Lucian Prejbeanu and Liliana D. Buda-Prejbeanu and Bernard Dieny and Giovanni De Ninno and Flavio Capotondi and Thierry Ruchon and Maurizio Sacchi}, doi = {10.1103/PhysRevLett.134.156701}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {156701}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic vortex dynamics probed by time-resolved magnetic helicoidal dichroism}, volume = {134}, year = {2025}, }
• (2025). Defect-immune sound radiation in a topologically nontrivial hyperbolic metamaterial. PRL, 134(15), 156602. (www)

  @article{ , abstract = {Topological insulators remain steadfast at the forefront of condensed matter physics due to their unique electronic properties. The well-known bulk-boundary correspondence ensures the existence of robust edge or interface states, which are protected by the topological characteristics of the material’s bulk band structure. Moving beyond the bound edge states traditionally emphasized in the literature, we explore how topologically protected states extend to nontrivial radiation away from the confining interfaces. Here, we design a metamaterial whose engineered hyperbolic dispersion entails both chiral and mirror symmetries. We discuss how the associated spin polarization degree of freedom enables defect-immune radiation with a variety of tunable directive far-field patterns. Our experiments unequivocally showcase the topological resilience of acoustic radiation in the wake of willfully added absorptive and obstructive defects, which has the potential to stimulate research into advanced room and urban acoustics.}, archive = {J_PRL}, author = {Yang Zhang and Li-Yang Zheng and Johan Christensen}, doi = {10.1103/PhysRevLett.134.156602}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {156602}, shortjournal = {Phys. Rev. Lett.}, title = {Defect-immune sound radiation in a topologically nontrivial hyperbolic metamaterial}, volume = {134}, year = {2025}, }
• (2025). Non-hermitian topology in multiterminal superconducting junctions. PRL, 134(15), 156601. (www)

  @article{ , abstract = {Recent experimental advancements in dissipation control have yielded significant insights into non-Hermitian Hamiltonians for open quantum systems. Of particular interest are the topological characteristics exhibited by these non-Hermitian systems, that arise from exceptional points—distinct degeneracies unique to such systems. In this Letter, we focus on Andreev bound states in multiterminal Josephson junctions with non-Hermiticity induced by normal metal or ferromagnetic leads. By investigating several systems of different synthetic dimensions and symmetries, we predict fragile and stable non-Hermitian topological phases in these engineered superconducting systems.}, archive = {J_PRL}, author = {David Christian Ohnmacht and Valentin Wilhelm and Hannes Weisbrich and Wolfgang Belzig}, doi = {10.1103/PhysRevLett.134.156601}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {156601}, shortjournal = {Phys. Rev. Lett.}, title = {Non-hermitian topology in multiterminal superconducting junctions}, volume = {134}, year = {2025}, }
• (2025). Unlocking new regimes in fractional quantum hall effect with quaternions. PRL, 134(15), 156501. (www)

  @article{ , abstract = {We demonstrate that formulating the composite-fermion theory of the fractional quantum Hall (FQH) effect in terms of quaternions greatly expands its reach and opens the door into many interesting issues that were previously not amenable to quantitative theoretical investigation. As an illustration, we explore the possibility of a nematic or a charge-density wave instability of the composite-fermion Fermi sea at half-filled Landau level and of the nearby FQH states by looking for a gap closing instability of the neutral magneto-roton excitation. Our quaternion formulation of the FQH effect has been inspired by mathematical developments in the theoretical analyses of gravitational wave modes and cosmic microwave background radiation, where an important role is played by spin-weighted spherical harmonics that are nothing but monopole harmonics appearing in the spherical geometry for the FQH effect.}, archive = {J_PRL}, author = {Mytraya Gattu and J. K. Jain}, doi = {10.1103/PhysRevLett.134.156501}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {156501}, shortjournal = {Phys. Rev. Lett.}, title = {Unlocking new regimes in fractional quantum hall effect with quaternions}, volume = {134}, year = {2025}, }
• (2025). Hydrodynamic modes and operator spreading in a long-range center-of-mass-conserving brownian sachdev-ye-kitaev model. PRL, 134(15), 156301. (www)

  @article{ , abstract = {We study a center-of-mass-conserving Brownian complex Sachdev-Ye-Kitaev model with long-range (power-law) interactions characterized by 1 / r η . The kinetic constraint and long-range interactions conspire to yield rich hydrodynamics associated with the conserved charge, which we reveal by computing the Schwinger-Keldysh effective action. Our result shows that charge transport in this system can be subdiffusive, diffusive, or superdiffusive, with the dynamical exponent controlled by η . We further employ a doubled Hilbert space methodology to derive an effective action for the out-of-time-order correlator, from which we obtain the phase diagram delineating regimes where the light cone is linear or logarithmic. Our results provide a concrete example of a quantum many-body system with kinetic constraint and long-range interactions in which the emergent hydrodynamic modes and out-of-time-order correlator can be computed analytically.}, archive = {J_PRL}, author = {Bai-Lin Cheng and Shao-Kai Jian and Zhi-Cheng Yang}, doi = {10.1103/PhysRevLett.134.156301}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {156301}, shortjournal = {Phys. Rev. Lett.}, title = {Hydrodynamic modes and operator spreading in a long-range center-of-mass-conserving brownian sachdev-ye-kitaev model}, volume = {134}, year = {2025}, }
• (2025). Electron-only magnetic reconnection and inverse magnetic-energy transfer at subion scales. PRL, 134(15), 155201. (www)

  @article{ , abstract = {We derive, and validate numerically, an analytical model for electron-only magnetic reconnection applicable to strongly magnetized plasmas. Our model predicts subion-scale reconnection rates significantly higher than those pertaining to large-scale reconnection, aligning with recent observations and simulations. We apply this reconnection model to the problem of inverse magnetic energy transfer at subion scales. We derive time-dependent scaling laws for the magnetic energy decay and the typical magnetic structure dimensions that differ from those previously found in the magnetohydrodynamics regime. These scaling laws are validated via two- and three-dimensional simulations, demonstrating that subion-scale magnetic fields can reach large, system-size scales via successive coalescence.}, archive = {J_PRL}, author = {Zhuo Liu and Caio Silva and Lucio M. Milanese and Muni Zhou and Noah R. Mandell and Nuno F. Loureiro}, doi = {10.1103/PhysRevLett.134.155201}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {155201}, shortjournal = {Phys. Rev. Lett.}, title = {Electron-only magnetic reconnection and inverse magnetic-energy transfer at subion scales}, volume = {134}, year = {2025}, }
• (2025). Autoresonant removal of fusion products in mirror machines. PRL, 134(15), 155101. (www)

  @article{ , abstract = {Magnetic confinement fusion reactors produce fusion byproduct particles that must be removed for efficient operation. It is suggested to use autoresonance (a continuous phase locking between anharmonic motion and a chirped drive) to remove the fusion products from a magnetic mirror, the simplest magnetic confinement configuration. An analogy to the driven pendulum is established via the guiding center approximation. The full 3D dynamics is simulated for α particles [the products of deuterium-tritium (DT) fusion] in agreement with the approximated 1D model. Monte Carlo simulations sampling the phase space of initial conditions are used to quantify the method’s efficiency. The DT fuel particles are out of the bandwidth of the chirped drive and, therefore, stay in the mirror for ongoing fusion. The method is also applicable for advanced aneutronic reactors, such as p − B 11 .}, archive = {J_PRL}, author = {Eli Gudinetsky and Tal Miller and Ilan Be’ery and Ido Barth}, doi = {10.1103/PhysRevLett.134.155101}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {155101}, shortjournal = {Phys. Rev. Lett.}, title = {Autoresonant removal of fusion products in mirror machines}, volume = {134}, year = {2025}, }
• (2025). Experimental observation of the motion of ions in a resonantly driven plasma wakefield accelerator. PRL, 134(15), 155001. (www)

  @article{ , abstract = {We show experimentally that an effect of motion of ions, observed in a plasma-based accelerator, depends inversely on the plasma ion mass. The effect appears within a single wakefield event and manifests itself as a bunch tail, occurring only when sufficient motion of ions suppresses wakefields. Wakefields are driven resonantly by multiple bunches, and simulation results indicate that the ponderomotive force causes the motion of ions. In this case, the effect is also expected to depend on the amplitude of the wakefields, experimentally confirmed through variations in the drive bunch charge.}, archive = {J_PRL}, author = {AWAKE Collaboration and M. Turner and E. Walter and C. Amoedo and N. Torrado and N. Lopes and A. Sublet and M. Bergamaschi and J. Pucek and J. Mezger and N. van Gils and L. Verra and G. Zevi Della Porta and J. Farmer and A. Clairembaud and F. Pannell and E. Gschwendtner and P. Muggli and R. Agnello and C. C. Ahdida and Y. Andrebe and O. Apsimon and R. Apsimon and J. M. Arnesano and V. Bencini and P. Blanchard and K. P. Blum and P. N. Burrows and B. Buttenschön and A. Caldwell and M. Chung and D. A. Cooke and C. Davut and G. Demeter and A. C. Dexter and S. Doebert and A. Fasoli and R. Fonseca and I. Furno and E. Granados and M. Granetzny and T. Graubner and O. Grulke and E. Guran and J. Henderson and F. Jenko and M. A. Kedves and F. Kraus and M. Krupa and T. Lefevre and L. Liang and S. Liu and K. Lotov and M. Martinez Calderon and S. Mazzoni and P. I. Morales Guzmán and M. Moreira and T. Nechaeva and N. Okhotnikov and C. Pakuza and A. Pardons and K. Pepitone and E. Poimendidou and A. Pukhov and R. L. Ramjiawan and L. Ranc and S. Rey and R. Rossel and H. Saberi and O. Schmitz and E. Senes and F. Silva and L. Silva and B. Spear and C. Stollberg and C. Swain and A. Topaloudis and P. Tuev and F. Velotti and V. Verzilov and J. Vieira and C. Welsch and M. Wendt and M. Wing and J. Wolfenden and B. Woolley and G. Xia and V. Yarygova and M. Zepp}, doi = {10.1103/PhysRevLett.134.155001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {155001}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental observation of the motion of ions in a resonantly driven plasma wakefield accelerator}, volume = {134}, year = {2025}, }
• (2025). Laminar-turbulent patterns in shear flows: Evasion of tipping, saddle-loop bifurcation, and log scaling of the turbulent fraction. PRL, 134(15), 154001. (www)

  @article{ , abstract = {Spatial pattern formation can be a signal for tipping points and abrupt transitions in complex systems. In wall shear flows, the homogeneous turbulent state is disconnected from the laminar one and disappears in a tipping catastrophe scenario. It, however, linearly destabilizes before tipping, giving rise to laminar-turbulent banded patterns. The subcritical transition to turbulence is thus a promising candidate for investigating the evasion of tipping and its consequences in a well-controlled setting. To do so, we analyze a one-dimensional two-scalar fields advection diffusion reaction model of the transition. We characterize the multistability of the nonlinear solutions emerging from the instability and show that the pattern wavelength is selected by turbulent fluctuations. At lower Reynolds numbers, the pattern follows a cascade of destabilizations toward larger and larger, eventually infinite wavelengths. In that limit, the periodic limit cycle associated with the spatial pattern hits the laminar fixed point, resulting in a saddle loop, also called homoclinic, global bifurcation and the emergence of solitary pulse solutions. This saddle-loop scenario predicts a logarithmic divergence of the wavelength, which captures available experimental and numerical data.}, archive = {J_PRL}, author = {Pavan V. Kashyap and Juan F. Marín and Yohann Duguet and Olivier Dauchot}, doi = {10.1103/PhysRevLett.134.154001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {154001}, shortjournal = {Phys. Rev. Lett.}, title = {Laminar-turbulent patterns in shear flows: Evasion of tipping, saddle-loop bifurcation, and log scaling of the turbulent fraction}, volume = {134}, year = {2025}, }
• (2025). Controlling the polarization and vortex charge of γ photons via nonlinear compton scattering. PRL, 134(15), 153802. (www)

  @article{ , abstract = {High-energy vortex γ photons have significant applications in many fields. However, their generation and angular momentum manipulation are still great challenges. Here, we first investigated the generation of vortex γ photons with controllable spin and orbital angular momenta via nonlinear Compton scattering of two-color counter-rotating circularly polarized ( C P ) laser fields. The radiation probabilities of vortex photons are calculated using the semiclassical approach that resolves angular momenta of emitted photons. We find that the angular momenta transferred to emitted photons are determined by the dominating photon absorption channel, leading to a structured spectrum with alternations in helicity and twist directions. By tuning the relative intensity ratio of the two-color C P laser fields, the polarization and vortex charge of the emitted γ photons can be controlled, enabling the generation of C P vortex γ photons with a user-defined polarization and topological charge, which may have multiple applications in nuclear physics, astrophysics, particle physics, etc.}, archive = {J_PRL}, author = {Jing-Jing Jiang and Kai-Hong Zhuang and Jia-Ding Chen and Jian-Xing Li and Yue-Yue Chen}, doi = {10.1103/PhysRevLett.134.153802}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153802}, shortjournal = {Phys. Rev. Lett.}, title = {Controlling the polarization and vortex charge of γ photons via nonlinear compton scattering}, volume = {134}, year = {2025}, }
• (2025). Giant nonreciprocity and gyration through modulation-induced hatano-nelson coupling in integrated photonics. PRL, 134(15), 153801. (www)

  @article{ , abstract = {Asymmetric energy exchange interactions, also known as Hatano-Nelson type couplings, enable the study of non-Hermitian physics and associated phenomena like the non-Hermitian skin effect and exceptional points (EPs). Since these interactions are by definition nonreciprocal, there have been very few options for implementations in integrated photonics. In this work, we show that asymmetric couplings are readily achievable in integrated photonic systems through time-domain dynamic modulation. We experimentally study this concept using a two-resonator photonic molecule produced in a lithium niobate on insulator platform that is electro-optically modulated by rf stimuli. We demonstrate the dynamic tuning of the Hatano-Nelson coupling between the resonators, surpassing the asymmetry that has been achieved in previous work, to reach an EP for the first time. We are additionally able to flip the relative sign of the couplings for opposite directions by going past the EP. Using this capability, we show that the through-chain transport can be configured to exhibit both giant ( ∼ 60 dB ) optical contrast as well as photonic gyration or nonreciprocal π phase contrast.}, archive = {J_PRL}, author = {Oğulcan E. Örsel and Jiho Noh and Penghao Zhu and Jieun Yim and Taylor L. Hughes and Ronny Thomale and Gaurav Bahl}, doi = {10.1103/PhysRevLett.134.153801}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153801}, shortjournal = {Phys. Rev. Lett.}, title = {Giant nonreciprocity and gyration through modulation-induced hatano-nelson coupling in integrated photonics}, volume = {134}, year = {2025}, }
• (2025). Strong intrinsic longitudinal coupling in circuit quantum electrodynamics. PRL, 134(15), 153603. (www)

  @article{ , abstract = {Radiation-pressure interactions between harmonic oscillators have enabled exquisite measurement precision and control, made possible by using strong sideband drives, enhancing the coupling rate while also linearizing the interaction. In this Letter, we demonstrate a strong intrinsic longitudinal coupling, a circuit quantum electrodynamics analog of the radiation-pressure interaction, between a transmon qubit and a linear microwave resonator. A red-detuned sideband drive results in an on-demand Jaynes-Cummings interaction with a high on-off ratio. We measure a longitudinal coupling rate an order of magnitude larger than all decay rates, placing the device in the strong coupling regime. The intrinsic longitudinal interaction demonstrated here will enable the development of high-connectivity quantum information processing hardware and the exploration of the gravitational decoherence of quantum objects.}, archive = {J_PRL}, author = {C. A. Potts and R. C. Dekker and S. Deve and E. W. Strijbis and G. A. Steele}, doi = {10.1103/PhysRevLett.134.153603}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153603}, shortjournal = {Phys. Rev. Lett.}, title = {Strong intrinsic longitudinal coupling in circuit quantum electrodynamics}, volume = {134}, year = {2025}, }
• (2025). Emergence of second-order coherence in the superradiant emission from a free-space atomic ensemble. PRL, 134(15), 153602. (www)

  @article{ , abstract = {We investigate the evolution of the second-order temporal coherence during the emission of a superradiant pulse by an elongated cloud of cold Rb atoms in free space. To do so, we measure the two-times intensity correlation function g N ( 2 ) ( t 1 , t 2 ) following the pulsed excitation of the cloud. By monitoring g N ( 2 ) ( t , t ) during the pulse, we observe the establishment of second-order coherence, and contrast it with the situation where the cloud is initially prepared in a steady state. We compare our findings to the predictions of the Dicke model, using an effective atom number to account for finite size effects, finding that the model reproduces the observed trend at early time. For longer times, we observe a subradiant decay, a feature that goes beyond Dicke’s model. Finally, we measure the g N ( 2 ) ( t 1 , t 2 ) at different times and observe the appearance of anticorrelations during the pulse that are not present when starting from a steady state.}, archive = {J_PRL}, author = {Giovanni Ferioli and Igor Ferrier-Barbut and Antoine Browaeys}, doi = {10.1103/PhysRevLett.134.153602}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153602}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of second-order coherence in the superradiant emission from a free-space atomic ensemble}, volume = {134}, year = {2025}, }
• (2025). Experimental observation of dirac exceptional points. PRL, 134(15), 153601. (www)

  @article{ , abstract = {The energy-level degeneracies, also known as exceptional points (EPs), are crucial for comprehending emerging phenomena in materials and enabling innovative functionalities for devices. Since EPs were proposed over half a century ago, only two types of EPs have been experimentally discovered, revealing intriguing phases of materials such as Dirac and Weyl semimetals. These discoveries have showcased numerous exotic topological properties and novel applications, such as unidirectional energy transfer. Here, we report the observation of a novel type of EP, named the Dirac EP, utilizing a nitrogen-vacancy center in diamond. Two of the eigenvalues are measured to be degenerate at the Dirac EP and remain real in its vicinity. This exotic band topology associated with the Dirac EP enables the preservation of the symmetry when passing through, and makes it possible to achieve adiabatic evolution in non-Hermitian systems. We examined the degeneracy between the two eigenstates by quantum state tomography, confirming that the degenerate point is a Dirac EP rather than a Hermitian degeneracy. Our research of the distinct type of EP contributes a fresh perspective on dynamics in non-Hermitian systems and is potentially valuable for applications in quantum control in non-Hermitian systems and the study of the topological properties of EPs.}, archive = {J_PRL}, author = {Yang Wu and Dongfanghao Zhu and Yunhan Wang and Xing Rong and Jiangfeng Du}, doi = {10.1103/PhysRevLett.134.153601}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153601}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental observation of dirac exceptional points}, volume = {134}, year = {2025}, }
• (2025). Exact spectral properties of fermi polarons in one-dimensional lattices: Anomalous fermi singularities and polaron quasiparticles. PRL, 134(15), 153403. (www)

  @article{ , abstract = {We calculate the exact spectral function of a single impurity repulsively interacting with a bath of fermions in one-dimensional lattices, by deriving the explicit expression of the form factor for both regular Bethe states and the irregular spin-flip state and η -pairing state, based on the exactly solvable one-dimensional Hubbard model. While at low impurity momentum Q ∼ 0 the spectral function is dominated by two power-law Fermi singularities, at large momentum we observe that the two singularities develop into two-sided distributions and eventually become anomalous Fermi singularities at the boundary of the Brillouin zone (i.e., Q = ± π ), with the power-law tails extending toward low energy. Near the quarter filling of the Fermi bath, we also find two broad polaron peaks at large impurity momentum, collectively contributed by many excited many-body states with non-negligible form factors. Our exact results of those distinct features in one-dimensional Fermi polarons, which have no correspondences in two and three dimensions, could be readily probed in cold-atom laboratories by trapping highly imbalanced two-component fermionic atoms into one-dimensional optical lattices.}, archive = {J_PRL}, author = {Hui Hu and Jia Wang and Xia-Ji Liu}, doi = {10.1103/PhysRevLett.134.153403}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153403}, shortjournal = {Phys. Rev. Lett.}, title = {Exact spectral properties of fermi polarons in one-dimensional lattices: Anomalous fermi singularities and polaron quasiparticles}, volume = {134}, year = {2025}, }
• (2025). Fate of thermalization of ultracold fermions with two-body dissipation. PRL, 134(15), 153402. (www)

  @article{ , abstract = {Two-body inelastic collisions arising from chemical reactions are prevalent in ultracold fermionic and bosonic molecular gases. Although recent advancements have achieved quantum degeneracy in these systems, loss dynamics are typically modeled phenomenologically using rate equations that often assume thermalization during chemical reactions. In this study, we employ the inelastic quantum Boltzmann equation to analyze particle loss, temperature evolution, and momentum distributions in single-component Fermi gases from first principles. Our results demonstrate that the conventional particle-number rate equation accurately describes the dynamics in trapped systems but fails to capture the behavior in homogeneous systems. Notably, under pure p -wave inelastic collisions and zero elastic collisions, we find that systems prepared near or above quantum degeneracy remain in a thermal state, whereas systems initialized deep within degeneracy exhibit nonequilibrium dynamics. Our theoretical predictions align well with recent experimental observations in trapped systems, and our claim can be further verified in atomic systems with induced two-body loss in box potentials.}, archive = {J_PRL}, author = {Xin-Yuan Gao and Yangqian Yan}, doi = {10.1103/PhysRevLett.134.153402}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153402}, shortjournal = {Phys. Rev. Lett.}, title = {Fate of thermalization of ultracold fermions with two-body dissipation}, volume = {134}, year = {2025}, }
• (2025). Generation of neutron airy beams. PRL, 134(15), 153401. (www)

  @article{ , abstract = {The Airy wave packet is a solution to the potential-free Schrödinger equation that exhibits remarkable properties such as self-acceleration, nondiffraction, and self-healing. Although Airy beams are now routinely realized with electromagnetic waves and electrons, the implementation with neutrons has remained elusive due to small transverse coherence lengths, low fluence rates, and the absence of neutron lenses. In this Letter, we overcome these challenges through a holographic approach and present the first experimental demonstration of neutron Airy beams. The presented techniques pave the way for fundamental physics studies with Airy beams of nonelementary particles, the development of novel neutron optics components, and the realization of neutron Airy-vortex beams.}, archive = {J_PRL}, author = {Dusan Sarenac and Owen Lailey and Melissa E. Henderson and Huseyin Ekinci and Charles W. Clark and David G. Cory and Lisa DeBeer-Schmitt and Michael G. Huber and Jonathan S. White and Kirill Zhernenkov and Dmitry A. Pushin}, doi = {10.1103/PhysRevLett.134.153401}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153401}, shortjournal = {Phys. Rev. Lett.}, title = {Generation of neutron airy beams}, volume = {134}, year = {2025}, }
• (2025). Rotationally resolved spectroscopy of a single polyatomic molecule. PRL, 134(15), 153002. (www)

  @article{ , abstract = {We report the first rotationally resolved spectrum of a single polyatomic molecular ion in the gas phase. Building upon the recently developed inelastic recoil spectroscopy technique, we have increased spectral resolution by a factor ∼ 10 000 ; sufficient to observe resolved rotational-vibrational transitions of a single, trapped cyclopropenyl cation ( c − C 3 H 3 + ). The precision and sensitivity of IRS shown in this work presents an attractive platform for astrochemistry, single molecule chiral detection, and tests of fundamental physics.}, archive = {J_PRL}, author = {Aaron Calvin and Samuel Kresch and Merrell Brzeczek and Elijah Lane and Lincoln Satterthwaite and Desi Hawkins and David Patterson}, doi = {10.1103/PhysRevLett.134.153002}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153002}, shortjournal = {Phys. Rev. Lett.}, title = {Rotationally resolved spectroscopy of a single polyatomic molecule}, volume = {134}, year = {2025}, }
• (2025). Quantum electrodynamics in strong electromagnetic fields: Substate resolved kα transition energies in heliumlike uranium. PRL, 134(15), 153001. (www)

  @article{ , abstract = {Using novel metallic magnetic calorimeter detectors at the CRYRING@ESR, we recorded x-ray spectra of stored and electron cooled heliumlike uranium ( U 90 + ) with an unmatched spectral resolution of close to 90 eV. This allowed for an accurate determination of the energies of all four components of the K α transitions in U 90 + . We find good agreement with state-of-the-art bound-state QED calculations for the strong-field regime. Our results do not support any systematic deviation between experiment and theory in heliumlike systems, the presence of which was subject of intense debates in recent years.}, archive = {J_PRL}, author = {Ph. Pfäfflein and G. Weber and S. Allgeier and Z. Andelkovic and S. Bernitt and A. I. Bondarev and A. Borovik, Jr and L. Duval and A. Fleischmann and O. Forstner and M. Friedrich and J. Glorius and A. Gumberidze and Ch. Hahn and F. Herfurth and D. Hengstler and M. O. Herdrich and P.-M. Hillenbrand and A. Kalinin and M. Kiffer and F. M. Kröger and M. Kubullek and P. Kuntz and M. Lestinsky and Yu. A. Litvinov and B. Löher and E. B. Menz and T. Over and N. Petridis and S. Ringleb and R. S. Sidhu and U. Spillmann and S. Trotsenko and A. Warczak and B. Zhu and Ch. Enss and Th. Stöhlker}, doi = {10.1103/PhysRevLett.134.153001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {153001}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum electrodynamics in strong electromagnetic fields: Substate resolved kα transition energies in heliumlike uranium}, volume = {134}, year = {2025}, }
• (2025). Universality in the near-side energy-energy correlator. PRL, 134(15), 151901. (www)

  @article{ , abstract = {We investigate the energy-energy correlator (EEC) of hadrons produced on the same side in e + e − annihilation or in leading jets in p p collisions. We observe a remarkable universality of the correlator. Using a nonperturbative transverse momentum dependent (TMD) fragmentation function to model the transition from the “free-hadron” region to the perturbative collinear region, we are able to describe the near-side shapes and peaks over a wide range of energy for both the e + e − annihilation and the p p jet substructure measurements in terms of just two parameters. We present further predictions for the ratio of the projected three-point energy correlator to the EEC. The excellent agreement between our calculations and the experimental data may provide new insights into the role of nonperturbative physics for EECs, and suggests the possibility of exploring nonperturbative TMDs using theoretical tools developed for the energy correlators.}, archive = {J_PRL}, author = {Xiaohui Liu and Werner Vogelsang and Feng Yuan and Hua Xing Zhu}, doi = {10.1103/PhysRevLett.134.151901}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151901}, shortjournal = {Phys. Rev. Lett.}, title = {Universality in the near-side energy-energy correlator}, volume = {134}, year = {2025}, }
• (2025). Axion detection experiments can probe majoron models. PRL, 134(15), 151803. (www)

  @article{ , abstract = {The majoron is a well-motivated light (pseudo-Nambu-Goldstone) boson associated with the spontaneous breaking of a global lepton-number symmetry. In this Letter, we relate the spontaneous breaking scale to its soft-breaking mass by requiring that the majoron is the main component of the dark matter. An electromagnetic-anomalous coupling can be induced by minimally modifying the original majoron model, surprisingly, predicting a parameter region that largely overlaps with the QCD-axion dark matter band. Thus, we expect that axion search experiments to be able to probe majoron models.}, archive = {J_PRL}, author = {Qiuyue Liang and Xavier Ponce Díaz and Tsutomu T. Yanagida}, doi = {10.1103/PhysRevLett.134.151803}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151803}, shortjournal = {Phys. Rev. Lett.}, title = {Axion detection experiments can probe majoron models}, volume = {134}, year = {2025}, }
• (2025). Final search for short-baseline neutrino oscillations with the PROSPECT-I detector at HFIR. PRL, 134(15), 151802. (www)

  @article{ , abstract = {The PROSPECT experiment is designed to perform precise searches for antineutrino disappearance at short distances (7–9 m) from compact nuclear reactor cores. This Letter reports results from a new neutrino oscillation analysis performed using the complete data sample from the PROSPECT-I detector operated at the High Flux Isotope Reactor in 2018. The analysis uses a multiperiod selection of inverse beta decay neutrino interactions with reduced backgrounds and enhanced statistical power to set limits on electron neutrino disappearance caused by mixing with sterile neutrinos with 0.2 – 20 eV 2 mass splittings. Inverse beta decay positron energy spectra from six different reactor-detector distance ranges are found to be statistically consistent with one another, as would be expected in the absence of sterile neutrino oscillations. The data excludes at 95% confidence level the existence of sterile neutrinos in regions above 3 eV 2 previously unexplored by terrestrial experiments, including all space below 10 eV 2 suggested by the recently strengthened Gallium Anomaly. The best-fit point of the Neutrino-4 reactor experiment’s claimed observation of short-baseline oscillation is ruled out at more than 5 standard deviations.}, archive = {J_PRL}, author = {PROSPECT Collaboration and M. Andriamirado and A. B. Balantekin and C. D. Bass and O. Benevides Rodrigues and E. P. Bernard and N. S. Bowden and C. D. Bryan and R. Carr and T. Classen and A. J. Conant and G. Deichert and M. J. Dolinski and A. Erickson and A. Galindo-Uribarri and S. Gokhale and C. Grant and S. Hans and A. B. Hansell and K. M. Heeger and B. Heffron and D. E. Jaffe and S. Jayakumar and J. Koblanski and P. Kunkle and C. E. Lane and B. R. Littlejohn and A. Lozano Sanchez and X. Lu and F. Machado and J. Maricic and M. P. Mendenhall and A. M. Meyer and R. Milincic and P. E. Mueller and H. P. Mumm and R. Neilson and X. Qian and C. Roca and R. Rosero and P. T. Surukuchi and F. Sutanto and D. Venegas-Vargas and P. B. Weatherly and J. Wilhelmi and M. Yeh and C. Zhang and X. Zhang}, doi = {10.1103/PhysRevLett.134.151802}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151802}, shortjournal = {Phys. Rev. Lett.}, title = {Final search for short-baseline neutrino oscillations with the PROSPECT-I detector at HFIR}, volume = {134}, year = {2025}, }
• (2025). Search for a hidden sector scalar from kaon decay in the dimuon final state at ICARUS. PRL, 134(15), 151801. (www)

  @article{ , abstract = {We present a search for long-lived particles (LLPs), produced in kaon decays, that decay to two muons inside the ICARUS neutrino detector. This channel would be a signal of hidden sector models that can address outstanding issues in particle physics such as the strong CP problem and the microphysical origin of dark matter. The search is performed with data collected in the Neutrinos at the Main Injector (NuMI) beam at Fermilab corresponding to 2.41 × 10 20 protons-on-target. No new physics signal is observed, and we set world leading limits on heavy QCD axions, as well as for the Higgs portal scalar among dedicated searches. Limits are also presented in a model-independent way applicable to any new physics model predicting the process K → π + S ( → μ μ ) , for a LLP S . This result is the first search for new physics performed with the ICARUS detector at Fermilab. It paves the way for the future program of LLP searches at ICARUS.}, archive = {J_PRL}, author = {ICARUS Collaboration and F. Abd Alrahman and P. Abratenko and N. Abrego-Martinez and A. Aduszkiewicz and F. Akbar and L. Aliaga Soplin and R. Alvarez Garrote and M. Artero Pons and J. Asaadi and W. F. Badgett and B. Baibussinov and B. Behera and V. Bellini and R. Benocci and J. Berger and S. Berkman and S. Bertolucci and M. Betancourt and F. Boffelli and M. Bonesini and T. Boone and B. Bottino and A. Braggiotti and D. Brailsford and S. J. Brice and V. Brio and C. Brizzolari and H. S. Budd and A. Campani and A. Campos and D. Carber and M. Carneiro and I. Caro Terrazas and H. Carranza and F. Castillo Fernandez and A. Castro and S. Centro and G. Cerati and A. Chatterjee and D. Cherdack and S. Cherubini and N. Chithirasreemadam and M. Cicerchia and T. E. Coan and A. Cocco and M. R. Convery and L. Cooper-Troendle and S. Copello and H. Da Motta and M. Dallolio and A. A. Dange and A. de Roeck and S. Di Domizio and L. Di Noto and C. Di Stefano and D. Di Ferdinando and M. Diwan and S. Dolan and L. Domine and S. Donati and F. Drielsma and J. Dyer and S. Dytman and A. Falcone and C. Farnese and A. Fava and A. Ferrari and N. Gallice and F. G. Garcia and C. Gatto and D. Gibin and A. Gioiosa and W. Gu and A. Guglielmi and G. Gurung and K. Hassinin and H. Hausner and A. Heggestuen and B. Howard and R. Howell and I. Ingratta and C. James and W. Jang and M. Jung and Y.-J. Jwa and L. Kashur and W. Ketchum and J. S. Kim and D.-H. Koh and J. Larkin and Y. Li and C. Mariani and C. M. Marshall and S. Martynenko and N. Mauri and K. S. McFarland and D. P. Méndez and A. Menegolli and G. Meng and O. G. Miranda and A. Mogan and N. Moggi and E. Montagna and C. Montanari and A. Montanari and M. Mooney and G. Moreno-Granados and J. Mueller and M. Murphy and D. Naples and V. C. L. Nguyen and S. Palestini and M. Pallavicini and V. Paolone and R. Papaleo and L. Pasqualini and L. Patrizii and L. Paudel and L. Pelegrina-Gutiérrez and G. Petrillo and C. Petta and V. Pia and F. Pietropaolo and F. Poppi and M. Pozzato and G. Putnam and X. Qian and A. Rappoldi and G. L. Raselli and S. Repetto and F. Resnati and A. M. Ricci and G. Riccobene and E. Richards and M. Rosenberg and M. Rossella and N. Rowe and P. Roy and C. Rubbia and M. Saad and I. Safa and S. Saha and P. Sala and G. Salmoria and S. Samanta and P. Sapienza and A. Scaramelli and A. Scarpelli and D. Schmitz and A. Schukraft and D. Senadheera and S-H. Seo and F. Sergiampietri and G. Sirri and J. S. Smedley and J. Smith and L. Stanco and J. Stewart and H. A. Tanaka and F. Tapia and M. Tenti and K. Terao and F. Terranova and V. Togo and D. Torretta and M. Torti and F. Tortorici and R. Triozzi and Y.-T. Tsai and S. Tufanli and T. Usher and F. Varanini and S. Ventura and M. Vicenzi and C. Vignoli and B. Viren and F. A. Wieler and Z. Williams and R. J. Wilson and P. Wilson and J. Wolfs and T. Wongjirad and A. Wood and E. Worcester and M. Worcester and M. Wospakrik and S. Yadav and H. Yu and J. Yu and A. Zani and J. Zennamo and J. Zettlemoyer and C. Zhang and S. Zucchelli}, doi = {10.1103/PhysRevLett.134.151801}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for a hidden sector scalar from kaon decay in the dimuon final state at ICARUS}, volume = {134}, year = {2025}, }
• (2025). Global symmetries, code ensembles, and sums over geometries. PRL, 134(15), 151603. (www)

  @article{ , abstract = {We consider Abelian topological quantum field theories (TQFTs) in 3D and show that gaugings of invertible global symmetries naturally give rise to additive codes. These codes emerge as nonanomalous subgroups of the 1-form symmetry group, parametrizing the fusion rules of condensable TQFT anyons. The boundary theories dual to TQFTs with a maximal symmetry subgroup gauged, i.e., with the corresponding anyons condensed, are “code” conformal field theories (CFTs). This observation bridges together, in the holographic sense, results on 1-form symmetries of 3D TQFTs with developments connecting codes to 2D CFTs. Building on this relationship, we proceed to consider the ensemble of maximal gaugings (topological boundary conditions) in a general, not necessarily Abelian 3D TQFT, and propose that the resulting ensemble of boundary CFTs has a holographic description as a gravitational theory: the bulk TQFT summed over topologies.}, archive = {J_PRL}, author = {Ahmed Barbar and Anatoly Dymarsky and Alfred D. Shapere}, doi = {10.1103/PhysRevLett.134.151603}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151603}, shortjournal = {Phys. Rev. Lett.}, title = {Global symmetries, code ensembles, and sums over geometries}, volume = {134}, year = {2025}, }
• (2025). AdS3×S3 virasoro-shapiro amplitude with ramond-ramond flux. PRL, 134(15), 151602. (www)

  @article{ , abstract = {We compute the anti–de Sitter Virasoro-Shapiro amplitude for scattering of dilatons in type IIB string theory with pure Ramond-Ramond flux on AdS 3 × S 3 × M 4 for M 4 = T 4 or K 3 , to all orders in α ′ in a small anti–de Sitter curvature expansion. This is achieved by comparing the flat space limit of the dual D1D5 conformal field theory correlator to an ansatz for the amplitude as a world-sheet integral in terms of single valued multiple polylogarithms. The first curvature correction is fully fixed in this way, and satisfies consistency checks in the high energy limit, and by comparison of the energy of massive string operators to a semiclassical expansion. Our result gives infinite predictions for conformal field theory data in the planar limit at strong coupling, which can guide future integrability studies.}, archive = {J_PRL}, author = {Shai M. Chester and De-liang Zhong (钟德亮}, doi = {10.1103/PhysRevLett.134.151602}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151602}, shortjournal = {Phys. Rev. Lett.}, title = {AdS3×S3 virasoro-shapiro amplitude with ramond-ramond flux}, volume = {134}, year = {2025}, }
• (2025). Flow-based sampling for entanglement entropy and the machine learning of defects. PRL, 134(15), 151601. (www)

  @article{ , abstract = {We introduce a novel technique to numerically calculate Rényi entanglement entropies in lattice quantum field theory using generative models. We describe how flow-based approaches can be combined with the replica trick using a custom neural-network architecture around a lattice defect connecting two replicas. Numerical tests for the ϕ 4 scalar field theory in two and three dimensions demonstrate that our technique outperforms state-of-the-art Monte Carlo calculations, and exhibit a promising scaling with the defect size.}, archive = {J_PRL}, author = {Andrea Bulgarelli and Elia Cellini and Karl Jansen and Stefan Kühn and Alessandro Nada and Shinichi Nakajima and Kim A. Nicoli and Marco Panero}, doi = {10.1103/PhysRevLett.134.151601}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151601}, shortjournal = {Phys. Rev. Lett.}, title = {Flow-based sampling for entanglement entropy and the machine learning of defects}, volume = {134}, year = {2025}, }
• (2025). Accessing universal relations of binary neutron star waveforms in massive scalar-tensor theory. PRL, 134(15), 151402. (www)

  @article{ , abstract = {We investigate how the quasiuniversal relations connecting tidal deformability with gravitational waveform characteristics and/or properties of individual neutron stars that were proposed in the literature within general relativity would be influenced in the massive Damour-Esposito-Farese-type scalar-tensor gravity. For this purpose, we systematically perform numerical relativity simulations of ∼ 120 binary neutron-star mergers with varying scalar coupling constants. Although only three neutron-star equations of state are adopted, a clear breach of universality can be observed in the datasets. In addition to presenting difficulties in constructing quasiuniversal relations in alternative gravity theories, we also briefly compare the impacts of non-general-relativity physics on the waveform features and those due to the first order or cross-over quantum chromodynamical phase transition.}, archive = {J_PRL}, author = {Alan Tsz-Lok Lam and Yong Gao and Hao-Jui Kuan and Masaru Shibata and Karim Van Aelst and Kenta Kiuchi}, doi = {10.1103/PhysRevLett.134.151402}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151402}, shortjournal = {Phys. Rev. Lett.}, title = {Accessing universal relations of binary neutron star waveforms in massive scalar-tensor theory}, volume = {134}, year = {2025}, }
• (2025). Observational signatures of highly magnified gravitational waves from compact binary coalescence. PRL, 134(15), 151401. (www)

  @article{ , abstract = {Gravitational lensing has empowered telescopes to discover astronomical objects that are otherwise out of reach without being highly magnified by foreground structures. While we expect gravitational waves (GWs) from compact binary coalescences to also experience lensing, the phenomenology of highly magnified GWs has not been fully exploited. In this Letter, we fill this gap and explore the observational signatures of these highly magnified GWs. We find that these signatures are robust against modeling details and can be used as smoking-gun evidence to confirm the detection of lensing of GWs without any electromagnetic observation. Additionally, diffraction becomes important in some cases, which limits the maximum possible magnification and gives waveform signatures of lensing that can only be observed by GW detectors. Even with current-generation observatories, we are already sensitive to these rare, highly magnified GWs and could use them to probe the high-redshift Universe beyond the usual horizon.}, archive = {J_PRL}, author = {Rico K. L. Lo and Luka Vujeva and Jose María Ezquiaga and Juno C. L. Chan}, doi = {10.1103/PhysRevLett.134.151401}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151401}, shortjournal = {Phys. Rev. Lett.}, title = {Observational signatures of highly magnified gravitational waves from compact binary coalescence}, volume = {134}, year = {2025}, }
• (2025). Dark matter axion search with HAYSTAC phase II. PRL, 134(15), 151006. (www)

  @article{ , abstract = {This Letter reports new results from the HAYSTAC experiment’s search for dark matter axions in our galactic halo. It represents the widest search to date that utilizes squeezing to realize subquantum limited noise. The new results cover 1.71 μ eV of newly scanned parameter space in the mass ranges 17.28 – 18.44 μ eV and 18.71 – 19.46 μ eV . No statistically significant evidence of an axion signal was observed, excluding couplings | g γ | ≥ 2.75 × | g γ KSVZ | and | g γ | ≥ 2.96 × | g γ KSVZ | at the 90% confidence level over the respective region. By combining this data with previously published results using HAYSTAC’s squeezed state receiver, a total of 2.27 μ eV of parameter space has now been scanned between 16.96 – 19.46 μ eV μ eV , excluding | g γ | ≥ 2.86 × | g γ KSVZ | at the 90% confidence level. These results demonstrate the squeezed state receiver’s ability to probe axion models over a significant mass range while achieving a scan rate enhancement relative to a quantum-limited experiment.}, archive = {J_PRL}, author = {HAYSTAC Collaboration and Xiran Bai and M. J. Jewell and J. Echevers and K. van Bibber and A. Droster and Maryam H. Esmat and Sumita Ghosh and Eleanor Graham and H. Jackson and Claire Laffan and S. K. Lamoreaux and A. F. Leder and K. W. Lehnert and S. M. Lewis and R. H. Maruyama and R. D. Nath and N. M. Rapidis and E. P. Ruddy and M. Silva-Feaver and M. Simanovskaia and Sukhman Singh and D. H. Speller and Sabrina Zacarias and Yuqi Zhu}, doi = {10.1103/PhysRevLett.134.151006}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151006}, shortjournal = {Phys. Rev. Lett.}, title = {Dark matter axion search with HAYSTAC phase II}, volume = {134}, year = {2025}, }
• (2025). Neutrinos and gamma rays from beta decays in an active galactic nucleus NGC 1068 jet. PRL, 134(15), 151005. (www)

  @article{ , abstract = {We show that TeV neutrinos and high-energy gamma rays detected from the nearby active galaxy NGC 1068 can simultaneously be explained in a model based on the beta decays of neutrons produced in the photodisintegration of He 4 nuclei on ultraviolet photons in the jet. The photodisintegration of nuclei occurs at energies above several PeV, which explains the 1–100 TeV energies of the observed neutrinos. The TeV gamma-ray flux accompanying the beta decays is expected to be much lower than the neutrino flux, which agrees with the observations of NGC 1068 showing a gamma-ray deficit as compared to the expectations from proton-photon interactions. Furthermore, the synchrotron and inverse Compton gamma-ray flux associated with protons’ Bethe-Heitler pair production and the photopion processes in the jet can be consistent with the observed gamma-ray flux at GeV energies for a plausible range of magnetic fields of jets. This scenario, combining beta decay and Bethe-Heitler, can be applied to other jet Seyfert galaxies such as NGC 4151. Future measurements of the neutrino flavor ratio can help confirm the beta-decay origin of the observed neutrinos.}, archive = {J_PRL}, author = {Koichiro Yasuda and Nobuyuki Sakai and Yoshiyuki Inoue and Alexander Kusenko}, doi = {10.1103/PhysRevLett.134.151005}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151005}, shortjournal = {Phys. Rev. Lett.}, title = {Neutrinos and gamma rays from beta decays in an active galactic nucleus NGC 1068 jet}, volume = {134}, year = {2025}, }
• (2025). First search for dark photon dark matter with a madmax prototype. PRL, 134(15), 151004. (www)

  @article{ , abstract = {We report the first result from a dark photon dark matter search in the mass range from 78.62 to 83.95 μ eV / c 2 with a dielectric haloscope prototype for madmax (Magnetized Disc and Mirror Axion eXperiment). Putative dark photons would convert to detectable photons within a stack consisting of three sapphire disks and a mirror. The emitted power of this system is received by an antenna and successively digitized using a low-noise receiver. No significant signal attributable to dark photons has been observed above the expected background. Assuming unpolarized dark photon dark matter with a local density of ρ χ = 0.3 G eV cm 3 we exclude a dark photon to photon mixing parameter χ > 2.7 × 10 − 12 over the full mass range and χ > 1.1 × 10 − 13 at a mass of 80.57 μ eV / c 2 with a 95% confidence level. This is the first physics result from a madmax prototype and exceeds previous constraints on χ in this mass range by up to almost three orders of magnitude.}, archive = {J_PRL}, author = {span class="sc">madmax Collaboration and J. Egge and D. Leppla-Weber and S. Knirck and B. Ary dos Santos Garcia and D. Bergermann and A. Caldwell and V. Dabhi and C. Diaconu and J. Diehl and G. Dvali and M. Ekmedžić and F. Gallo and E. Garutti and S. Heyminck and F. Hubaut and A. Ivanov and J. Jochum and P. Karst and M. Kramer and D. Kreikemeyer-Lorenzo and C. Krieger and C. Lee and A. Lindner and J. P. A. Maldonado and B. Majorovits and S. Martens and A. Martini and A. Miyazaki and E. Öz and P. Pralavorio and G. Raffelt and A. Ringwald and J. Redondo and S. Roset and N. Salama and J. Schaffran and A. Schmidt and F. Steffen and C. Strandhagen and I. Usherov and H. Wang and G. Wieching and G. Cancelo and M. Di Federico and G. Hoshino and L. Stefanazzi}, doi = {10.1103/PhysRevLett.134.151004}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151004}, shortjournal = {Phys. Rev. Lett.}, title = {First search for dark photon dark matter with a madmax prototype}, volume = {134}, year = {2025}, }
• (2025). Constraints on local primordial non-gaussianity with 3D velocity reconstruction from the kinetic sunyaev-zeldovich effect. PRL, 134(15), 151003. (www)

  @article{ , abstract = {The cosmic velocity field is an unbiased probe of the total matter distribution but is challenging to measure directly at intermediate and high redshifts. The large-scale velocity field imprints a signal in the cosmic microwave background (CMB) through the kinetic Sunyaev-Zeldovich (kSZ) effect. We perform the first 3D reconstruction of the large-scale velocity field from the kSZ effect by applying a quadratic estimator to CMB temperature maps and the 3D positions of galaxies. We do so by combining CMB data from the fifth data release of the Atacama Cosmology Telescope (in combination with Planck) and a spectroscopic galaxy sample from the Sloan Digital Sky Survey. We then measure the galaxy-velocity cross-power spectrum and detect the presence of the kSZ signal at a signal-to-noise ratio of 7.2 σ . Using this galaxy-velocity cross-correlation alone, we constrain the amplitude of local primordial non-Gaussianity finding f NL = − 9 0 − 350 + 210 . This pathfinder measurement sets the stage for joint galaxy-CMB kSZ constraints to significantly enhance the f NL information obtained from galaxy surveys through sample variance cancellation.}, archive = {J_PRL}, author = {Alex Laguë and Mathew S. Madhavacheril and Kendrick M. Smith and Simone Ferraro and Emmanuel Schaan}, doi = {10.1103/PhysRevLett.134.151003}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151003}, shortjournal = {Phys. Rev. Lett.}, title = {Constraints on local primordial non-gaussianity with 3D velocity reconstruction from the kinetic sunyaev-zeldovich effect}, volume = {134}, year = {2025}, }
• (2025). Cooling the shock: New supernova constraints on dark photons. PRL, 134(15), 151002. (www)

  @article{ , abstract = {During the accretion phase of a core-collapse supernova (SN), dark-photon (DP) cooling can be largest in the gain layer below the stalled shock wave. In this way, it could counteract the usual shock rejuvenation by neutrino energy deposition and thus prevent the explosion. This peculiar energy-loss profile derives from the resonant nature of DP production. The largest cooling and thus strongest constraints obtain for DP masses of 0.1–0.4 MeV, a range corresponding to the photon plasma mass in the gain region. Electron-capture supernovae, once observationally unambiguously identified, could provide strong bounds even down to nearly 0.01 MeV. For a coupling strength so small that neutrino-driven explosions are expected to survive, the DP cooling of the core is too small to modify the neutrino signal, i.e., our new argument supersedes the traditional SN1987A cooling bound.}, archive = {J_PRL}, author = {Andrea Caputo and Hans-Thomas Janka and Georg Raffelt and Seokhoon Yun}, doi = {10.1103/PhysRevLett.134.151002}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151002}, shortjournal = {Phys. Rev. Lett.}, title = {Cooling the shock: New supernova constraints on dark photons}, volume = {134}, year = {2025}, }
• (2025). Dwarf galaxies imply dark matter is heavier than 2.2×10−21 eV. PRL, 134(15), 151001. (www)

  @article{ , abstract = {It is widely established that a lower bound on the dark matter particle mass, m , can be obtained by demanding that the de Broglie wavelength in a given galaxy must be smaller than the virial radius of the galaxy, leading to m ≳ 10 − 22 eV when applied to typical dwarf galaxies. This lower limit has never been derived precisely or rigorously. We use stellar kinematical data for the Milky Way satellite galaxy Leo II to self-consistently reconstruct a statistical ensemble of dark matter wave functions and corresponding density profiles. By comparison to a data-driven, model-independent reconstruction, and using a variant of the maximum mean discrepancy as a statistical measure, we determine that a self-consistent description of dark matter in the local Universe requires m > 2.2 × 10 − 21 e V ( C L > 95 % ). This lower limit is free of any assumptions pertaining to cosmology, microphysics (including spin), or dynamics of dark matter, and only assumes that it is predominantly composed of a single bosonic particle species.}, archive = {J_PRL}, author = {Tim Zimmermann and James Alvey and David J. E. Marsh and Malcolm Fairbairn and Justin I. Read}, doi = {10.1103/PhysRevLett.134.151001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {151001}, shortjournal = {Phys. Rev. Lett.}, title = {Dwarf galaxies imply dark matter is heavier than 2.2×10−21 eV}, volume = {134}, year = {2025}, }
• (2025). Experimental demonstration of spontaneous symmetry breaking with emergent multiqubit entanglement. PRL, 134(15), 150406. (www)

  @article{ , abstract = {Spontaneous symmetry breaking (SSB) is crucial to the occurrence of phase transitions. Once a phase transition occurs, a quantum system presents degenerate eigenstates that lack the symmetry of the Hamiltonian. After crossing the critical point, the system is essentially evolved to a quantum superposition of these eigenstates until decoherence sets in. Despite the fundamental importance and potential applications in quantum technologies, such quantum-mechanical SSB phenomena have not been experimentally explored in many-body systems. We here present an experimental demonstration of the SSB process in the Lipkin-Meshkov-Glick model, governed by the competition between the individual driving and intraqubit interaction. The model is realized in a circuit quantum electrodynamics system, where 6 Xmon qubits are coupled in an all-to-all manner through virtual photon exchange mediated by a resonator. The observed nonclassical correlations among these qubits in the symmetry-breaking region go beyond the conventional description of SSB, shedding new light on phase transitions for quantum many-body systems.}, archive = {J_PRL}, author = {Ri-Hua Zheng and Wen Ning and Jia-Hao Lü and Xue-Jia Yu and Fan Wu and Cheng-Lin Deng and Zhen-Biao Yang and Kai Xu and Dongning Zheng and Heng Fan and Shi-Biao Zheng}, doi = {10.1103/PhysRevLett.134.150406}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150406}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental demonstration of spontaneous symmetry breaking with emergent multiqubit entanglement}, volume = {134}, year = {2025}, }
• (2025). Efficient detection of strong-to-weak spontaneous symmetry breaking via the rényi-1 correlator. PRL, 134(15), 150405. (www)

  @article{ , abstract = {Strong-to-weak spontaneous symmetry breaking (SWSSB) has recently emerged as a universal feature of quantum mixed-state phases of matter. While various information-theoretic diagnostics have been proposed to define and characterize SWSSB phases, relating these diagnostics to observables which can be efficiently and scalably probed on modern quantum devices remains challenging. Here we propose a new observable for SWSSB in mixed states, called the Rényi-1 correlator, which naturally suggests a route toward scalably detecting certain SWSSB phases in experiment. Specifically, if the canonical purification (CP) of a given mixed state can be reliably prepared, then SWSSB in the mixed state can be detected via ordinary two-point correlation functions in the CP state. We discuss several simple examples of CP states which can be efficiently prepared on quantum devices, and whose reduced density matrices exhibit SWSSB. The Rényi-1 correlator also satisfies several useful theoretical properties: it naturally inherits a stability theorem recently proven for the closely related fidelity correlator, and it directly defines SWSSB as a particular pattern of ordinary spontaneous symmetry breaking in the CP state.}, archive = {J_PRL}, author = {Zack Weinstein}, doi = {10.1103/PhysRevLett.134.150405}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150405}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient detection of strong-to-weak spontaneous symmetry breaking via the rényi-1 correlator}, volume = {134}, year = {2025}, }
• (2025). Clifford circuits augmented time-dependent variational principle. PRL, 134(15), 150404. (www)

  @article{ , abstract = {The recently proposed Clifford circuits augmented matrix product states (CA-MPSs) [, and , Phys. Rev. Lett. 133 , 190402 (2024) ] seamlessly augment density matrix renormalization groups with Clifford circuits. In CA-MPSs, the entanglement from stabilizers is transferred to the Clifford circuits, which can be easily handled according to the Gottesman-Knill theorem. As a result, an MPS needs only to deal with the nonstabilizer entanglement, which largely reduces the bond dimension and the resource required for the accurate simulation of many-body systems. In this Letter, we generalize CA-MPSs to the framework of the time-dependent variational principle (TDVP) for time evolution simulations. In this method, we apply Clifford circuits to the resulting MPS in each TDVP step with a two-site sweeping process similar as in density matrix renormalization groups, aiming at reducing the entanglement entropy in the MPS, and the Hamiltonian is transformed accordingly using the chosen Clifford circuits. Similar as in CA-MPSs, the Clifford circuits does not increase the number of terms in the Hamiltonian, which makes the overhead very small in the new method. We test this method in X X Z chain, 2D Heisenberg model, and Kitaev honeycomb model. The results show that the Clifford circuits augmented TDVP method can reduce the entanglement entropy in the time evolution process and hence makes the simulation reliable for a longer time. The Clifford circuits augmented time-dependent variational principle provides a useful tool for the simulation of the time evolution process of many-body systems in the future.}, archive = {J_PRL}, author = {Xiangjian Qian and Jiale Huang and Mingpu Qin}, doi = {10.1103/PhysRevLett.134.150404}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150404}, shortjournal = {Phys. Rev. Lett.}, title = {Clifford circuits augmented time-dependent variational principle}, volume = {134}, year = {2025}, }
• (2025). Clifford dressed time-dependent variational principle. PRL, 134(15), 150403. (www)

  @article{ , abstract = {We propose an enhanced time-dependent variational principle (TDVP) algorithm for matrix product states that integrates Clifford disentangling techniques to efficiently manage entanglement growth. By leveraging the Clifford group, which maps Pauli strings to other Pauli strings while maintaining low computational complexity, we introduce a Clifford dressed single-site 1-TDVP scheme. During the TDVP integration, we apply a global Clifford transformation as needed to reduce entanglement by iteratively sweeping over two-qubit Clifford unitaries that connect neighboring sites in a checkerboard pattern. We validate the new algorithm numerically using various quantum many-body models, including both integrable and nonintegrable systems. Our results demonstrate that the Clifford dressed TDVP significantly improves entanglement management and computational efficiency, achieving higher accuracy, extended simulation times, and enhanced precision in computed observables compared to standard TDVP approaches. Additionally, we propose incorporating Clifford gates directly within the two-site 2-TDVP scheme.}, archive = {J_PRL}, author = {Antonio Francesco Mello and Alessandro Santini and Guglielmo Lami and Jacopo De Nardis and Mario Collura}, doi = {10.1103/PhysRevLett.134.150403}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150403}, shortjournal = {Phys. Rev. Lett.}, title = {Clifford dressed time-dependent variational principle}, volume = {134}, year = {2025}, }
• (2025). Time-resolved stochastic dynamics of quantum thermal machines. PRL, 134(15), 150402. (www)

  @article{ , abstract = {Steady-state quantum thermal machines are typically characterized by a continuous flow of heat between different reservoirs. However, at the level of discrete stochastic realizations, heat flow is unraveled as a series of abrupt quantum jumps, each representing an exchange of finite quanta with the environment. In this work, we present a framework that resolves the dynamics of quantum thermal machines into cycles classified as enginelike, coolinglike, or idle. We analyze the statistics of individual cycle types and their durations, enabling us to determine both the fraction of cycles useful for thermodynamic tasks and the average waiting time between cycles of a given type. Central to our analysis is the notion of intermittency, which captures the operational consistency of the machine by assessing the frequency and distribution of idle cycles. Our framework offers a novel approach to characterizing thermal machines, with significant relevance to experiments involving mesoscopic transport through quantum dots.}, archive = {J_PRL}, author = {Abhaya S. Hegde and Patrick P. Potts and Gabriel T. Landi}, doi = {10.1103/PhysRevLett.134.150402}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150402}, shortjournal = {Phys. Rev. Lett.}, title = {Time-resolved stochastic dynamics of quantum thermal machines}, volume = {134}, year = {2025}, }
• (2025). Threefold way for typical entanglement. PRL, 134(15), 150401. (www)

  @article{ , abstract = {A typical quantum state with no symmetry can be realized by letting a random unitary act on a fixed state, and the subsystem entanglement spectrum follows the Laguerre unitary ensemble (LUE). For integer-spin time reversal symmetry, we have an analogous scenario where we prepare a time-reversal symmetric state and let random orthogonal matrices act on it, leading to the Laguerre orthogonal ensemble (LOE). However, for half-integer-spin time reversal symmetry, a straightforward analog leading to the Laguerre symplectic ensemble (LSE) is no longer valid because that time-reversal symmetric state is forbidden by the Kramers’ theorem. We devise a system in which the global time reversal operator is fractionalized on the subsystems, and show that LSE arises in the system. Extending this idea, we incorporate general symmetry fractionalization into the system, and show that the statistics of the entanglement spectrum is decomposed into a direct sum of LOE, LUE, and/or LSE. Here, various degeneracies in the entanglement spectrum may appear, depending on the non-Abelian nature of the symmetry group and the cohomology class of the nontrivial projective representation on the subsystem. Our work establishes the entanglement counterpart of Dyson’s threefold way for Hamiltonians with symmetries.}, archive = {J_PRL}, author = {Haruki Yagi and Ken Mochizuki and Zongping Gong}, doi = {10.1103/PhysRevLett.134.150401}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150401}, shortjournal = {Phys. Rev. Lett.}, title = {Threefold way for typical entanglement}, volume = {134}, year = {2025}, }
• (2025). Quantum liang information flow probe of causality across critical points. PRL, 134(15), 150202. (www)

  @article{ , abstract = {Investigating causation in the quantum domain is crucial. Despite numerous studies of correlations in quantum many-body systems, causation, which is very distinct from correlations, has hardly been studied. We address this by demonstrating the efficacy of the newly established causation measure, quantum Liang information flow, in quantifying causality across phase diagrams of quantum many-body systems. We focus on quantum criticality, which are highly nonclassical points. We extract causation behavior across a spectrum-wide critical point and a ground state second-order phase transition in both integrable and nonintegrable systems. Across criticality, each case exhibits distinct hallmarks, different from correlation measures. We also deduce that quantum causation qualitatively follows the quasiparticle picture of information propagation in integrable systems but exhibits enhanced quantum nonlocality near criticality. At times significantly larger than the spatial separation, it extracts additional features from the equilibrium wave function, leading to a peak just before the critical point for near boundary sites.}, archive = {J_PRL}, author = {Roopayan Ghosh and Bin Yi and Sougato Bose}, doi = {10.1103/PhysRevLett.134.150202}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150202}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum liang information flow probe of causality across critical points}, volume = {134}, year = {2025}, }
• (2025). Experimental single-copy distillation of quantumness from higher-dimensional entanglement. PRL, 134(15), 150201. (www)

  @article{ , abstract = {Entanglement is at the heart of quantum theory and is responsible for various quantum-enabling technologies. In practice, during its preparation, storage, and distribution to the intended recipients, this valuable quantum resource may suffer from noisy interactions that reduce its usefulness for the desired information-processing tasks. Conventional schemes of entanglement distillation aim to alleviate this problem by performing collective operations on multiple copies of these decohered states and sacrificing some of them to recover Bell pairs. However, for this scheme to work, the states to be distilled should already contain a large enough fraction of maximally entangled states before these collective operations. Not all entangled quantum states meet this premise. Here, by using the paradigmatic family of two-qutrit Werner states as an exemplifying example, we experimentally demonstrate how one may use single-copy local filtering operations to meet this requirement and to recover the quantumness hidden in these higher-dimensional states. Among others, our results provide the first proof-of-principle experimental certification of the Bell-nonlocal properties of these intriguing entangled states, the activation of their usefulness for quantum teleportation, dense coding, and an enhancement of their quantum steerability, and hence usefulness for certain discrimination tasks. Our theoretically established lower bounds on the steering robustness of these states, when they admit a symmetric quasiextension or a bosonic symmetric extension, and when they show hidden dense-codability, may also be of independent interest.}, archive = {J_PRL}, author = {Xiao-Xu Fang and Gelo Noel M. Tabia and Kai-Siang Chen and Yeong-Cherng Liang and He Lu}, doi = {10.1103/PhysRevLett.134.150201}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150201}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental single-copy distillation of quantumness from higher-dimensional entanglement}, volume = {134}, year = {2025}, }
• (2025). Editorial: Celebrating the first century of quantum physics and preparing for the next one. PRL, 134(15), 150001. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 150001 (2025)}, archive = {J_PRL}, author = {Dagmar Bruß}, doi = {10.1103/PhysRevLett.134.150001}, journal = {Physical Review Letters}, month = {4}, number = {15}, pages = {150001}, shortjournal = {Phys. Rev. Lett.}, title = {Editorial: Celebrating the first century of quantum physics and preparing for the next one}, volume = {134}, year = {2025}, }
• (2025). Hierarchy of chaotic dynamics in random modular networks. PRL, 134(14), 148402. (www)

  @article{ , abstract = {We introduce a model of randomly connected neural populations and study its dynamics by means of the dynamical mean-field theory and simulations. Our analysis uncovers a rich phase diagram, featuring high- and low-dimensional chaotic phases, separated by a crossover region characterized by low values of the maximal Lyapunov exponent and participation ratio dimension, but with high values of the Lyapunov dimension that change significantly across the region. Counterintuitively, chaos can be attenuated by either adding noise to strongly modular connectivity or by introducing modularity into random connectivity. Extending the model to include a multilevel, hierarchical connectivity reveals that a loose balance between activities across levels drives the system towards the edge of chaos.}, archive = {J_PRL}, author = {Łukasz Kuśmierz and Ulises Pereira-Obilinovic and Zhixin Lu and Dana Mastrovito and Stefan Mihalas}, doi = {10.1103/PhysRevLett.134.148402}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148402}, shortjournal = {Phys. Rev. Lett.}, title = {Hierarchy of chaotic dynamics in random modular networks}, volume = {134}, year = {2025}, }
• (2025). Information gain limit of biomolecular computation. PRL, 134(14), 148401. (www)

  @article{ , abstract = {Biomolecules stochastically occupy different configurations that correspond to distinct functional states. Changing biochemical inputs such as rate constants alters the output probability distribution of configurations, and thus constitutes a form of computation. In the cell, such computations are often coupled to thermodynamic forces such as ATP hydrolysis that drive systems far from equilibrium, resulting in energy expenditure even during times when computations are not being performed. The information-theoretic advantage of this costly computational paradigm is unclear. Here we introduce a theoretical framework showing how much the thermodynamic force enables changes in probability distributions, quantified by the information gain , beyond what is possible at equilibrium. Using this framework, we derive a general expression relating the force to the maximum information gain in an arbitrary computation, revealing how small input changes can exponentially alter outputs. We numerically show that biomolecular systems can closely approach this universal bound, illustrating how energy expenditure is needed to achieve the information processing capabilities observed in nature.}, archive = {J_PRL}, author = {Easun Arunachalam and Milo M. Lin}, doi = {10.1103/PhysRevLett.134.148401}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148401}, shortjournal = {Phys. Rev. Lett.}, title = {Information gain limit of biomolecular computation}, volume = {134}, year = {2025}, }
• (2025). Enhanced stability and chaotic condensates in multispecies nonreciprocal mixtures. PRL, 134(14), 148301. (www)

  @article{ , abstract = {Random nonreciprocal interactions between a large number of conserved densities are shown to enhance the stability of the system toward pattern formation. The enhanced stability is an exact result when the number of species approaches infinity and is confirmed numerically by simulations of the multispecies nonreciprocal Cahn-Hilliard model. Furthermore, the diversity in dynamical patterns increases with an increasing number of components, and novel steady states such as pulsating or spatiotemporally chaotic condensates are observed. Our results may help to unravel the mechanisms by which living systems self-organize via metabolism.}, archive = {J_PRL}, author = {Laya Parkavousi and Navdeep Rana and Ramin Golestanian and Suropriya Saha}, doi = {10.1103/PhysRevLett.134.148301}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148301}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced stability and chaotic condensates in multispecies nonreciprocal mixtures}, volume = {134}, year = {2025}, }
• (2025). Anomalous softness in amorphous matter in the reversible plastic regime. PRL, 134(14), 148204. (www)

  @article{ , abstract = {We study an elastoplastic model of an amorphous solid subject to athermal quasistatic cyclic shear strain. We focus on cycling amplitudes in the so-called reversible-plastic regime where, after a transient, the system locks into a hysteretic limit cycle and returns to the same microscopic configuration after one or more strain cycles. We show that the ground state energy of the terminal limit cycle decreases with increasing cycling amplitude. In analogy to an annealed alloy or an aged colloidal glass, one would expect the states with lower energy to be mechanically harder and to require larger stresses and strains to trigger microscopic rearrangements. However, we show the opposite result: the systems with lower energy cycled at higher strain amplitude are mechanically softer and begin to exhibit plastic rearrangements at smaller stresses and strains within the cycle. We explain this anomaly quantitatively in terms of Eshelby inclusion theory where an inclusion is subjected to a particular negative stress value after it undergoes a yielding event. These results point the way toward measurements to be conducted in experiments and particle-based computer simulations on cyclically sheared amorphous solids.}, archive = {J_PRL}, author = {A. Elgailani and D. Vandembroucq and C. E. Maloney}, doi = {10.1103/PhysRevLett.134.148204}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148204}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous softness in amorphous matter in the reversible plastic regime}, volume = {134}, year = {2025}, }
• (2025). Hyperelastic swelling of stiff hydrogels. PRL, 134(14), 148203. (www)

  @article{ , abstract = {Hydrogels are swollen polymer networks where elastic deformation is coupled to nanoscale fluid flow. As a consequence, hydrogels can withstand large strains and exhibit nonlinear, hyperelastic properties. Previous studies have shown that low-modulus hydrogels and semiflexible biopolymer networks universally contract when sheared on timescales much longer than the poroelastic relaxation timescale. Using rheological and tribological measurements, we find that stiff polyacrylamide and polyacrylic acid hydrogels, with moduli of order , exclusively swell (dilate) when sheared. Poroelastic relaxation was examined using strain-controlled compression, indicating a volumetric diffusion constant of order . Upon shearing, we observed an increase in normal stress that varied quadratically with shear strain, which persisted for hours. Moreover, we show that this dilatant behavior manifests as swelling during tribological sliding, imbibing the hydrogel with fluid. We suggest that this inherent, hyperelastic dilatancy is an important feature in all stiff hydrogels, and may explain rehydration and mechanical rejuvenation in biological tissues such as cartilage.}, archive = {J_PRL}, author = {Jing Wang and Justin C. Burton}, doi = {10.1103/PhysRevLett.134.148203}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148203}, shortjournal = {Phys. Rev. Lett.}, title = {Hyperelastic swelling of stiff hydrogels}, volume = {134}, year = {2025}, }
• (2025). Rheological regimes in agitated granular media under shear. PRL, 134(14), 148202. (www)

  @article{ , abstract = {Agitated granular media have a rich rheology: they exhibit Newtonian behavior at low shear rate and density, develop a yield stress at high density, and cross over to Bagnoldian shear thickening when sheared rapidly—making it challenging to encompass them in one theoretical framework. We measure the rheology of air-fluidized glass particles, spanning 5 orders of magnitude in shear rate. By comparing fluidization-induced to Brownian agitation, we show that all rheological regimes can be delineated by two dimensionless numbers—the Péclet number, Pe, and the ratio of shear-to-fluidization power, —and propose a constitutive relation that captures all flow behaviors, qualitatively and quantitatively, in one unified framework.}, archive = {J_PRL}, author = {Olfa D’Angelo and Matthias Sperl and W. Till Kranz}, doi = {10.1103/PhysRevLett.134.148202}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148202}, shortjournal = {Phys. Rev. Lett.}, title = {Rheological regimes in agitated granular media under shear}, volume = {134}, year = {2025}, }
• (2025). Falsifiability test for classical nucleation theory. PRL, 134(14), 148201. (www)

  @article{ , abstract = {Classical nucleation theory (CNT) is built upon the capillarity approximation, i.e., the assumption that the nucleation properties can be inferred from the bulk properties of the melt and the crystal. Although the simplicity and usefulness of CNT cannot be overstated, experiments and simulations regularly uncover significant deviations from its predictions, which are often reconciled through phenomenological extensions of the CNT, fueling the debate over the general validity of the theory. In this Letter, we present a falsifiability test for any nucleation theory grounded in the capillarity approximation. We focus on cases where the theory predicts no differences in nucleation rates between different crystal polymorphs. We then introduce a system in which all polymorphs have the same free energy (both bulk and interfacial) across all state points. Through extensive molecular simulations, we show that the polymorphs exhibit remarkably different nucleation properties, directly contradicting predictions of CNT. We argue that CNT’s primary limitation lies in its neglect of structural fluctuations within the liquid phase.}, archive = {J_PRL}, author = {Camilla Beneduce and Diogo E. P. Pinto and Lorenzo Rovigatti and Flavio Romano and Petr Šulc and Francesco Sciortino and John Russo}, doi = {10.1103/PhysRevLett.134.148201}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148201}, shortjournal = {Phys. Rev. Lett.}, title = {Falsifiability test for classical nucleation theory}, volume = {134}, year = {2025}, }
• (2025). Real-time visualization of single polymer conformational change in the bulk state during mechanical deformation. PRL, 134(14), 148101. (www)

  @article{ , abstract = {Although polymers are most often used within bulk materials, investigating their conformations and dynamics has long been a challenging endeavor in this configuration, particularly under external forces. Addressing this, we utilize single-molecule localization microscopy as a powerful imaging tool to visualize bottlebrush poly( n -butyl acrylate) chains in the bulk state under spherical indentation, quantitatively describing changes in behavior of single polymer chains. We compare these experiments to displacement fields determined analytically and confirmed through finite element analysis. This study pioneers visualizing polymer conformational changes in their native environment in situ , offering transformative insights into polymer behavior and dynamics.}, archive = {J_PRL}, author = {Ruiqi Xiao and Subhadeep Pal and Christopher P. Rademacher and Jie Chen and Qifeng Wang and Wei Chen and Kenneth R. Shull and Sinan Keten and Muzhou Wang}, doi = {10.1103/PhysRevLett.134.148101}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148101}, shortjournal = {Phys. Rev. Lett.}, title = {Real-time visualization of single polymer conformational change in the bulk state during mechanical deformation}, volume = {134}, year = {2025}, }
• (2025). Learning classical density functionals for ionic fluids. PRL, 134(14), 148001. (www)

  @article{ , abstract = {Accurate and efficient theoretical techniques for describing ionic fluids are highly desirable for many applications across the physical, biological, and materials sciences. With a rigorous statistical mechanical foundation, classical density functional theory (cDFT) is an appealing approach, but the competition between strong Coulombic interactions and steric repulsion limits the accuracy of current approximate functionals. Here, we extend a recently presented machine learning (ML) approach [Sammüller et al. , Proc. Natl. Acad. Sci. U.S.A. , 120 , e2312484120 (2023) ] designed for systems with short-ranged interactions to ionic fluids. By adopting ideas from local molecular field theory, the framework we present amounts to using neural networks to learn the local relationship between the one-body direct correlation functions and inhomogeneous density profiles for a “mimic” short-ranged system, with effects of long-ranged interactions accounted for in a mean-field, yet well-controlled, manner. By comparing to results from molecular simulations, we show that our approach accurately describes the structure and thermodynamics of prototypical models for electrolyte solutions and ionic liquids, including size-asymmetric and multivalent systems. The framework we present acts as an important step toward extending ML approaches for cDFT to systems with accurate interatomic potentials.}, archive = {J_PRL}, author = {Anna T. Bui and Stephen J. Cox}, doi = {10.1103/PhysRevLett.134.148001}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {148001}, shortjournal = {Phys. Rev. Lett.}, title = {Learning classical density functionals for ionic fluids}, volume = {134}, year = {2025}, }
• (2025). Physical networks become what they learn. PRL, 134(14), 147402. (www)

  @article{ , abstract = {Physical networks can develop tuned responses, or functions, by design, by evolution, or by learning via local rules. In all of these cases, tunable degrees of freedom characterizing internal interactions are modified to lower a cost penalizing deviations from desired outputs. An important class of such networks follows dynamics that minimize a global physical quantity, or Lyapunov function, with respect to physical degrees of freedom. In such networks, learning is a “double optimization” process in which two quantities, one defined by the task and the other prescribed by physics, are minimized with respect to different but coupled sets of variables. Here, we show how this learning process couples the high-dimensional “cost landscape” to the “physical landscape,” linking the physical and cost Hessian matrices. Physical responses of trained networks to random perturbations thus reveal the functions to which they were tuned. Our results, illustrated using electrical networks with adaptable resistors, are generic to networks that perform tasks in the linear response regime.}, archive = {J_PRL}, author = {Menachem Stern and Marcelo Guzman and Felipe Martins and Andrea J. Liu and Vijay Balasubramanian}, doi = {10.1103/PhysRevLett.134.147402}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {147402}, shortjournal = {Phys. Rev. Lett.}, title = {Physical networks become what they learn}, volume = {134}, year = {2025}, }
• (2025). Statistical mechanics of frustrated assemblies and incompatible graphs. PRL, 134(14), 147401. (www)

  @article{ , abstract = {Geometrically frustrated assemblies where building blocks misfit have been shown to generate intriguing phenomena from self-limited growth, fiber formation, to structural complexity. We introduce a graph theory formulation of geometrically frustrated assemblies, capturing frustrated interactions through the concept of incompatible flows, providing a direct link between structural connectivity and frustration. This theory offers a minimal yet comprehensive framework for the fundamental statistical mechanics of frustrated assemblies, and connects it to tensor gauge theory formulations of amorphous solids. Through numerical simulations, the theory reveals new characteristics of frustrated assemblies, including two distinct percolation transitions for structure and incompatible flows, a crossover between cumulative and noncumulative frustration controlled by disorder, and a divergent length scale in their response.}, archive = {J_PRL}, author = {José M. Ortiz-Tavárez and Zhen Yang and Nicholas Kotov and Xiaoming Mao}, doi = {10.1103/PhysRevLett.134.147401}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {147401}, shortjournal = {Phys. Rev. Lett.}, title = {Statistical mechanics of frustrated assemblies and incompatible graphs}, volume = {134}, year = {2025}, }
• (2025). Superuniversal statistics of complex time delays in non-hermitian scattering systems. PRL, 134(14), 147203. (www)

  @article{ , abstract = {The Wigner-Smith time delay of flux conserving systems is a real quantity that measures how long an excitation resides in an interaction region. The complex generalization of time delay to non-Hermitian systems is still under development, in particular, its statistical properties in the short-wavelength limit of complex chaotic scattering systems has not been investigated. From the experimentally measured multiport scattering ( ) matrices of one-dimensional graphs, a two-dimensional billiard, and a three-dimensional cavity, we calculate the complex Wigner-Smith ( ), as well as each individual reflection ( ) and transmission ( ) time delay. The complex reflection time-delay differences ( ) between each port are calculated, and the transmission time-delay differences ( ) are introduced for systems exhibiting nonreciprocal scattering. Large time delays are associated with scattering singularities such as coherent perfect absorption, reflectionless scattering, slow light, and unidirectional invisibility. We demonstrate that the large-delay tails of the distributions of the real and imaginary parts of each time-delay quantity are superuniversal, independent of experimental parameters: wave propagation dimension , number of scattering channels , Dyson symmetry class , and uniform attenuation . The tails determine the abundance of the singularities in generic scattering systems, and the superuniversality is in direct contrast with the well-established time-delay statistics of unitary scattering systems, where the tail of the distribution depends explicitly on the values of and . We relate the distribution statistics to the topological properties of the corresponding singularities. Although the results presented here are based on classical microwave experiments, they are applicable to any non-Hermitian wave-chaotic scattering system in the short-wavelength limit, such as optical or acoustic resonators.}, archive = {J_PRL}, author = {Nadav Shaibe and Jared M. Erb and Steven M. Anlage}, doi = {10.1103/PhysRevLett.134.147203}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {147203}, shortjournal = {Phys. Rev. Lett.}, title = {Superuniversal statistics of complex time delays in non-hermitian scattering systems}, volume = {134}, year = {2025}, }
• (2025). Crisis in time-dependent dynamical systems. PRL, 134(14), 147202. (www)

  @article{ , abstract = {Many dynamical systems operate in a fluctuating environment. However, even in low-dimensional setups, transitions and bifurcations have not yet been fully understood. In this Letter we focus on crises, a sudden flooding of the phase space due to the crossing of the boundary of the basin of attraction. We find that crises occur also in nonautonomous systems although the underlying mechanism is more complex. We show that in the vicinity of the transition, the escape probability scales as , where is the distance from the critical point, while is a model-dependent parameter. This prediction is tested and verified in a few different systems, including the Kuramoto model with inertia, where the crisis controls the loss of stability of a chimera state.}, archive = {J_PRL}, author = {Simona Olmi and Antonio Politi}, doi = {10.1103/PhysRevLett.134.147202}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {147202}, shortjournal = {Phys. Rev. Lett.}, title = {Crisis in time-dependent dynamical systems}, volume = {134}, year = {2025}, }
• (2025). Dissipation-driven emergence of a soliton condensate in a nonlinear electrical transmission line. PRL, 134(14), 147201. (www)

  @article{ , abstract = {We present an experimental study on the perturbed evolution of Korteweg–de Vries soliton gases in a weakly dissipative nonlinear electrical transmission line. The system’s dynamics reveal that an initially dense, fully randomized soliton gas evolves into a coherent macroscopic state identified as a soliton condensate through nonlinear spectral analysis. The emergence of the soliton condensate is driven by the spatial rearrangement of the systems’s eigenmodes and by the proliferation of new solitonic states due to nonadiabatic effects, a phenomenon not accounted for by the existing hydrodynamic theories.}, archive = {J_PRL}, author = {Loic Fache and Hervé Damart and François Copie and Thibault Bonnemain and Thibault Congy and Giacomo Roberti and Pierre Suret and Gennady El and Stéphane Randoux}, doi = {10.1103/PhysRevLett.134.147201}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {147201}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipation-driven emergence of a soliton condensate in a nonlinear electrical transmission line}, volume = {134}, year = {2025}, }
• (2025). Generalized einstein relation for markovian friction coefficients from molecular trajectories. PRL, 134(14), 147101. (www)

  @article{ , abstract = {We present a generalized Einstein relation for the friction coefficients associated with an underlying memory kernel in terms of observable time correlation functions. There is considerable freedom in the correlations involved, and this allows the expression to be tailored to the particular system to achieve numerical stability. We demonstrate this by recovering the site-specific friction coefficients from trajectories of a freely diffusing model trimer, and we show that the accuracy is greatly improved over established Volterra inversion methods for kernel extraction.}, archive = {J_PRL}, author = {J. M. Hall and M. G. Guenza}, doi = {10.1103/PhysRevLett.134.147101}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {147101}, shortjournal = {Phys. Rev. Lett.}, title = {Generalized einstein relation for markovian friction coefficients from molecular trajectories}, volume = {134}, year = {2025}, }
• (2025). Nanoscale casimir force softening originated from quantum surface responses. PRL, 134(14), 146901. (www)

  @article{ , abstract = {Strong coupling between vacuum fields and quantum matter occurs at the nanoscale and broadens the horizon of light-matter interaction. Nanoscale Casimir force, as an exhibition of vacuum fields, inevitably experiences the influence of surface electron responses due to their quantum character, which are ignorable in micron Casimir force. Here, we develop a three-dimensional conformal map method to tackle typical experimental configurations with surface electron contributions to Casimir force purposely and delicately included. Based on this method, we reveal that quantum surface responses (QSRs) can either enhance or suppress the nanoscale Casimir force, depending on materials and crystal facets. The mechanism is demonstrated to be the Casimir force softening, which results from QSRs effectively altering the distance seen by the Casimir interaction. With such an understanding, we then provide a recipe to handle the nanoscale Casimir force between nanoscale complex objects. Our findings not only highlight the interaction between QSRs and vacuum fields but also provide a recipe for theoretical and experimental investigation of nanoscale fluctuation-type problems.}, archive = {J_PRL}, author = {Hewan Zhang and Kun Ding}, doi = {10.1103/PhysRevLett.134.146901}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146901}, shortjournal = {Phys. Rev. Lett.}, title = {Nanoscale casimir force softening originated from quantum surface responses}, volume = {134}, year = {2025}, }
• (2025). Emergent surface multiferroicity. PRL, 134(14), 146703. (www)

  @article{ , abstract = {We show that the surface of a centrosymmetric, collinear, compensated antiferromagnet, which hosts bulk ferroically ordered magnetic octupoles, exhibits a linear magnetoelectric effect, a net magnetization, and a net electric dipole moment. Thus, the surface satisfies all the conditions of a multiferroic, in striking contrast to the bulk, which is neither polar nor exhibits any net magnetization or linear magnetoelectric response. Of particular interest is the case of nonrelativistic -wave spin split antiferromagnets, in which the bulk magnetic octupoles and consequently the surface multiferroicity exist even without spin-orbit interaction. We illustrate our findings using first-principles calculations, taking as an example material. Our Letter underscores the bulk-boundary correspondence in these unconventional antiferromagnets.}, archive = {J_PRL}, author = {Sayantika Bhowal and Andrea Urru and Sophie F. Weber and Nicola A. Spaldin}, doi = {10.1103/PhysRevLett.134.146703}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146703}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent surface multiferroicity}, volume = {134}, year = {2025}, }
• (2025). Giant nuclear-electronic spin pumping in the heisenberg antiferromagnet RbMnF3. PRL, 134(14), 146702. (www)

  @article{ , abstract = {Collective nuclear spin excitations, called nuclear spin waves, or nuclear magnons, are enabled in strongly magnetic materials by the hyperfine coupling between the nuclear and electronic spins in an atom, and the exchange interaction between electronic spins. The investigation of nuclear spin waves garnered significant interest from theoretical and experimental researchers worldwide during the 1970s and 1980s, but gradually waned in prominence. Recently, it has been reported that the nuclear magnetic resonance in the canted antiferromagnet MnCO 3 produces spin pumping effects similar to the ones studied in ferro- and antiferromagnetic materials, bridging two quite separate worlds, the one of nuclear spin excitations and the other of spintronics. In this Letter, we report the observation of giant nuclear-electronic spin pumping effects driven by radio frequencies in the Heisenberg antiferromagnet RbMnF 3 . In this material, the small values of the electronic magnon frequencies in the vicinity of the antiferromagnetic or spin-flop transition result in an enhanced frequency pulling of the nuclear magnetic resonance frequencies that produces a strong coupling between the nuclear and electronic spin degrees of freedom. This results in nuclear-electronic spin pumping signals in the Heisenberg antiferromagnet RbMnF 3 that are almost 2 orders of magnitude larger than in MnCO 3 and remain visible at temperatures nearly 10 times higher. A theory for the nuclear-electronic spin pumping process accounts well for the experimental results.}, archive = {J_PRL}, author = {J. D. M. de Lima and D. S. Maior and E. C. Souza and D. R. Ratkovski and F. L. A. Machado and R. L. Rodríguez-Suárez and S. M. Rezende}, doi = {10.1103/PhysRevLett.134.146702}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146702}, shortjournal = {Phys. Rev. Lett.}, title = {Giant nuclear-electronic spin pumping in the heisenberg antiferromagnet RbMnF3}, volume = {134}, year = {2025}, }
• (2025). Nonlinear longitudinal and transverse magnetoresistances due to current-induced magnon creation-annihilation processes. PRL, 134(14), 146701. (www)

  @article{ , abstract = {Charge-spin conversion phenomena, such as the spin Hall effect, allow for the excitation of magnons in a magnetic layer by passing an electric current in an adjacent nonmagnetic conductor. We demonstrate that this current-induced modification of the magnon density generates an additional nonlinear longitudinal and transverse magnetoresistance for every magnetoresistance that depends on the magnetization. Using harmonic measurements, we evidence that these magnon creation-annihilation magnetoresistances dominate the second harmonic longitudinal and transverse resistance of thin Y 3 Fe 5 O 12 / Pt bilayers. Our results apply to both insulating and metallic magnetic layers, elucidating the dependence of the magnetoresistance on applied current and magnetic field for a broad variety of systems excited by spin currents.}, archive = {J_PRL}, author = {Paul Noël and Richard Schlitz and Emir Karadža and Charles-Henri Lambert and Luca Nessi and Federico Binda and Pietro Gambardella}, doi = {10.1103/PhysRevLett.134.146701}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146701}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear longitudinal and transverse magnetoresistances due to current-induced magnon creation-annihilation processes}, volume = {134}, year = {2025}, }
• (2025). Quantum geometry and bounds on dissipation in slowly driven quantum systems. PRL, 134(14), 146603. (www)

  @article{ , abstract = {We show that energy dissipation in slowly driven, Markovian quantum systems at low temperature is linked to the geometry of the driving protocol through the quantum (or Fubini-Study) metric. Utilizing these findings, we establish lower bounds on dissipation rates in two-tone protocols, such as those employed for topological frequency conversion. Notably, in appropriate limits these bounds are only determined by the topology of the protocol and an effective quality factor of the system-bath coupling. Our results bridge topological and geometric phenomena with energy dissipation in open quantum systems, and further provide design principles for optimal driving protocols.}, archive = {J_PRL}, author = {Iliya Esin and Étienne Lantagne-Hurtubise and Frederik Nathan and Gil Refael}, doi = {10.1103/PhysRevLett.134.146603}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146603}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum geometry and bounds on dissipation in slowly driven quantum systems}, volume = {134}, year = {2025}, }
• (2025). Photonic chiral state transfer near the liouvillian exceptional point. PRL, 134(14), 146602. (www)

  @article{ , abstract = {As branch-point singularities of non-Hermitian matrices, the exceptional points (EPs) exhibit unique spectral topology and criticality, with intriguing dynamic consequences in non-Hermitian settings. In quantum open systems, EPs also emerge in the Liouvillian spectrum, but their dynamic impact often pertains to the transient dynamics and is challenging to demonstrate. Here, using the flexible control afforded by single-photon interferometry, we study the chiral state transfer when the Liouvillian EP is parametrically encircled. Reconstructing the density-matrix evolution by experimentally simulating the quantum Langevin equation, we show that the chirality of the dynamics is only present within an intermediate encircling timescale and dictated by the landscape of the Liouvillian spectrum near the EP. However, the chirality disappears at long times as the system always relaxes to the steady state. We then demonstrate the power-law decay of the chirality in regard to the encircling time with a parameter-dependent exponent. Our experiment confirms the transient nature of chiral state transfer near a Liouvillian EP in quantum open systems, while our scheme paves the way for simulating general open-system dynamics using single photons.}, archive = {J_PRL}, author = {Huixia Gao and Konghao Sun and Dengke Qu and Kunkun Wang and Lei Xiao and Wei Yi and Peng Xue}, doi = {10.1103/PhysRevLett.134.146602}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146602}, shortjournal = {Phys. Rev. Lett.}, title = {Photonic chiral state transfer near the liouvillian exceptional point}, volume = {134}, year = {2025}, }
• (2025). Higher berry curvature from the wave function. i. schmidt decomposition and matrix product states. PRL, 134(14), 146601. (www)

  @article{ , abstract = {Higher Berry curvature (HBC) is the proposed generalization of Berry curvature to infinitely extended systems. Heuristically, HBC captures the flow of local Berry curvature in a system. Here, we provide a simple formula for computing the HBC for extended d = 1 systems at the level of wave functions using the Schmidt decomposition. We also find a corresponding formula for matrix product states and show that for translationally invariant matrix product states this gives rise to a quantized invariant. We demonstrate our approach with an exactly solvable model and numerical calculations for generic models using the infinite density matrix renormalization group algorithm.}, archive = {J_PRL}, author = {Ophelia Evelyn Sommer and Xueda Wen and Ashvin Vishwanath}, doi = {10.1103/PhysRevLett.134.146601}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146601}, shortjournal = {Phys. Rev. Lett.}, title = {Higher berry curvature from the wave function. i. schmidt decomposition and matrix product states}, volume = {134}, year = {2025}, }
• (2025). Finite correlation length scaling of disorder parameter at quantum criticality. PRL, 134(14), 146503. (www)

  @article{ , abstract = {The disorder parameter, defined as the expectation value of the symmetry transformation acting on a subsystem, can be used to characterize symmetric phases as an analogy to detecting spontaneous symmetry-breaking phases using local order parameters. In a dual picture, disorder parameters actually detect spontaneous symmetry breaking of higher-form symmetries. In this Letter, we show that the nonlocal disorder parameters can be conveniently and efficiently evaluated using infinite projected entangled pair states. Moreover, we propose a finite correlation length scaling theory of the disorder parameter within the quantum critical region and validate the scaling theory with variationally optimized infinite projected entangled pair states. We find from the finite correlation length scaling that the disorder parameter satisfies perimeter law at a critical point, i.e., it decays exponentially with the boundary size of the subsystem, indicating spontaneous higher-form symmetry breaking at the critical point of the dual model.}, archive = {J_PRL}, author = {Wen-Tao Xu and Rui-Zhen Huang}, doi = {10.1103/PhysRevLett.134.146503}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146503}, shortjournal = {Phys. Rev. Lett.}, title = {Finite correlation length scaling of disorder parameter at quantum criticality}, volume = {134}, year = {2025}, }
• (2025). Anomalous quantum oscillations from boson-mediated interband scattering. PRL, 134(14), 146502. (www)

  @article{ , abstract = {Quantum oscillations (QOs) in metals refer to the periodic variation of thermodynamic and transport properties as a function of inverse applied magnetic field. QO frequencies are normally associated with semiclassical trajectories of Fermi surface orbits, but recent experiments challenge the canonical description. We develop a theory of composite frequency quantum oscillations (CFQOs) in two-dimensional Fermi liquids with several Fermi surfaces and interband scattering mediated by a dynamical boson, e.g., phonons or spin fluctuations. Specifically, we show that CFQOs arise from oscillations in the fermionic self-energy with anomalous frequency splitting and distinct strongly non-Lifshitz–Kosevich temperature dependences. Our theory goes beyond the framework of semiclassical Fermi surface trajectories highlighting the role of interaction effects. We provide experimental predictions and discuss the effect of nonequilibrium boson occupation in driven systems.}, archive = {J_PRL}, author = {Léo Mangeolle and Johannes Knolle}, doi = {10.1103/PhysRevLett.134.146502}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146502}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous quantum oscillations from boson-mediated interband scattering}, volume = {134}, year = {2025}, }
• (2025). Doping dependence of 2-spinon excitations in the doped 1D cuprate Ba2CuO3+δ. PRL, 134(14), 146501. (www)

  @article{ , abstract = {Recent photoemission experiments on the quasi-one-dimensional Ba-based cuprates suggest that doped holes experience an attractive potential not captured using the simple Hubbard model. This observation has garnered significant attention due to its potential relevance to Cooper pair formation in high- T c cuprate superconductors. To scrutinize this assertion, we examined signatures of such an attractive potential in doped 1D cuprates Ba 2 CuO 3 + δ by measuring the dispersion of the 2-spinon excitations using Cu L 3 -edge resonant inelastic x-ray scattering (RIXS). Upon doping, the 2-spinon excitations appear to weaken, with a shift of the minimal position corresponding to the nesting vector of the Fermi points, q F . Notably, we find that the energy scale of the 2-spinons near the Brillouin zone boundary is substantially softened compared to that predicted by the Hubbard model in one dimension. Such a discrepancy implies missing ingredients, which lends support for the presence of an additional attractive potential between holes.}, archive = {J_PRL}, author = {Jiarui Li and Daniel Jost and Ta Tang and Ruohan Wang and Yong Zhong and Zhuoyu Chen and Mirian Garcia-Fernandez and Jonathan Pelliciari and Valentina Bisogni and Brian Moritz and Kejin Zhou and Yao Wang and Thomas P. Devereaux and Wei-Sheng Lee and Zhi-Xun Shen}, doi = {10.1103/PhysRevLett.134.146501}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146501}, shortjournal = {Phys. Rev. Lett.}, title = {Doping dependence of 2-spinon excitations in the doped 1D cuprate Ba2CuO3+δ}, volume = {134}, year = {2025}, }
• (2025). Light-field dressing of transient photoexcited states above the fermi energy. PRL, 134(14), 146401. (www)

  @article{ , abstract = {Time-periodic light field provides an emerging pathway for dynamically engineering quantum materials by forming hybrid states between photons and Bloch electrons. So far, experimental progress on light-field dressed states has been mainly focused on the occupied states; however, it is unclear if the transient photoexcited states above the Fermi energy E F can also be dressed, leaving the dynamical interplay between photoexcitation and light-field dressing elusive. Here, we provide direct experimental evidence for light-field dressing of the transient photoexcited surface states above E F , which exhibits distinct dynamics with a delay response as compared to light-field dressed states below E F . Our work reveals the dual roles of the pump pulse in both photoexcitation and light-field dressing, providing a more comprehensive picture with new insights on the light-induced manipulation of transient electronic states.}, archive = {J_PRL}, author = {Fei Wang and Wanying Chen and Changhua Bao and Tianyun Lin and Haoyuan Zhong and Hongyun Zhang and Shuyun Zhou}, doi = {10.1103/PhysRevLett.134.146401}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146401}, shortjournal = {Phys. Rev. Lett.}, title = {Light-field dressing of transient photoexcited states above the fermi energy}, volume = {134}, year = {2025}, }
• (2025). Ultrahigh thermal conductance across superlubric interfaces in twisted graphite. PRL, 134(14), 146302. (www)

  @article{ , abstract = {Interlayer rotation in van der Waals (vdW) materials offers a unique degree of freedom for manipulating lattice dynamics and leads to an exotic state with vanishing friction called structural superlubricity. Extensive theoretical calculations have also predicted the potential of twisted vdW materials for controlling heat flow in advanced electronics. However, precise experimental measurements have proven extremely challenging with only a handful of efforts to date reporting inconsistent results. Here, we have managed to achieve simultaneous mechanical characterizations and thermal measurements of the intrinsic twisted interfaces in microfabricated graphite mesas. Remarkably, the conductance of superlubric interfaces reaches about which surpasses the measured values for artificially stacked vdW structures by nearly an order of magnitude. Nonetheless, we successfully resolved over 30-fold variation of thermal conductance as the buried interfaces were rotated to a locked state. Further, atomic simulations revealed the predominant role of the transverse acoustic phonons. Together, our findings highlight a general physical picture that directly correlates interfacial thermal transport with sliding resistance, and lay the foundation for twist-enabled thermal management which are particularly beneficial to twistronics and slidetronics.}, archive = {J_PRL}, author = {Fuwei Yang and Wenjiang Zhou and Zhibin Zhang and Xuanyu Huang and Jingwen Zhang and Nianjie Liang and Wujuan Yan and Yuxi Wang and Mingchao Ding and Quanlin Guo and Yu Han and Te-Huan Liu and Kaihui Liu and Quanshui Zheng and Bai Song}, doi = {10.1103/PhysRevLett.134.146302}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146302}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrahigh thermal conductance across superlubric interfaces in twisted graphite}, volume = {134}, year = {2025}, }
• (2025). Energy transport in superionic crystals. PRL, 134(14), 146301. (www)

  @article{ , abstract = {In this Letter, we propose a rigorous concept based on the Onsager reciprocal theorem to describe the thermal transport behaviors in superionic crystals. Our results show that thermal energy in superionic crystals can be transferred through the conduction of atomic vibrations, the enthalpy diffusion caused by ions’ diffusion and the thermodiffusion coupling. The thermal conductivity resulting from the heat conduction pathway decreases with temperature as scatterings among vibrations and between vibrations and ions become stronger. However, the thermal conductivity due to enthalpy diffusion increases with temperature, which is because ions diffuse farther at high temperatures. The thermal conductivity owing to the thermodiffusion coupling is negligible since the chemical potential gradient under steady state is small. The apparent thermal conductivity of superionic crystals is therefore determined by the competition between these two thermal pathways, and can exhibit a diverse behavior of negative, weak, and positive temperature dependence as observed in experiments. This Letter unveils the thermal transport mechanisms in superionic crystals, which explains the long-standing and confusing thermal conductivity temperature dependence of superionic crystals.}, archive = {J_PRL}, author = {Wenxiang Liu and Yanguang Zhou}, doi = {10.1103/PhysRevLett.134.146301}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146301}, shortjournal = {Phys. Rev. Lett.}, title = {Energy transport in superionic crystals}, volume = {134}, year = {2025}, }
• (2025). Control of andreev reflection via a single-molecule orbital. PRL, 134(14), 146201. (www)

  @article{ , abstract = {Charge transport across a single-molecule junction fabricated from a normal-metal tip, a phthalocyanine, and a conventional superconductor in a scanning tunneling microscope is explored as a function of the gradually closed vacuum gap. The phthalocyanine (2H-Pc) molecule and its pyrrolic-hydrogen-abstracted derivative (Pc) exhibit vastly different behavior. Andreev reflection across the 2H-Pc contact exhibits a temporary enhancement that diminishes again with increasing conductance. In contrast, the single-Pc junction lacks Andreev reflection in the same conductance range. Spectroscopies and supporting nonequilibrium Green’s function calculations highlight the importance of a molecular orbital close to the Fermi energy for Andreev reflection.}, archive = {J_PRL}, author = {Lorenz Meyer and Jose L. Lado and Nicolas Néel and Jörg Kröger}, doi = {10.1103/PhysRevLett.134.146201}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146201}, shortjournal = {Phys. Rev. Lett.}, title = {Control of andreev reflection via a single-molecule orbital}, volume = {134}, year = {2025}, }
• (2025). Imaging the progression of radiolytic damage in molecular crystals with scanning nanobeam electron diffraction. PRL, 134(14), 146101. (www)

  @article{ , abstract = {Almost every electron microscopy experiment is fundamentally limited by radiation damage. Nevertheless, little is known about the onset and progression of radiolysis in beam-sensitive materials. Here we apply ambient-temperature scanning nanobeam electron diffraction to record simultaneous dual-space movies of organic and organometallic nanocrystals at sequential stages of beam-induced radiolytic decay. We show that the underlying mosaic of coherently diffracting domains undergoes internal rearrangement as a function of accumulating electron fluence, causing the intensities of some associated Bragg reflections to fade nonmonotonically. Furthermore, we demonstrate that repeated irradiation at a single probe position leads to the isotropic propagation of delocalized radiolytic damage well beyond the direct footprint of the incident beam. We refer to these expanding tides of amorphization as “impact craters.”}, archive = {J_PRL}, author = {Ambarneil Saha and Matthew Mecklenburg and Alexander J. Pattison and Aaron S. Brewster and Jose A. Rodriguez and Peter Ercius}, doi = {10.1103/PhysRevLett.134.146101}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146101}, shortjournal = {Phys. Rev. Lett.}, title = {Imaging the progression of radiolytic damage in molecular crystals with scanning nanobeam electron diffraction}, volume = {134}, year = {2025}, }
• (2025). Adatom engineering magnetic order in superconductors: Applications to altermagnetic superconductivity. PRL, 134(14), 146001. (www)

  @article{ , abstract = {We study theoretically how superlattices based on adatoms on surfaces of unconventional superconductors can be used to engineer novel pairing states that break time-reversal symmetry and exhibit nontrivial magnetic point symmetries. We illustrate this using a square-lattice Hubbard model with d -wave superconductivity and a subleading s -wave state as an example. An adatom superlattice with square-lattice symmetries is shown to stabilize an “orbital altermagnetic superconductor,” a state that exhibits loop current patterns and associated orbital magnetic moments, which preserve superlattice translations but are odd under fourfold rotations. This state is further characterized by a nonzero Berry curvature quadrupole moment and, upon including spin-orbit coupling, by an altermagnetic spin splitting of the bands and nontrivial spin textures in the superlattice unit cell, with zero net spin moment.}, archive = {J_PRL}, author = {Lucas V. Pupim and Mathias S. Scheurer}, doi = {10.1103/PhysRevLett.134.146001}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {146001}, shortjournal = {Phys. Rev. Lett.}, title = {Adatom engineering magnetic order in superconductors: Applications to altermagnetic superconductivity}, volume = {134}, year = {2025}, }
• (2025). Two mechanisms limiting the emitted electron current from a cathode to an anode. PRL, 134(14), 145301. (www)

  @article{ , abstract = {It is known that the current of emitted electrons flowing through a plasma can saturate upon formation of a potential well adjacent to the cathode (the “space charge effect”). Here, we demonstrate another saturation mechanism that will often set a more restrictive limit on the global current. When “backflow saturation” occurs, the cathode sheath weakens to allow emitted electrons that already entered the plasma to backflow to the cathode. This effect could not be captured by studies modelling the cathode sheath by itself because its origin is coupled to processes in the interior plasma and anode sheath. By modeling a full plasma diode, we show that depending on conditions the global current can be limited in four ways; by backflow alone, by space charge alone, by both mechanisms in a stable cooperative form, or by both in a competing oscillatory form.}, archive = {J_PRL}, author = {M. D. Campanell and C. Y. Wang and K. L. Nguyen}, doi = {10.1103/PhysRevLett.134.145301}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {145301}, shortjournal = {Phys. Rev. Lett.}, title = {Two mechanisms limiting the emitted electron current from a cathode to an anode}, volume = {134}, year = {2025}, }
• (2025). Characteristic E-region plasma signature of magnetospheric wave-particle interactions. PRL, 134(14), 145201. (www)

  @article{ , abstract = {Plasma waves in the magnetosphere scatter electrons, causing them to precipitate into Earth’s atmosphere, imparting their temporal characteristics to diffuse auroras. In a case study of conjugate radar and satellite observations, we demonstrate a close and unprecedented association between enhanced electrostatic cyclotron harmonic wave activity in the magnetosphere and the appearance of meter-scale plasma turbulence a few seconds later in the lower ionosphere on nearby magnetic field lines. Such direct structuring of the ionosphere carries implications for our understanding of space weather.}, archive = {J_PRL}, author = {Magnus F. Ivarsen and Yukinaga Miyashita and Jean-Pierre St-Maurice and Glenn C. Hussey and Brian Pitzel and Draven Galeschuk and Saif Marei and Richard B. Horne and Yoshiya Kasahara and Shoya Matsuda and Satoshi Kasahara and Kunihiro Keika and Yoshizumi Miyoshi and Kazuhiro Yamamoto and Atsuki Shinbori and Devin R. Huyghebaert and Ayako Matsuoka and Shoichiro Yokota and Fuminori Tsuchiya}, doi = {10.1103/PhysRevLett.134.145201}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {145201}, shortjournal = {Phys. Rev. Lett.}, title = {Characteristic E-region plasma signature of magnetospheric wave-particle interactions}, volume = {134}, year = {2025}, }
• (2025). Reconfigurable chiral edge states in synthetic dimensions on an integrated photonic chip. PRL, 134(14), 143801. (www)

  @article{ , abstract = {Chiral edge states are a hallmark of topological physics, and the emergence of synthetic dimensions has provided ideal platforms for investigating chiral topology while overcoming the limitations of real space. Conventional studies have primarily concentrated on symmetric chiral behaviors, limited by complex and inflexible systems. Here, we demonstrate a programmable integrated photonic platform to generate and manipulate reconfigurable chiral edge states in synthetic dimensions within a single lithium niobate microring resonator. Our system is realized by integrating independent frequency and pseudospin degrees of freedom in the dynamically modulated resonator, which features tunable artificial gauge potentials and long-range couplings. We demonstrate a variety of reconfigurable chiral behaviors in synthetic dimensions, including the realization and frustration of chiral edge states in a synthetic Hall ladder, the generation of imbalanced chiral edge currents, and the regulation of chiral behaviors among chirality, single-pseudospin enhancement, and complete suppression. This work paves the way for exploring chiral edge states in high-dimensional synthetic space on a programmable photonic chip, showing promising potential for applications in optical communications, quantum simulations, signal processing, and photonic neuromorphic computing.}, archive = {J_PRL}, author = {Weiwei Liu and Xiaolong Su and Chijun Li and Cheng Zeng and Bing Wang and Yongjie Wang and Yufan Ding and Chengzhi Qin and Jinsong Xia and Peixiang Lu}, doi = {10.1103/PhysRevLett.134.143801}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {143801}, shortjournal = {Phys. Rev. Lett.}, title = {Reconfigurable chiral edge states in synthetic dimensions on an integrated photonic chip}, volume = {134}, year = {2025}, }
• (2025). Multi-axis inertial sensing with 2D matter-wave arrays. PRL, 134(14), 143601. (www)

  @article{ , abstract = {Atom interferometery is an exquisite measurement technique sensitive to inertial forces. However, it is commonly limited to a single sensitive axis, allowing high-precision multidimensional sensing only through subsequent or postcorrected measurements. We report on a novel method for multi-axis inertial sensing based on the correlation of simultaneous light-pulse atom interferometers in 2D array arrangements of Bose-Einstein condensates (BEC). Deploying a scalable 3 × 3 BEC array spanning 1.6 m m 2 created using time-averaged optical potentials, we perform measurements of linear acceleration induced by gravity and simultaneously demonstrate sensitivity to angular velocity and acceleration of a rotating reference mirror, as well as gravity gradients and higher-order derivatives. Our Letter enables simple, high-precision multi-axis inertial sensing compatible with high rotation rates, e.g., for inertial navigation in dynamic environments. We finally envision further applications of our method, e.g., 3D in situ measurements and reconstruction of laser beam intensities and wave fronts.}, archive = {J_PRL}, author = {K. Stolzenberg and C. Struckmann and S. Bode and R. Li and A. Herbst and V. Vollenkemper and D. Thomas and A. Rajagopalan and E. M. Rasel and N. Gaaloul and D. Schlippert}, doi = {10.1103/PhysRevLett.134.143601}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {143601}, shortjournal = {Phys. Rev. Lett.}, title = {Multi-axis inertial sensing with 2D matter-wave arrays}, volume = {134}, year = {2025}, }
• (2025). Suppressing the decoherence of alkali-metal spins at low magnetic fields. PRL, 134(14), 143201. (www)

  @article{ , abstract = {Interactions of electron spins with rotational degrees of freedom during collisions or with external fields are fundamental processes that limit the coherence time of spin gases. We experimentally study the decoherence of hot cesium spins dominated by spin rotation interaction during binary collisions with N 2 molecules or by absorption of near-resonant light. We report an order of magnitude suppression of the spin decoherence rate by either of those processes at low magnetic fields. This work extends the use of magnetic fields as a control knob, not only to suppress decoherence from random spin-conserving processes in the spin-exchange relaxation free (SERF) regime but also to suppress processes that relax electron spins rather than conserve them.}, archive = {J_PRL}, author = {Mark Dikopoltsev and Avraham Berrebi and Uriel Levy and Or Katz}, doi = {10.1103/PhysRevLett.134.143201}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {143201}, shortjournal = {Phys. Rev. Lett.}, title = {Suppressing the decoherence of alkali-metal spins at low magnetic fields}, volume = {134}, year = {2025}, }
• (2025). First proton-induced cross sections on a stored rare ion beam: Measurement of te118(p,γ) for explosive nucleosynthesis. PRL, 134(14), 142701. (www)

  @article{ , abstract = {We present the first nuclear cross-section measurements of and (p,n) reactions on at energies relevant for the -process nucleosynthesis. Absolute cross-section values for center-of-mass energies of 6, 7 and 10 MeV are provided, together with a theoretical extrapolation to the Gamow window. This experiment marks the first time that direct proton-induced reactions have been measured on a radioactive ion beam at the Experimental Storage Ring (ESR) at GSI, Darmstadt. This paves the way for a large variety of measurements, delivering new constraints for explosive nucleosynthesis and for physics beyond nuclear stability.}, archive = {J_PRL}, author = {S. F. Dellmann and J. Glorius and Yu. A. Litvinov and R. Reifarth and L. Varga and M. Aliotta and F. Amjad and K. Blaum and L. Bott and C. Brandau and B. Brückner and C. G. Bruno and R.-J. Chen and T. Davinson and T. Dickel and I. Dillmann and D. Dmytriev and P. Erbacher and O. Forstner and D. Freire-Fernández and H. Geissel and K. Göbel and C. J. Griffin and R. E. Grisenti and A. Gumberidze and E. Haettner and S. Hagmann and T. Heftrich and M. Heil and R. Heß and P.-M. Hillenbrand and C. Hornung and R. Joseph and B. Jurado and E. Kazanseva and K. Khasawneh and R. Knöbel and D. Kostyleva and C. Kozhuharov and I. Kulikov and N. Kuzminchuk and D. Kurtulgil and C. Langer and G. Leckenby and C. Lederer-Woods and M. Lestinsky and S. Litvinov and B. Löher and B. Lorentz and E. Lorenz and J. Marsh and E. Menz and T. Morgenroth and I. Mukha and N. Petridis and U. Popp and A. Psaltis and S. Purushothaman and E. Rocco and P. Roy and M. S. Sanjari and C. Scheidenberger and M. Sguazzin and R. S. Sidhu and U. Spillmann and M. Steck and T. Stöhlker and A. Surzhykov and J. A. Swartz and Y. Tanaka and H. Törnqvist and D. Vescovi and M. Volknandt and H. Weick and M. Weigand and P. J. Woods and T. Yamaguchi and J. Zhao}, doi = {10.1103/PhysRevLett.134.142701}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {142701}, shortjournal = {Phys. Rev. Lett.}, title = {First proton-induced cross sections on a stored rare ion beam: Measurement of te118(p,γ) for explosive nucleosynthesis}, volume = {134}, year = {2025}, }
• (2025). Observation of tt¯ production in Pb+Pb collisions at sNN=5.02 TeV with the ATLAS detector. PRL, 134(14), 142301. (www)

  @article{ , abstract = {Top-quark pair production is observed in lead–lead ( Pb + Pb ) collisions at s NN = 5.02 TeV at the Large Hadron Collider with the ATLAS detector. The data sample was recorded in 2015 and 2018, amounting to an integrated luminosity of 1.9 nb − 1 . Events with exactly one electron and one muon and at least two jets are selected. Top-quark pair production is measured with an observed (expected) significance of 5.0 (4.1) standard deviations. The measured top-quark pair production cross section is σ t t ¯ = 3.6 − 0.9 + 1.0 ( stat ) − 0.5 + 0.8 ( syst ) μ b , with a total relative uncertainty of 31%, and is consistent with theoretical predictions using a range of different nuclear parton distribution functions. The observation of this process consolidates the evidence of the existence of all quark flavors in the preequilibrium stage of the quark-gluon plasma at very high energy densities, similar to the conditions present in the early Universe.}, archive = {J_PRL}, author = {ATLAS Collaboration and G. Aad and E. Aakvaag and B. Abbott and S. Abdelhameed and K. Abeling and N. J. Abicht and S. H. Abidi and M. Aboelela and A. Aboulhorma and H. Abramowicz and Y. Abulaiti and B. S. Acharya and A. Ackermann and C. Adam Bourdarios and L. Adamczyk and S. V. Addepalli and M. J. Addison and J. Adelman and A. Adiguzel and T. Adye and A. A. Affolder and Y. Afik and M. N. Agaras and A. Aggarwal and C. Agheorghiesei and F. Ahmadov and S. Ahuja and X. Ai and G. Aielli and A. Aikot and M. Ait Tamlihat and B. Aitbenchikh and M. Akbiyik and T. P. A. Åkesson and A. V. Akimov and D. Akiyama and N. N. Akolkar and S. Aktas and K. Al Khoury and G. L. Alberghi and J. Albert and P. Albicocco and G. L. Albouy and S. Alderweireldt and Z. L. Alegria and M. Aleksa and I. N. Aleksandrov and C. Alexa and T. Alexopoulos and F. Alfonsi and M. Algren and M. Alhroob and B. Ali and H. M. J. Ali and S. Ali and S. W. Alibocus and M. Aliev and G. Alimonti and W. Alkakhi and C. Allaire and B. M. M. Allbrooke and J. S. Allen and J. F. Allen and C. A. Allendes Flores and P. P. Allport and A. Aloisio and F. Alonso and C. Alpigiani and Z. M. K. Alsolami and A. Alvarez Fernandez and M. Alves Cardoso and M. G. Alviggi and M. Aly and Y. Amaral Coutinho and A. Ambler and C. Amelung and M. Amerl and C. G. Ames and D. Amidei and B. Amini and K. Amirie and S. P. Amor Dos Santos and K. R. Amos and D. Amperiadou and S. An and V. Ananiev and C. Anastopoulos and T. Andeen and J. K. Anders and A. C. Anderson and A. Andreazza and S. Angelidakis and A. Angerami and A. V. Anisenkov and A. Annovi and C. Antel and E. Antipov and M. Antonelli and F. Anulli and M. Aoki and T. Aoki and M. A. Aparo and L. Aperio Bella and C. Appelt and A. Apyan and S. J. Arbiol Val and C. Arcangeletti and A. T. H. Arce and J-F. Arguin and S. Argyropoulos and J.-H. Arling and O. Arnaez and H. Arnold and G. Artoni and H. Asada and K. Asai and S. Asai and N. A. Asbah and R. A. Ashby Pickering and K. Assamagan and R. Astalos and K. S. V. Astrand and S. Atashi and R. J. Atkin and H. Atmani and P. A. Atmasiddha and K. Augsten and A. D. Auriol and V. A. Austrup and G. Avolio and K. Axiotis and G. Azuelos and D. Babal and H. Bachacou and K. Bachas and A. Bachiu and E. Bachmann and A. Badea and T. M. Baer and P. Bagnaia and M. Bahmani and D. Bahner and K. Bai and J. T. Baines and L. Baines and O. K. Baker and E. Bakos and D. Bakshi Gupta and L. E. Balabram Filho and V. Balakrishnan and R. Balasubramanian and E. M. Baldin and P. Balek and E. Ballabene and F. Balli and L. M. Baltes and W. K. Balunas and J. Balz and I. Bamwidhi and E. Banas and M. Bandieramonte and A. Bandyopadhyay and S. Bansal and L. Barak and M. Barakat and E. L. Barberio and D. Barberis and M. Barbero and M. Z. Barel and T. Barillari and M-S. Barisits and T. Barklow and P. Baron and D. A. Baron Moreno and A. Baroncelli and A. J. Barr and J. D. Barr and F. Barreiro and J. Barreiro Guimarães da Costa and M. G. Barros Teixeira and S. Barsov and F. Bartels and R. Bartoldus and A. E. Barton and P. Bartos and A. Basan and M. Baselga and S. Bashiri and A. Bassalat and M. J. Basso and S. Bataju and R. Bate and R. L. Bates and S. Batlamous and B. Batool and M. Battaglia and D. Battulga and M. Bauce and M. Bauer and P. Bauer and L. T. Bazzano Hurrell and J. B. Beacham and T. Beau and J. Y. Beaucamp and P. H. Beauchemin and P. Bechtle and H. P. Beck and K. Becker and A. J. Beddall and V. A. Bednyakov and C. P. Bee and L. J. Beemster and M. Begalli and M. Begel and J. K. Behr and J. F. Beirer and F. Beisiegel and M. Belfkir and G. Bella and L. Bellagamba and A. Bellerive and P. Bellos and K. Beloborodov and D. Benchekroun and F. Bendebba and Y. Benhammou and K. C. Benkendorfer and L. Beresford and M. Beretta and E. Bergeaas Kuutmann and N. Berger and B. Bergmann and J. Beringer and G. Bernardi and C. Bernius and F. U. Bernlochner and F. Bernon and A. Berrocal Guardia and T. Berry and P. Berta and A. Berthold and S. Bethke and A. Betti and A. J. Bevan and N. K. Bhalla and S. Bharthuar and S. Bhatta and D. S. Bhattacharya and P. Bhattarai and Z. M. Bhatti and K. D. Bhide and V. S. Bhopatkar and R. M. Bianchi and G. Bianco and O. Biebel and M. Biglietti and C. S. Billingsley and Y. Bimgdi and M. Bindi and A. Bingham and A. Bingul and C. Bini and G. A. Bird and M. Birman and M. Biros and S. Biryukov and T. Bisanz and E. Bisceglie and J. P. Biswal and D. Biswas and I. Bloch and A. Blue and U. Blumenschein and J. Blumenthal and V. S. Bobrovnikov and M. Boehler and B. Boehm and D. Bogavac and A. G. Bogdanchikov and L. S. Boggia and C. Bohm and V. Boisvert and P. Bokan and T. Bold and M. Bomben and M. Bona and M. Boonekamp and A. G. Borbély and I. S. Bordulev and G. Borissov and D. Bortoletto and D. Boscherini and M. Bosman and K. Bouaouda and N. Bouchhar and L. Boudet and J. Boudreau and E. V. Bouhova-Thacker and D. Boumediene and R. Bouquet and A. Boveia and J. Boyd and D. Boye and I. R. Boyko and L. Bozianu and J. Bracinik and N. Brahimi and G. Brandt and O. Brandt and B. Brau and J. E. Brau and R. Brener and L. Brenner and R. Brenner and S. Bressler and G. Brianti and D. Britton and D. Britzger and I. Brock and R. Brock and G. Brooijmans and A. J. Brooks and E. M. Brooks and E. Brost and L. M. Brown and L. E. Bruce and T. L. Bruckler and P. A. Bruckman de Renstrom and B. Brüers and A. Bruni and G. Bruni and D. Brunner and M. Bruschi and N. Bruscino and T. Buanes and Q. Buat and D. Buchin and A. G. Buckley and W. E. Bulanowska and O. Bulekov and B. A. Bullard and S. Burdin and C. D. Burgard and A. M. Burger and B. Burghgrave and O. Burlayenko and J. Burleson and J. T. P. Burr and J. C. Burzynski and E. L. Busch and V. Büscher and P. J. Bussey and J. M. Butler and C. M. Buttar and J. M. Butterworth and W. Buttinger and C. J. Buxo Vazquez and A. R. Buzykaev and S. Cabrera Urbán and L. Cadamuro and D. Caforio and H. Cai and Y. Cai and V. M. M. Cairo and O. Cakir and N. Calace and P. Calafiura and G. Calderini and P. Calfayan and G. Callea and L. P. Caloba and D. Calvet and S. Calvet and R. Camacho Toro and S. Camarda and D. Camarero Munoz and P. Camarri and M. T. Camerlingo and D. Cameron and C. Camincher and M. Campanelli and A. Camplani and V. Canale and A. C. Canbay and E. Canonero and J. Cantero and Y. Cao and F. Capocasa and M. Capua and A. Carbone and R. Cardarelli and J. C. J. Cardenas and M. P. Cardiff and G. Carducci and T. Carli and G. Carlino and J. I. Carlotto and B. T. Carlson and E. M. Carlson and J. Carmignani and L. Carminati and A. Carnelli and M. Carnesale and S. Caron and E. Carquin and I. B. Carr and S. Carrá and G. Carratta and A. M. Carroll and M. P. Casado and M. Caspar and F. L. Castillo and L. Castillo Garcia and V. Castillo Gimenez and N. F. Castro and A. Catinaccio and J. R. Catmore and T. Cavaliere and V. Cavaliere and L. J. Caviedes Betancourt and Y. C. Cekmecelioglu and E. Celebi and S. Cella and V. Cepaitis and K. Cerny and A. S. Cerqueira and A. Cerri and L. Cerrito and F. Cerutti and B. Cervato and A. Cervelli and G. Cesarini and S. A. Cetin and P. M. Chabrillat and D. Chakraborty and J. Chan and W. Y. Chan and J. D. Chapman and E. Chapon and B. Chargeishvili and D. G. Charlton and C. Chauhan and Y. Che and S. Chekanov and S. V. Chekulaev and G. A. Chelkov and B. Chen and H. Chen and J. Chen and M. Chen and S. Chen and S. J. Chen and X. Chen and Y. Chen and C. L. Cheng and H. C. Cheng and S. Cheong and A. Cheplakov and E. Cheremushkina and E. Cherepanova and R. Cherkaoui El Moursli and E. Cheu and K. Cheung and L. Chevalier and V. Chiarella and G. Chiarelli and N. Chiedde and G. Chiodini and A. S. Chisholm and A. Chitan and M. Chitishvili and M. V. Chizhov and K. Choi and Y. Chou and E. Y. S. Chow and K. L. Chu and M. C. Chu and X. Chu and Z. Chubinidze and J. Chudoba and J. J. Chwastowski and D. Cieri and K. M. Ciesla and V. Cindro and A. Ciocio and F. Cirotto and Z. H. Citron and M. Citterio and D. A. Ciubotaru and A. Clark and P. J. Clark and N. Clarke Hall and C. Clarry and S. E. Clawson and C. Clement and Y. Coadou and M. Cobal and A. Coccaro and R. F. Coelho Barrue and R. Coelho Lopes De Sa and S. Coelli and L. S. Colangeli and B. Cole and J. Collot and P. Conde Muiño and M. P. Connell and S. H. Connell and E. I. Conroy and F. Conventi and H. G. Cooke and A. M. Cooper-Sarkar and F. A. Corchia and A. Cordeiro Oudot Choi and L. D. Corpe and M. Corradi and F. Corriveau and A. Cortes-Gonzalez and M. J. Costa and F. Costanza and D. Costanzo and B. M. Cote and J. Couthures and G. Cowan and K. Cranmer and L. Cremer and D. Cremonini and S. Crépé-Renaudin and F. Crescioli and M. Cristinziani and M. Cristoforetti and V. Croft and J. E. Crosby and G. Crosetti and A. Cueto and H. Cui and Z. Cui and W. R. Cunningham and F. Curcio and J. R. Curran and P. Czodrowski and M. J. Da Cunha Sargedas De Sousa and J. V. Da Fonseca Pinto and C. Da Via and W. Dabrowski and T. Dado and S. Dahbi and T. Dai and D. Dal Santo and C. Dallapiccola and M. Dam and G. D’amen and V. D’Amico and J. Damp and J. R. Dandoy and D. Dannheim and M. Danninger and V. Dao and G. Darbo and S. J. Das and F. Dattola and S. D’Auria and A. D’Avanzo and T. Davidek and I. Dawson and H. A. Day-hall and K. De and C. De Almeida Rossi and R. De Asmundis and N. De Biase and S. De Castro and N. De Groot and P. de Jong and H. De la Torre and A. De Maria and A. De Salvo and U. De Sanctis and F. De Santis and A. De Santo and J. B. De Vivie De Regie and J. Debevc and D. V. Dedovich and J. Degens and A. M. Deiana and F. Del Corso and J. Del Peso and L. Delagrange and F. Deliot and C. M. Delitzsch and M. Della Pietra and D. Della Volpe and A. Dell’Acqua and L. Dell’Asta and M. Delmastro and C. C. Delogu and P. A. Delsart and S. Demers and M. Demichev and S. P. Denisov and H. Denizli and L. D’Eramo and D. Derendarz and F. Derue and P. Dervan and K. Desch and C. Deutsch and F. A. Di Bello and A. Di Ciaccio and L. Di Ciaccio and A. Di Domenico and C. Di Donato and A. Di Girolamo and G. Di Gregorio and A. Di Luca and B. Di Micco and R. Di Nardo and K. F. Di Petrillo and M. Diamantopoulou and F. A. Dias and T. Dias Do Vale and M. A. Diaz and A. R. Didenko and M. Didenko and E. B. Diehl and S. Díez Cornell and C. Diez Pardos and C. Dimitriadi and A. Dimitrievska and J. Dingfelder and T. Dingley and I-M. Dinu and S. J. Dittmeier and F. Dittus and M. Divisek and B. Dixit and F. Djama and T. Djobava and C. Doglioni and A. Dohnalova and Z. Dolezal and K. Domijan and K. M. Dona and M. Donadelli and B. Dong and J. Donini and A. D’Onofrio and M. D’Onofrio and J. Dopke and A. Doria and N. Dos Santos Fernandes and P. Dougan and M. T. Dova and A. T. Doyle and M. A. Draguet and M. P. Drescher and E. Dreyer and I. Drivas-koulouris and M. Drnevich and M. Drozdova and D. Du and T. A. du Pree and F. Dubinin and M. Dubovsky and E. Duchovni and G. Duckeck and O. A. Ducu and D. Duda and A. Dudarev and E. R. Duden and M. D’uffizi and L. Duflot and M. Dührssen and I. Duminica and A. E. Dumitriu and M. Dunford and S. Dungs and K. Dunne and A. Duperrin and H. Duran Yildiz and M. Düren and A. Durglishvili and D. Duvnjak and B. L. Dwyer and G. I. Dyckes and M. Dyndal and B. S. Dziedzic and Z. O. Earnshaw and G. H. Eberwein and B. Eckerova and S. Eggebrecht and E. Egidio Purcino De Souza and L. F. Ehrke and G. Eigen and K. Einsweiler and T. Ekelof and P. A. Ekman and S. El Farkh and Y. El Ghazali and H. El Jarrari and A. El Moussaouy and V. Ellajosyula and M. Ellert and F. Ellinghaus and N. Ellis and J. Elmsheuser and M. Elsawy and M. Elsing and D. Emeliyanov and Y. Enari and I. Ene and S. Epari and P. A. Erland and D. Ernani Martins Neto and M. Errenst and M. Escalier and C. Escobar and E. Etzion and G. Evans and H. Evans and L. S. Evans and A. Ezhilov and S. Ezzarqtouni and F. Fabbri and L. Fabbri and G. Facini and V. Fadeyev and R. M. Fakhrutdinov and D. Fakoudis and S. Falciano and L. F. Falda Ulhoa Coelho and F. Fallavollita and G. Falsetti and J. Faltova and C. Fan and K. Y. Fan and Y. Fan and Y. Fang and M. Fanti and M. Faraj and Z. Farazpay and A. Farbin and A. Farilla and T. Farooque and J. N. Farr and S. M. Farrington and F. Fassi and D. Fassouliotis and M. Faucci Giannelli and W. J. Fawcett and L. Fayard and P. Federic and P. Federicova and O. L. Fedin and M. Feickert and L. Feligioni and D. E. Fellers and C. Feng and Z. Feng and M. J. Fenton and L. Ferencz and R. A. M. Ferguson and P. Fernandez Martinez and M. J. V. Fernoux and J. Ferrando and A. Ferrari and P. Ferrari and R. Ferrari and D. Ferrere and C. Ferretti and M. P. Fewell and D. Fiacco and F. Fiedler and P. Fiedler and S. Filimonov and A. Filipčič and E. K. Filmer and F. Filthaut and M. C. N. Fiolhais and L. Fiorini and W. C. Fisher and T. Fitschen and P. M. Fitzhugh and I. Fleck and P. Fleischmann and T. Flick and M. Flores and L. R. Flores Castillo and L. Flores Sanz De Acedo and F. M. Follega and N. Fomin and J. H. Foo and A. Formica and A. C. Forti and E. Fortin and A. W. Fortman and M. G. Foti and L. Fountas and D. Fournier and H. Fox and P. Francavilla and S. Francescato and S. Franchellucci and M. Franchini and S. Franchino and D. Francis and L. Franco and V. Franco Lima and L. Franconi and M. Franklin and G. Frattari and Y. Y. Frid and J. Friend and N. Fritzsche and A. Froch and D. Froidevaux and J. A. Frost and Y. Fu and S. Fuenzalida Garrido and M. Fujimoto and K. Y. Fung and E. Furtado De Simas Filho and M. Furukawa and J. Fuster and A. Gaa and A. Gabrielli and P. Gadow and G. Gagliardi and L. G. Gagnon and S. Gaid and S. Galantzan and J. Gallagher and E. J. Gallas and A. L. Gallen and B. J. Gallop and K. K. Gan and S. Ganguly and Y. Gao and F. M. Garay Walls and B. Garcia and C. García and A. Garcia Alonso and A. G. Garcia Caffaro and J. E. García Navarro and M. Garcia-Sciveres and G. L. Gardner and R. W. Gardner and N. Garelli and R. B. Garg and J. M. Gargan and C. A. Garner and C. M. Garvey and V. K. Gassmann and G. Gaudio and V. Gautam and P. Gauzzi and J. Gavranovic and I. L. Gavrilenko and A. Gavrilyuk and C. Gay and G. Gaycken and E. N. Gazis and A. A. Geanta and A. Gekow and C. Gemme and M. H. Genest and A. D. Gentry and S. George and W. F. George and T. Geralis and A. A. Gerwin and P. Gessinger-Befurt and M. E. Geyik and M. Ghani and K. Ghorbanian and A. Ghosal and A. Ghosh and B. Giacobbe and S. Giagu and T. Giani and A. Giannini and S. M. Gibson and M. Gignac and D. T. Gil and A. K. Gilbert and B. J. Gilbert and D. Gillberg and G. Gilles and L. Ginabat and D. M. Gingrich and M. P. Giordani and P. F. Giraud and G. Giugliarelli and D. Giugni and F. Giuli and I. Gkialas and L. K. Gladilin and C. Glasman and G. Glemža and M. Glisic and I. Gnesi and Y. Go and M. Goblirsch-Kolb and B. Gocke and D. Godin and B. Gokturk and S. Goldfarb and T. Golling and M. G. D. Gololo and D. Golubkov and J. P. Gombas and A. Gomes and G. Gomes Da Silva and A. J. Gomez Delegido and R. Gonçalo and L. Gonella and A. Gongadze and F. Gonnella and J. L. Gonski and R. Y. González Andana and S. González de la Hoz and R. Gonzalez Lopez and C. Gonzalez Renteria and M. V. Gonzalez Rodrigues and R. Gonzalez Suarez and S. Gonzalez-Sevilla and L. Goossens and B. Gorini and E. Gorini and A. Gorišek and T. C. Gosart and A. T. Goshaw and M. I. Gostkin and S. Goswami and C. A. Gottardo and S. A. Gotz and M. Gouighri and A. G. Goussiou and N. Govender and R. P. Grabarczyk and I. Grabowska-Bold and K. Graham and E. Gramstad and S. Grancagnolo and C. M. Grant and P. M. Gravila and F. G. Gravili and H. M. Gray and M. Greco and M. J. Green and C. Grefe and A. S. Grefsrud and I. M. Gregor and K. T. Greif and P. Grenier and S. G. Grewe and A. A. Grillo and K. Grimm and S. Grinstein and J.-F. Grivaz and E. Gross and J. Grosse-Knetter and L. Guan and J. G. R. Guerrero Rojas and G. Guerrieri and R. Gugel and J. A. M. Guhit and A. Guida and E. Guilloton and S. Guindon and F. Guo and J. Guo and L. Guo and Y. Guo and A. Gupta and R. Gupta and S. Gurbuz and S. S. Gurdasani and G. Gustavino and P. Gutierrez and L. F. Gutierrez Zagazeta and M. Gutsche and C. Gutschow and C. Gwenlan and C. B. Gwilliam and E. S. Haaland and A. Haas and M. Habedank and C. Haber and H. K. Hadavand and A. Hadef and A. I. Hagan and J. J. Hahn and E. H. Haines and M. Haleem and J. Haley and G. D. Hallewell and L. Halser and K. Hamano and M. Hamer and E. J. Hampshire and J. Han and L. Han and S. Han and K. Hanagaki and M. Hance and D. A. Hangal and H. Hanif and M. D. Hank and J. B. Hansen and P. H. Hansen and D. Harada and T. Harenberg and S. Harkusha and M. L. Harris and Y. T. Harris and J. Harrison and N. M. Harrison and P. F. Harrison and N. M. Hartman and N. M. Hartmann and R. Z. Hasan and Y. Hasegawa and F. Haslbeck and S. Hassan and R. Hauser and C. M. Hawkes and R. J. Hawkings and Y. Hayashi and D. Hayden and C. Hayes and R. L. Hayes and C. P. Hays and J. M. Hays and H. S. Hayward and F. He and M. He and Y. He and N. B. Heatley and V. Hedberg and A. L. Heggelund and C. Heidegger and K. K. Heidegger and J. Heilman and S. Heim and T. Heim and J. G. Heinlein and J. J. Heinrich and L. Heinrich and J. Hejbal and A. Held and S. Hellesund and C. M. Helling and S. Hellman and R. C. W. Henderson and L. Henkelmann and A. M. Henriques Correia and H. Herde and Y. Hernández Jiménez and L. M. Herrmann and T. Herrmann and G. Herten and R. Hertenberger and L. Hervas and M. E. Hesping and N. P. Hessey and J. Hessler and M. Hidaoui and N. Hidic and E. Hill and S. J. Hillier and J. R. Hinds and F. Hinterkeuser and M. Hirose and S. Hirose and D. Hirschbuehl and T. G. Hitchings and B. Hiti and J. Hobbs and R. Hobincu and N. Hod and M. C. Hodgkinson and B. H. Hodkinson and A. Hoecker and D. D. Hofer and J. Hofer and M. Holzbock and L. B. A. H. Hommels and B. P. Honan and J. J. Hong and J. Hong and T. M. Hong and B. H. Hooberman and W. H. Hopkins and M. C. Hoppesch and Y. Horii and M. E. Horstmann and S. Hou and M. R. Housenga and A. S. Howard and J. Howarth and J. Hoya and M. Hrabovsky and T. Hryn’ova and P. J. Hsu and S.-C. Hsu and T. Hsu and M. Hu and Q. Hu and S. Huang and X. Huang and Y. Huang and Z. Huang and Z. Hubacek and M. Huebner and F. Huegging and T. B. Huffman and M. Hufnagel Maranha De Faria and C. A. Hugli and M. Huhtinen and S. K. Huiberts and R. Hulsken and N. Huseynov and J. Huston and J. Huth and R. Hyneman and G. Iacobucci and G. Iakovidis and L. Iconomidou-Fayard and J. P. Iddon and P. Iengo and R. Iguchi and Y. Iiyama and T. Iizawa and Y. Ikegami and D. Iliadis and N. Ilic and H. Imam and G. Inacio Goncalves and S. A. Infante Cabanas and T. Ingebretsen Carlson and J. M. Inglis and G. Introzzi and M. Iodice and V. Ippolito and R. K. Irwin and M. Ishino and W. Islam and C. Issever and S. Istin and H. Ito and R. Iuppa and A. Ivina and J. M. Izen and V. Izzo and P. Jacka and P. Jackson and C. S. Jagfeld and G. Jain and P. Jain and K. Jakobs and T. Jakoubek and J. Jamieson and W. Jang and M. Javurkova and P. Jawahar and L. Jeanty and J. Jejelava and P. Jenni and C. E. Jessiman and C. Jia and H. Jia and J. Jia and X. Jia and Z. Jia and C. Jiang and S. Jiggins and J. Jimenez Pena and S. Jin and A. Jinaru and O. Jinnouchi and P. Johansson and K. A. Johns and J. W. Johnson and F. A. Jolly and D. M. Jones and E. Jones and K. S. Jones and P. Jones and R. W. L. Jones and T. J. Jones and H. L. Joos and R. Joshi and J. Jovicevic and X. Ju and J. J. Junggeburth and T. Junkermann and A. Juste Rozas and M. K. Juzek and S. Kabana and A. Kaczmarska and M. Kado and H. Kagan and M. Kagan and A. Kahn and C. Kahra and T. Kaji and E. Kajomovitz and N. Kakati and I. Kalaitzidou and N. J. Kang and D. Kar and K. Karava and E. Karentzos and O. Karkout and S. N. Karpov and Z. M. Karpova and V. Kartvelishvili and A. N. Karyukhin and E. Kasimi and J. Katzy and S. Kaur and K. Kawade and M. P. Kawale and C. Kawamoto and T. Kawamoto and E. F. Kay and F. I. Kaya and S. Kazakos and V. F. Kazanin and Y. Ke and J. M. Keaveney and R. Keeler and G. V. Kehris and J. S. Keller and J. J. Kempster and O. Kepka and J. Kerr and B. P. Kerridge and B. P. Kerševan and L. Keszeghova and R. A. Khan and A. Khanov and A. G. Kharlamov and T. Kharlamova and E. E. Khoda and M. Kholodenko and T. J. Khoo and G. Khoriauli and J. Khubua and Y. A. R. Khwaira and B. Kibirige and D. Kim and D. W. Kim and Y. K. Kim and N. Kimura and M. K. Kingston and A. Kirchhoff and C. Kirfel and F. Kirfel and J. Kirk and A. E. Kiryunin and S. Kita and C. Kitsaki and O. Kivernyk and M. Klassen and C. Klein and L. Klein and M. H. Klein and S. B. Klein and U. Klein and A. Klimentov and T. Klioutchnikova and P. Kluit and S. Kluth and E. Kneringer and T. M. Knight and A. Knue and M. Kobel and D. Kobylianskii and S. F. Koch and M. Kocian and P. Kodyš and D. M. Koeck and P. T. Koenig and T. Koffas and O. Kolay and I. Koletsou and T. Komarek and K. Köneke and A. X. Y. Kong and T. Kono and N. Konstantinidis and P. Kontaxakis and B. Konya and R. Kopeliansky and S. Koperny and K. Korcyl and K. Kordas and A. Korn and S. Korn and I. Korolkov and N. Korotkova and B. Kortman and O. Kortner and S. Kortner and W. H. Kostecka and V. V. Kostyukhin and A. Kotsokechagia and A. Kotwal and A. Koulouris and A. Kourkoumeli-Charalampidi and C. Kourkoumelis and E. Kourlitis and O. Kovanda and R. Kowalewski and W. Kozanecki and A. S. Kozhin and V. A. Kramarenko and G. Kramberger and P. Kramer and M. W. Krasny and A. Krasznahorkay and A. C. Kraus and J. W. Kraus and J. A. Kremer and T. Kresse and L. Kretschmann and J. Kretzschmar and K. Kreul and P. Krieger and K. Krizka and K. Kroeninger and H. Kroha and J. Kroll and K. S. Krowpman and U. Kruchonak and H. Krüger and N. Krumnack and M. C. Kruse and O. Kuchinskaia and S. Kuday and S. Kuehn and R. Kuesters and T. Kuhl and V. Kukhtin and Y. Kulchitsky and S. Kuleshov and M. Kumar and N. Kumari and P. Kumari and A. Kupco and T. Kupfer and A. Kupich and O. Kuprash and H. Kurashige and L. L. Kurchaninov and O. Kurdysh and Y. A. Kurochkin and A. Kurova and M. Kuze and A. K. Kvam and J. Kvita and N. G. Kyriacou and L. A. O. Laatu and C. Lacasta and F. Lacava and H. Lacker and D. Lacour and N. N. Lad and E. Ladygin and A. Lafarge and B. Laforge and T. Lagouri and F. Z. Lahbabi and S. Lai and J. E. Lambert and S. Lammers and W. Lampl and C. Lampoudis and G. Lamprinoudis and A. N. Lancaster and E. Lançon and U. Landgraf and M. P. J. Landon and V. S. Lang and O. K. B. Langrekken and A. J. Lankford and F. Lanni and K. Lantzsch and A. Lanza and M. Lanzac Berrocal and J. F. Laporte and T. Lari and F. Lasagni Manghi and M. Lassnig and V. Latonova and S. D. Lawlor and Z. Lawrence and R. Lazaridou and M. Lazzaroni and H. D. M. Le and E. M. Le Boulicaut and L. T. Le Pottier and B. Leban and A. Lebedev and M. LeBlanc and F. Ledroit-Guillon and S. C. Lee and S. Lee and T. F. Lee and L. L. Leeuw and M. Lefebvre and C. Leggett and G. Lehmann Miotto and M. Leigh and W. A. Leight and W. Leinonen and A. Leisos and M. A. L. Leite and C. E. Leitgeb and R. Leitner and K. J. C. Leney and T. Lenz and S. Leone and C. Leonidopoulos and A. Leopold and R. Les and C. G. Lester and M. Levchenko and J. Levêque and L. J. Levinson and G. Levrini and M. P. Lewicki and C. Lewis and D. J. Lewis and L. Lewitt and A. Li and B. Li and C. Li and C-Q. Li and H. Li and J. Li and K. Li and L. Li and R. Li and S. Li and T. Li and X. Li and Z. Li and S. Liang and Z. Liang and M. Liberatore and B. Liberti and K. Lie and J. Lieber Marin and H. Lien and H. Lin and L. Linden and R. E. Lindley and J. H. Lindon and J. Ling and E. Lipeles and A. Lipniacka and A. Lister and J. D. Little and B. Liu and B. X. Liu and D. Liu and E. H. L. Liu and J. K. K. Liu and K. Liu and M. Liu and M. Y. Liu and P. Liu and Q. Liu and X. Liu and Y. Liu and Y. L. Liu and Y. W. Liu and S. L. Lloyd and E. M. Lobodzinska and P. Loch and E. Lodhi and T. Lohse and K. Lohwasser and E. Loiacono and J. D. Lomas and J. D. Long and I. Longarini and R. Longo and A. Lopez Solis and N. A. Lopez-canelas and N. Lorenzo Martinez and A. M. Lory and M. Losada and G. Löschcke Centeno and O. Loseva and X. Lou and A. Lounis and P. A. Love and G. Lu and M. Lu and S. Lu and Y. J. Lu and H. J. Lubatti and C. Luci and F. L. Lucio Alves and F. Luehring and O. Lukianchuk and B. S. Lunday and O. Lundberg and B. Lund-Jensen and N. A. Luongo and M. S. Lutz and A. B. Lux and D. Lynn and R. Lysak and E. Lytken and V. Lyubushkin and T. Lyubushkina and M. M. Lyukova and M. Firdaus M. Soberi and H. Ma and K. Ma and L. L. Ma and W. Ma and Y. Ma and J. C. MacDonald and P. C. Machado De Abreu Farias and R. Madar and T. Madula and J. Maeda and T. Maeno and P. T. Mafa and H. Maguire and V. Maiboroda and A. Maio and K. Maj and O. Majersky and S. Majewski and N. Makovec and V. Maksimovic and B. Malaescu and Pa. Malecki and V. P. Maleev and F. Malek and M. Mali and D. Malito and U. Mallik and S. Maltezos and S. Malyukov and J. Mamuzic and G. Mancini and M. N. Mancini and G. Manco and J. P. Mandalia and S. S. Mandarry and I. Mandić and L. Manhaes de Andrade Filho and I. M. Maniatis and J. Manjarres Ramos and D. C. Mankad and A. Mann and S. Manzoni and L. Mao and X. Mapekula and A. Marantis and G. Marchiori and M. Marcisovsky and C. Marcon and M. Marinescu and S. Marium and M. Marjanovic and A. Markhoos and M. Markovitch and M. K. Maroun and E. J. Marshall and Z. Marshall and S. Marti-Garcia and J. Martin and T. A. Martin and V. J. Martin and B. Martin dit Latour and L. Martinelli and M. Martinez and P. Martinez Agullo and V. I. Martinez Outschoorn and P. Martinez Suarez and S. Martin-Haugh and G. Martinovicova and V. S. Martoiu and A. C. Martyniuk and A. Marzin and D. Mascione and L. Masetti and J. Masik and A. L. Maslennikov and S. L. Mason and P. Massarotti and P. Mastrandrea and A. Mastroberardino and T. Masubuchi and T. T. Mathew and J. Matousek and D. M. Mattern and J. Maurer and T. Maurin and A. J. Maury and B. Maček and D. A. Maximov and A. E. May and R. Mazini and I. Maznas and M. Mazza and S. M. Mazza and E. Mazzeo and J. P. Mc Gowan and S. P. Mc Kee and C. A. Mc Lean and C. C. McCracken and E. F. McDonald and A. E. McDougall and L. F. Mcelhinney and J. A. Mcfayden and R. P. McGovern and R. P. Mckenzie and T. C. Mclachlan and D. J. Mclaughlin and S. J. McMahon and C. M. Mcpartland and R. A. McPherson and S. Mehlhase and A. Mehta and D. Melini and B. R. Mellado Garcia and A. H. Melo and F. Meloni and A. M. Mendes Jacques Da Costa and H. Y. Meng and L. Meng and S. Menke and M. Mentink and E. Meoni and G. Mercado and S. Merianos and C. Merlassino and C. Meroni and J. Metcalfe and A. S. Mete and E. Meuser and C. Meyer and J-P. Meyer and R. P. Middleton and L. Mijović and G. Mikenberg and M. Mikestikova and M. Mikuž and H. Mildner and A. Milic and D. W. Miller and E. H. Miller and L. S. Miller and A. Milov and D. A. Milstead and T. Min and A. A. Minaenko and I. A. Minashvili and A. I. Mincer and B. Mindur and M. Mineev and Y. Mino and L. M. Mir and M. Miralles Lopez and M. Mironova and M. C. Missio and A. Mitra and V. A. Mitsou and Y. Mitsumori and O. Miu and P. S. Miyagawa and T. Mkrtchyan and M. Mlinarevic and T. Mlinarevic and M. Mlynarikova and S. Mobius and P. Mogg and M. H. Mohamed Farook and A. F. Mohammed and S. Mohapatra and G. Mokgatitswane and L. Moleri and B. Mondal and S. Mondal and K. Mönig and E. Monnier and L. Monsonis Romero and J. Montejo Berlingen and A. Montella and M. Montella and F. Montereali and F. Monticelli and S. Monzani and A. Morancho Tarda and N. Morange and A. L. Moreira De Carvalho and M. Moreno Llácer and C. Moreno Martinez and J. M. Moreno Perez and P. Morettini and S. Morgenstern and M. Morii and M. Morinaga and M. Moritsu and F. Morodei and P. Moschovakos and B. Moser and M. Mosidze and T. Moskalets and P. Moskvitina and J. Moss and P. Moszkowicz and A. Moussa and Y. Moyal and E. J. W. Moyse and O. Mtintsilana and S. Muanza and J. Mueller and D. Muenstermann and R. Müller and G. A. Mullier and A. J. Mullin and J. J. Mullin and A. E. Mulski and D. P. Mungo and D. Munoz Perez and F. J. Munoz Sanchez and M. Murin and W. J. Murray and M. Muškinja and C. Mwewa and A. G. Myagkov and A. J. Myers and G. Myers and M. Myska and B. P. Nachman and K. Nagai and K. Nagano and R. Nagasaka and J. L. Nagle and E. Nagy and A. M. Nairz and Y. Nakahama and K. Nakamura and K. Nakkalil and H. Nanjo and E. A. Narayanan and Y. Narukawa and I. Naryshkin and L. Nasella and S. Nasri and C. Nass and G. Navarro and J. Navarro-Gonzalez and A. Nayaz and P. Y. Nechaeva and S. Nechaeva and F. Nechansky and L. Nedic and T. J. Neep and A. Negri and M. Negrini and C. Nellist and C. Nelson and K. Nelson and S. Nemecek and M. Nessi and M. S. Neubauer and F. Neuhaus and J. Newell and P. R. Newman and Y. W. Y. Ng and B. Ngair and H. D. N. Nguyen and R. B. Nickerson and R. Nicolaidou and J. Nielsen and M. Niemeyer and J. Niermann and N. Nikiforou and V. Nikolaenko and I. Nikolic-Audit and P. Nilsson and I. Ninca and G. Ninio and A. Nisati and N. Nishu and R. Nisius and N. Nitika and J-E. Nitschke and E. K. Nkadimeng and T. Nobe and T. Nommensen and M. B. Norfolk and B. J. Norman and M. Noury and J. Novak and T. Novak and R. Novotny and L. Nozka and K. Ntekas and N. M. J. Nunes De Moura Junior and J. Ocariz and A. Ochi and I. Ochoa and S. Oerdek and J. T. Offermann and A. Ogrodnik and A. Oh and C. C. Ohm and H. Oide and R. Oishi and M. L. Ojeda and Y. Okumura and L. F. Oleiro Seabra and I. Oleksiyuk and S. A. Olivares Pino and G. Oliveira Correa and D. Oliveira Damazio and J. L. Oliver and Ö. O. Öncel and A. P. O’Neill and A. Onofre and P. U. E. Onyisi and M. J. Oreglia and D. Orestano and R. S. Orr and L. M. Osojnak and Y. Osumi and G. Otero y Garzon and H. Otono and P. S. Ott and G. J. Ottino and M. Ouchrif and F. Ould-Saada and T. Ovsiannikova and M. Owen and R. E. Owen and V. E. Ozcan and F. Ozturk and N. Ozturk and S. Ozturk and H. A. Pacey and A. Pacheco Pages and C. Padilla Aranda and G. Padovano and S. Pagan Griso and G. Palacino and A. Palazzo and J. Pampel and J. Pan and T. Pan and D. K. Panchal and C. E. Pandini and J. G. Panduro Vazquez and H. D. Pandya and H. Pang and P. Pani and G. Panizzo and L. Panwar and L. Paolozzi and S. Parajuli and A. Paramonov and C. Paraskevopoulos and D. Paredes Hernandez and A. Pareti and K. R. Park and T. H. Park and F. Parodi and V. A. Parrish and J. A. Parsons and U. Parzefall and B. Pascual Dias and L. Pascual Dominguez and E. Pasqualucci and S. Passaggio and F. Pastore and P. Patel and U. M. Patel and J. R. Pater and T. Pauly and F. Pauwels and C. I. Pazos and M. Pedersen and R. Pedro and S. V. Peleganchuk and O. Penc and E. A. Pender and S. Peng and G. D. Penn and K. E. Penski and M. Penzin and B. S. Peralva and A. P. Pereira Peixoto and L. Pereira Sanchez and D. V. Perepelitsa and G. Perera and E. Perez Codina and M. Perganti and H. Pernegger and S. Perrella and O. Perrin and K. Peters and R. F. Y. Peters and B. A. Petersen and T. C. Petersen and E. Petit and V. Petousis and C. Petridou and T. Petru and A. Petrukhin and M. Pettee and A. Petukhov and K. Petukhova and R. Pezoa and L. Pezzotti and G. Pezzullo and A. J. Pfleger and T. M. Pham and T. Pham and P. W. Phillips and G. Piacquadio and E. Pianori and F. Piazza and R. Piegaia and D. Pietreanu and A. D. Pilkington and M. Pinamonti and J. L. Pinfold and B. C. Pinheiro Pereira and J. Pinol Bel and A. E. Pinto Pinoargote and L. Pintucci and K. M. Piper and A. Pirttikoski and D. A. Pizzi and L. Pizzimento and M.-A. Pleier and V. Pleskot and E. Plotnikova and G. Poddar and R. Poettgen and L. Poggioli and S. Polacek and G. Polesello and A. Poley and A. Polini and C. S. Pollard and Z. B. Pollock and E. Pompa Pacchi and N. I. Pond and D. Ponomarenko and L. Pontecorvo and S. Popa and G. A. Popeneciu and A. Poreba and D. M. Portillo Quintero and S. Pospisil and M. A. Postill and P. Postolache and K. Potamianos and P. A. Potepa and I. N. Potrap and C. J. Potter and H. Potti and J. Poveda and M. E. Pozo Astigarraga and A. Prades Ibanez and J. Pretel and D. Price and M. Primavera and L. Primomo and M. A. Principe Martin and R. Privara and T. Procter and M. L. Proffitt and N. Proklova and K. Prokofiev and G. Proto and J. Proudfoot and M. Przybycien and W. W. Przygoda and A. Psallidas and J. E. Puddefoot and D. Pudzha and D. Pyatiizbyantseva and J. Qian and R. Qian and D. Qichen and Y. Qin and T. Qiu and A. Quadt and M. Queitsch-Maitland and G. Quetant and R. P. Quinn and G. Rabanal Bolanos and D. Rafanoharana and F. Raffaeli and F. Ragusa and J. L. Rainbolt and J. A. Raine and S. Rajagopalan and E. Ramakoti and L. Rambelli and I. A. Ramirez-Berend and K. Ran and D. S. Rankin and N. P. Rapheeha and H. Rasheed and V. Raskina and D. F. Rassloff and A. Rastogi and S. Rave and S. Ravera and B. Ravina and I. Ravinovich and M. Raymond and A. L. Read and N. P. Readioff and D. M. Rebuzzi and A. S. Reed and K. Reeves and J. A. Reidelsturz and D. Reikher and A. Rej and C. Rembser and H. Ren and M. Renda and F. Renner and A. G. Rennie and A. L. Rescia and S. Resconi and M. Ressegotti and S. Rettie and W. F. Rettie and J. G. Reyes Rivera and E. Reynolds and O. L. Rezanova and P. Reznicek and H. Riani and N. Ribaric and E. Ricci and R. Richter and S. Richter and E. Richter-Was and M. Ridel and S. Ridouani and P. Rieck and P. Riedler and E. M. Riefel and J. O. Rieger and M. Rijssenbeek and M. Rimoldi and L. Rinaldi and P. Rincke and M. P. Rinnagel and G. Ripellino and I. Riu and J. C. Rivera Vergara and F. Rizatdinova and E. Rizvi and B. R. Roberts and S. S. Roberts and D. Robinson and M. Robles Manzano and A. Robson and A. Rocchi and C. Roda and S. Rodriguez Bosca and Y. Rodriguez Garcia and A. M. Rodríguez Vera and S. Roe and J. T. Roemer and O. Røhne and R. A. Rojas and C. P. A. Roland and J. Roloff and A. Romaniouk and E. Romano and M. Romano and A. C. Romero Hernandez and N. Rompotis and L. Roos and S. Rosati and B. J. Rosser and E. Rossi and L. P. Rossi and L. Rossini and R. Rosten and M. Rotaru and B. Rottler and C. Rougier and D. Rousseau and D. Rousso and A. Roy and S. Roy-Garand and A. Rozanov and Z. M. A. Rozario and Y. Rozen and A. Rubio Jimenez and V. H. Ruelas Rivera and T. A. Ruggeri and A. Ruggiero and A. Ruiz-Martinez and A. Rummler and Z. Rurikova and N. A. Rusakovich and H. L. Russell and G. Russo and J. P. Rutherfoord and S. Rutherford Colmenares and M. Rybar and E. B. Rye and A. Ryzhov and J. A. Sabater Iglesias and H. F-W. Sadrozinski and F. Safai Tehrani and S. Saha and M. Sahinsoy and A. Saibel and M. Saimpert and M. Saito and T. Saito and A. Sala and D. Salamani and A. Salnikov and J. Salt and A. Salvador Salas and D. Salvatore and F. Salvatore and A. Salzburger and D. Sammel and E. Sampson and D. Sampsonidis and D. Sampsonidou and J. Sánchez and V. Sanchez Sebastian and H. Sandaker and C. O. Sander and J. A. Sandesara and M. Sandhoff and C. Sandoval and L. Sanfilippo and D. P. C. Sankey and T. Sano and A. Sansoni and L. Santi and C. Santoni and H. Santos and A. Santra and E. Sanzani and K. A. Saoucha and J. G. Saraiva and J. Sardain and O. Sasaki and K. Sato and C. Sauer and E. Sauvan and P. Savard and R. Sawada and C. Sawyer and L. Sawyer and C. Sbarra and A. Sbrizzi and T. Scanlon and J. Schaarschmidt and U. Schäfer and A. C. Schaffer and D. Schaile and R. D. Schamberger and C. Scharf and M. M. Schefer and V. A. Schegelsky and D. Scheirich and M. Schernau and C. Scheulen and C. Schiavi and M. Schioppa and B. Schlag and S. Schlenker and J. Schmeing and M. A. Schmidt and K. Schmieden and C. Schmitt and N. Schmitt and S. Schmitt and L. Schoeffel and A. Schoening and P. G. Scholer and E. Schopf and M. Schott and J. Schovancova and S. Schramm and T. Schroer and H-C. Schultz-Coulon and M. Schumacher and B. A. Schumm and Ph. Schune and H. R. Schwartz and A. Schwartzman and T. A. Schwarz and Ph. Schwemling and R. Schwienhorst and F. G. Sciacca and A. Sciandra and G. Sciolla and F. Scuri and C. D. Sebastiani and K. Sedlaczek and S. C. Seidel and A. Seiden and B. D. Seidlitz and C. Seitz and J. M. Seixas and G. Sekhniaidze and L. Selem and N. Semprini-Cesari and A. Semushin and D. Sengupta and V. Senthilkumar and L. Serin and M. Sessa and H. Severini and F. Sforza and A. Sfyrla and Q. Sha and E. Shabalina and H. Shaddix and A. H. Shah and R. Shaheen and J. D. Shahinian and D. Shaked Renous and L. Y. Shan and M. Shapiro and A. Sharma and A. S. Sharma and P. Sharma and P. B. Shatalov and K. Shaw and S. M. Shaw and Q. Shen and D. J. Sheppard and P. Sherwood and L. Shi and X. Shi and S. Shimizu and C. O. Shimmin and I. P. J. Shipsey and S. Shirabe and M. Shiyakova and M. J. Shochet and D. R. Shope and B. Shrestha and S. Shrestha and I. Shreyber and M. J. Shroff and P. Sicho and A. M. Sickles and E. Sideras Haddad and A. C. Sidley and A. Sidoti and F. Siegert and Dj. Sijacki and F. Sili and J. M. Silva and I. Silva Ferreira and M. V. Silva Oliveira and S. B. Silverstein and S. Simion and R. Simoniello and E. L. Simpson and H. Simpson and L. R. Simpson and S. Simsek and S. Sindhu and P. Sinervo and S. N. Singh and S. Singh and S. Sinha and M. Sioli and I. Siral and E. Sitnikova and J. Sjölin and A. Skaf and E. Skorda and P. Skubic and M. Slawinska and I. Slazyk and V. Smakhtin and B. H. Smart and S. Yu. Smirnov and Y. Smirnov and L. N. Smirnova and O. Smirnova and A. C. Smith and D. R. Smith and E. A. Smith and J. L. Smith and R. Smith and H. Smitmanns and M. Smizanska and K. Smolek and A. A. Snesarev and H. L. Snoek and S. Snyder and R. Sobie and A. Soffer and C. A. Solans Sanchez and E. Yu. Soldatov and U. Soldevila and A. A. Solodkov and S. Solomon and A. Soloshenko and K. Solovieva and O. V. Solovyanov and P. Sommer and A. Sonay and W. Y. Song and A. Sopczak and A. L. Sopio and F. Sopkova and J. D. Sorenson and I. R. Sotarriva Alvarez and V. Sothilingam and O. J. Soto Sandoval and S. Sottocornola and R. Soualah and Z. Soumaimi and D. South and N. Soybelman and S. Spagnolo and M. Spalla and D. Sperlich and B. Spisso and D. P. Spiteri and M. Spousta and E. J. Staats and R. Stamen and A. Stampekis and E. Stanecka and W. Stanek-Maslouska and M. V. Stange and B. Stanislaus and M. M. Stanitzki and B. Stapf and E. A. Starchenko and G. H. Stark and J. Stark and P. Staroba and P. Starovoitov and R. Staszewski and G. Stavropoulos and A. Stefl and P. Steinberg and B. Stelzer and H. J. Stelzer and O. Stelzer-Chilton and H. Stenzel and T. J. Stevenson and G. A. Stewart and J. R. Stewart and M. C. Stockton and G. Stoicea and M. Stolarski and S. Stonjek and A. Straessner and J. Strandberg and S. Strandberg and M. Stratmann and M. Strauss and T. Strebler and P. Strizenec and R. Ströhmer and D. M. Strom and R. Stroynowski and A. Strubig and S. A. Stucci and B. Stugu and J. Stupak and N. A. Styles and D. Su and S. Su and W. Su and X. Su and D. Suchy and K. Sugizaki and V. V. Sulin and M. J. Sullivan and D. M. S. Sultan and L. Sultanaliyeva and S. Sultansoy and S. Sun and W. Sun and O. Sunneborn Gudnadottir and N. Sur and M. R. Sutton and H. Suzuki and M. Svatos and M. Swiatlowski and T. Swirski and I. Sykora and M. Sykora and T. Sykora and D. Ta and K. Tackmann and A. Taffard and R. Tafirout and J. S. Tafoya Vargas and Y. Takubo and M. Talby and A. A. Talyshev and K. C. Tam and N. M. Tamir and A. Tanaka and J. Tanaka and R. Tanaka and M. Tanasini and Z. Tao and S. Tapia Araya and S. Tapprogge and A. Tarek Abouelfadl Mohamed and S. Tarem and K. Tariq and G. Tarna and G. F. Tartarelli and M. J. Tartarin and P. Tas and M. Tasevsky and E. Tassi and A. C. Tate and G. Tateno and Y. Tayalati and G. N. Taylor and W. Taylor and P. Teixeira-Dias and J. J. Teoh and K. Terashi and J. Terron and S. Terzo and M. Testa and R. J. Teuscher and A. Thaler and O. Theiner and T. Theveneaux-Pelzer and O. Thielmann and D. W. Thomas and J. P. Thomas and E. A. Thompson and P. D. Thompson and E. Thomson and R. E. Thornberry and C. Tian and Y. Tian and V. Tikhomirov and Yu. A. Tikhonov and S. Timoshenko and D. Timoshyn and E. X. L. Ting and P. Tipton and A. Tishelman-Charny and S. H. Tlou and K. Todome and S. Todorova-Nova and S. Todt and L. Toffolin and M. Togawa and J. Tojo and S. Tokár and O. Toldaiev and G. Tolkachev and M. Tomoto and L. Tompkins and E. Torrence and H. Torres and E. Torró Pastor and M. Toscani and C. Tosciri and M. Tost and D. R. Tovey and I. S. Trandafir and T. Trefzger and A. Tricoli and I. M. Trigger and S. Trincaz-Duvoid and D. A. Trischuk and A. Tropina and L. Truong and M. Trzebinski and A. Trzupek and F. Tsai and M. Tsai and A. Tsiamis and P. V. Tsiareshka and S. Tsigaridas and A. Tsirigotis and V. Tsiskaridze and E. G. Tskhadadze and M. Tsopoulou and Y. Tsujikawa and I. I. Tsukerman and V. Tsulaia and S. Tsuno and K. Tsuri and D. Tsybychev and Y. Tu and A. Tudorache and V. Tudorache and S. Turchikhin and I. Turk Cakir and R. Turra and T. Turtuvshin and P. M. Tuts and S. Tzamarias and E. Tzovara and F. Ukegawa and P. A. Ulloa Poblete and E. N. Umaka and G. Unal and A. Undrus and G. Unel and J. Urban and P. Urrejola and G. Usai and R. Ushioda and M. Usman and F. Ustuner and Z. Uysal and V. Vacek and B. Vachon and T. Vafeiadis and A. Vaitkus and C. Valderanis and E. Valdes Santurio and M. Valente and S. Valentinetti and A. Valero and E. Valiente Moreno and A. Vallier and J. A. Valls Ferrer and D. R. Van Arneman and T. R. Van Daalen and A. Van Der Graaf and P. Van Gemmeren and M. Van Rijnbach and S. Van Stroud and I. Van Vulpen and P. Vana and M. Vanadia and U. M. Vande Voorde and W. Vandelli and E. R. Vandewall and D. Vannicola and L. Vannoli and R. Vari and E. W. Varnes and C. Varni and D. Varouchas and L. Varriale and K. E. Varvell and M. E. Vasile and L. Vaslin and A. Vasyukov and L. M. Vaughan and R. Vavricka and T. Vazquez Schroeder and J. Veatch and V. Vecchio and M. J. Veen and I. Veliscek and L. M. Veloce and F. Veloso and S. Veneziano and A. Ventura and S. Ventura Gonzalez and A. Verbytskyi and M. Verducci and C. Vergis and M. Verissimo De Araujo and W. Verkerke and J. C. Vermeulen and C. Vernieri and M. Vessella and M. C. Vetterli and A. Vgenopoulos and N. Viaux Maira and T. Vickey and O. E. Vickey Boeriu and G. H. A. Viehhauser and L. Vigani and M. Vigl and M. Villa and M. Villaplana Perez and E. M. Villhauer and E. Vilucchi and M. G. Vincter and A. Visibile and C. Vittori and I. Vivarelli and E. Voevodina and F. Vogel and J. C. Voigt and P. Vokac and Yu. Volkotrub and E. Von Toerne and B. Vormwald and K. Vorobev and M. Vos and K. Voss and M. Vozak and L. Vozdecky and N. Vranjes and M. Vranjes Milosavljevic and M. Vreeswijk and N. K. Vu and R. Vuillermet and O. Vujinovic and I. Vukotic and I. K. Vyas and S. Wada and C. Wagner and J. M. Wagner and W. Wagner and S. Wahdan and H. Wahlberg and C. H. Waits and J. Walder and R. Walker and W. Walkowiak and A. Wall and E. J. Wallin and T. Wamorkar and A. Z. Wang and C. Wang and H. Wang and J. Wang and P. Wang and R. Wang and S. M. Wang and S. Wang and T. Wang and W. T. Wang and W. Wang and X. Wang and Y. Wang and Z. Wang and A. Warburton and R. J. Ward and A. L. Warnerbring and N. Warrack and S. Waterhouse and A. T. Watson and H. Watson and M. F. Watson and E. Watton and G. Watts and B. M. Waugh and J. M. Webb and C. Weber and H. A. Weber and M. S. Weber and S. M. Weber and C. Wei and Y. Wei and A. R. Weidberg and E. J. Weik and J. Weingarten and C. Weiser and C. J. Wells and T. Wenaus and B. Wendland and T. Wengler and N. S. Wenke and N. Wermes and M. Wessels and A. M. Wharton and A. S. White and A. White and M. J. White and D. Whiteson and L. Wickremasinghe and W. Wiedenmann and M. Wielers and C. Wiglesworth and D. J. Wilbern and H. G. Wilkens and J. J. H. Wilkinson and D. M. Williams and H. H. Williams and S. Williams and S. Willocq and B. J. Wilson and D. J. Wilson and P. J. Windischhofer and F. I. Winkel and F. Winklmeier and B. T. Winter and M. Wittgen and M. Wobisch and T. Wojtkowski and Z. Wolffs and J. Wollrath and M. W. Wolter and H. Wolters and M. C. Wong and E. L. Woodward and S. D. Worm and B. K. Wosiek and K. W. Woźniak and S. Wozniewski and K. Wraight and C. Wu and M. Wu and S. L. Wu and X. Wu and Y. Wu and Z. Wu and J. Wuerzinger and T. R. Wyatt and B. M. Wynne and S. Xella and L. Xia and M. Xia and M. Xie and A. Xiong and J. Xiong and D. Xu and H. Xu and L. Xu and R. Xu and T. Xu and Y. Xu and Z. Xu and B. Yabsley and S. Yacoob and Y. Yamaguchi and E. Yamashita and H. Yamauchi and T. Yamazaki and Y. Yamazaki and S. Yan and Z. Yan and H. J. Yang and H. T. Yang and S. Yang and T. Yang and X. Yang and Y. Yang and W-M. Yao and H. Ye and J. Ye and S. Ye and X. Ye and Y. Yeh and I. Yeletskikh and B. Yeo and M. R. Yexley and T. P. Yildirim and P. Yin and K. Yorita and S. Younas and C. J. S. Young and C. Young and C. Yu and Y. Yu and J. Yuan and M. Yuan and R. Yuan and L. Yue and M. Zaazoua and B. Zabinski and I. Zahir and Z. K. Zak and T. Zakareishvili and S. Zambito and J. A. Zamora Saa and J. Zang and D. Zanzi and R. Zanzottera and O. Zaplatilek and C. Zeitnitz and H. Zeng and J. C. Zeng and D. T. Zenger, Jr and O. Zenin and T. Ženiš and S. Zenz and S. Zerradi and D. Zerwas and M. Zhai and D. F. Zhang and J. Zhang and K. Zhang and L. Zhang and P. Zhang and R. Zhang and S. Zhang and T. Zhang and X. Zhang and Y. Zhang and Z. Zhang and H. Zhao and T. Zhao and Y. Zhao and Z. Zhao and A. Zhemchugov and J. Zheng and K. Zheng and X. Zheng and Z. Zheng and D. Zhong and B. Zhou and H. Zhou and N. Zhou and Y. Zhou and C. G. Zhu and J. Zhu and X. Zhu and Y. Zhu and X. Zhuang and K. Zhukov and N. I. Zimine and J. Zinsser and M. Ziolkowski and L. Živković and A. Zoccoli and K. Zoch and T. G. Zorbas and O. Zormpa and W. Zou and L. Zwalinski}, doi = {10.1103/PhysRevLett.134.142301}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {142301}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of tt¯ production in Pb+Pb collisions at sNN=5.02 TeV with the ATLAS detector}, volume = {134}, year = {2025}, }
• (2025). Phases of theories with ZN 1-form symmetry, and the roles of center vortices and magnetic monopoles. PRL, 134(14), 141902. (www)

  @article{ , abstract = {We analyze the phases of theories having a microscopic Z N 1-form symmetry, starting with a topological BF theory and deforming it so that only the microscopic symmetry is preserved. These theories have a well-defined notion of confinement, prototypical examples being pure SU ( N ) and Z N gauge theories in the continuum and on the lattice. Our analysis shows that the generic phases are in d = 2 , only the confined phase; in d = 3 , both the confined phase and the topological BF phase; and in d = 4 , the confined phase, the topological BF phase, and a Coulomb phase. We construct a Z N lattice gauge theory with a deformation that, surprisingly, produces up to ( N − 1 ) photons. We give an interpretation of these findings in terms of the behaviors of two competing drivers of confinement—magnetic monopoles and center vortices—and conclude that proliferation of center vortices is necessary but insufficient for confinement, while proliferation of magnetic monopoles is both necessary and sufficient.}, archive = {J_PRL}, author = {Mendel Nguyen and Tin Sulejmanpasic and Mithat Ünsal}, doi = {10.1103/PhysRevLett.134.141902}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {141902}, shortjournal = {Phys. Rev. Lett.}, title = {Phases of theories with ZN 1-form symmetry, and the roles of center vortices and magnetic monopoles}, volume = {134}, year = {2025}, }
• (2025). Novel azimuthal observables from two-photon collision at e+e− colliders. PRL, 134(14), 141901. (www)

  @article{ , abstract = {In this Letter, we advocate a set of novel azimuthal-angle-related observables associated with exclusive hadron production from two-photon fusion at e + e − colliders, taking the γ γ → π π as a benchmark process. As a direct consequence of the linearly polarized quasireal photons emitted off the electron and positron beams, the cos 2 ϕ azimuthal asymmetry in dipion production is predicted within the transverse-momentum-dependent factorization framework. In numerical analysis, we take the helicity amplitudes of γ γ → π π determined from the partial wave solutions in dispersion relation as input, and find that the predicted cos 2 ϕ azimuthal modulation may reach 40% for the typical kinematical setup of Belle 2 and BESIII experiments. Future accurate measurement of this azimuthal asymmetry may facilitate the direct extraction of the relative phase between two helicity amplitudes with photon helicity configurations + + and + − . This knowledge provides a valuable input for the dispersive determination of the hadronic light-by-light contributions.}, archive = {J_PRL}, author = {Yu Jia and Jian Zhou and Ya-jin Zhou}, doi = {10.1103/PhysRevLett.134.141901}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {141901}, shortjournal = {Phys. Rev. Lett.}, title = {Novel azimuthal observables from two-photon collision at e+e− colliders}, volume = {134}, year = {2025}, }
• (2025). Wilson loops with lagrangians: Large-spin operator product expansion and cusp anomalous dimension dictionary. PRL, 134(14), 141601. (www)

  @article{ , abstract = {In the context of planar conformal gauge theory, we study five-point correlation functions between the interaction Lagrangian and four of the lightest single-trace, gauge-invariant scalar primaries. After performing two light-cone operator product expansions (OPEs), we express this correlator in terms of the three-point functions between two leading-twist spinning operators and the Lagrangian. For finite values of spin, we compute these structure constants in perturbation theory up to two loops in N = 4 super Yang-Mills theory. Large values of spin are captured by null polygon kinematics, where we use dualities with null polygon Wilson loops as well as factorization properties to bootstrap the universal behavior of the structure constants at all loops. We find explicit maps that relate the Lagrangian structure constants with the leading-twist anomalous dimension. From the large-spin map, we recover the cusp anomalous dimension at strong and weak coupling, including genus-one terms.}, archive = {J_PRL}, author = {Till Bargheer and Carlos Bercini and Bruno Fernandes and Vasco Gonçalves and Jeremy Mann}, doi = {10.1103/PhysRevLett.134.141601}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {141601}, shortjournal = {Phys. Rev. Lett.}, title = {Wilson loops with lagrangians: Large-spin operator product expansion and cusp anomalous dimension dictionary}, volume = {134}, year = {2025}, }
• (2025). Resonant excitation of quasinormal modes of black holes. PRL, 134(14), 141401. (www)

  @article{ , abstract = {We elucidate that a distinctive resonant excitation between quasinormal modes (QNMs) of black holes emerges as a universal phenomenon at an avoided crossing near the exceptional point through high-precision numerical analysis and theory of QNMs based on the framework of non-Hermitian physics. This resonant phenomenon not only allows us to decipher a long-standing mystery concerning the peculiar behaviors of QNMs but also stands as a novel beacon for characterizing black hole spacetime geometry. Our findings pave the way for rigorous examinations of black holes and the exploration of new physics in gravity.}, archive = {J_PRL}, author = {Hayato Motohashi}, doi = {10.1103/PhysRevLett.134.141401}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {141401}, shortjournal = {Phys. Rev. Lett.}, title = {Resonant excitation of quasinormal modes of black holes}, volume = {134}, year = {2025}, }
• (2025). Search for light dark matter with NEWS-G at the laboratoire souterrain de modane using a methane target. PRL, 134(14), 141002. (www)

  @article{ , abstract = {The NEWS-G direct detection experiment uses spherical proportional counters to search for light dark matter candidates. New results from a 10 day physics run with a 135 cm in diameter spherical proportional counter at the Laboratoire Souterrain de Modane are reported. The target consists of 114 g of methane, providing sensitivity to dark matter spin-dependent coupling to protons. New constraints are presented in the mass range 0.17 to 1.2 GeV / c 2 , with a 90% confidence level cross-section upper limit of 30.9 pb for a mass of 0.76 GeV / c 2 .}, archive = {J_PRL}, author = {NEWS-G Collaboration and M. M. Arora and L. Balogh and C. Beaufort and A. Brossard and M. Chapellier and J. Clarke and E. C. Corcoran and J.-M. Coquillat and A. Dastgheibi-Fard and Y. Deng and D. Durnford and C. Garrah and G. Gerbier and I. Giomataris and G. Giroux and P. Gorel and M. Gros and P. Gros and O. Guillaudin and E. W. Hoppe and I. Katsioulas and F. Kelly and P. Knights and P. Lautridou and A. Makowski and I. Manthos and R. D. Martin and J. Matthews and H. M. McCallum and H. Meadows and L. Millins and J.-F. Muraz and T. Neep and K. Nikolopoulos and N. Panchal and M.-C. Piro and N. Rowe and D. Santos and G. Savvidis and I. Savvidis and D. Spathara and F. Vazquez de Sola Fernandez and R. Ward}, doi = {10.1103/PhysRevLett.134.141002}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {141002}, shortjournal = {Phys. Rev. Lett.}, title = {Search for light dark matter with NEWS-G at the laboratoire souterrain de modane using a methane target}, volume = {134}, year = {2025}, }
• (2025). Dimming starlight with dark compact objects. PRL, 134(14), 141001. (www)

  @article{ , abstract = {We demonstrate a new technique to search for dark compact objects. When dark matter comprising a dark compact object interacts with photons, the compact object can disperse light traveling though it. As these objects pass between Earth and a distant star, they act as “lampshades” that dim the star. We examine how dimming effects from clumps of dark matter in the Galaxy could be searched for in microlensing surveys, which measure the brightness of stars as a function of time. Using the EROS-2 and OGLE surveys, we show that a dimming analysis of existing data can be used to constrain dark sectors and could be used to discover dark matter in compact objects.}, archive = {J_PRL}, author = {Joseph Bramante and Melissa D. Diamond and J. Leo Kim}, doi = {10.1103/PhysRevLett.134.141001}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {141001}, shortjournal = {Phys. Rev. Lett.}, title = {Dimming starlight with dark compact objects}, volume = {134}, year = {2025}, }
• (2025). Transition of anticoncentration in gaussian boson sampling. PRL, 134(14), 140601. (www)

  @article{ , abstract = {Gaussian boson sampling is a promising method for experimental demonstrations of quantum advantage because it is easier to implement than other comparable schemes. While most of the properties of Gaussian boson sampling are understood to the same degree as for these other schemes, we understand relatively little about the statistical properties of its output distribution. The most relevant statistical property, from the perspective of demonstrating quantum advantage, is the “anticoncentration” of the output distribution as measured by its second moment. The degree of anticoncentration features in arguments for the complexity-theoretic hardness of Gaussian boson sampling. In this Letter, we develop a graph-theoretic framework for analyzing the moments of the Gaussian boson sampling distribution. Using this framework, we show that Gaussian boson sampling undergoes a transition in anticoncentration as a function of the number of modes that are initially squeezed compared to the number of photons measured at the end of the circuit. When the number of initially squeezed modes scales sufficiently slowly with the number of photons, there is a lack of anticoncentration. However, if the number of initially squeezed modes scales quickly enough, the output probabilities anticoncentrate weakly.}, archive = {J_PRL}, author = {Adam Ehrenberg and Joseph T. Iosue and Abhinav Deshpande and Dominik Hangleiter and Alexey V. Gorshkov}, doi = {10.1103/PhysRevLett.134.140601}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {140601}, shortjournal = {Phys. Rev. Lett.}, title = {Transition of anticoncentration in gaussian boson sampling}, volume = {134}, year = {2025}, }
• (2025). Mixing time of open quantum systems via hypocoercivity. PRL, 134(14), 140405. (www)

  @article{ , abstract = {Understanding the mixing of open quantum systems is a fundamental problem in physics and quantum information science. Existing approaches for estimating the mixing time often rely on the spectral gap estimation of the Lindbladian generator, which can be challenging to obtain in practice. We propose a novel theoretical framework to estimate the mixing time of open quantum systems that treats the Hamiltonian and dissipative part separately, thus circumventing the need for a priori estimation of the spectral gap of the full Lindbladian generator. This framework yields mixing time estimates for a class of quantum systems that are otherwise hard to analyze, even though it does not apply to arbitrary Lindbladians. The technique is based on the construction of an energy functional inspired by the hypocoercivity of (classical) kinetic theory.}, archive = {J_PRL}, author = {Di Fang and Jianfeng Lu and Yu Tong}, doi = {10.1103/PhysRevLett.134.140405}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {140405}, shortjournal = {Phys. Rev. Lett.}, title = {Mixing time of open quantum systems via hypocoercivity}, volume = {134}, year = {2025}, }
• (2025). Full eigenstate thermalization via free cumulants in quantum lattice systems. PRL, 134(14), 140404. (www)

  @article{ , abstract = {The eigenstate thermalization hypothesis (ETH) has been established as the general framework to understand quantum statistical mechanics. Only recently has the attention been paid to so-called full ETH, which accounts for higher-order correlations among matrix elements, and that can be rationalized theoretically using the language of free probability. In this work, we perform the first numerical investigation of the full ETH in physical many-body systems with local interactions by testing the decomposition of higher-order correlators into thermal free cumulants for local operators. We perform exact diagonalization on two classes of local nonintegrable (chaotic) quantum many-body systems: spin chain Hamiltonians and Floquet brickwork unitary circuits. We show that the dynamics of four-time correlation functions are encoded in fourth-order free cumulants, as predicted by ETH. Their dependence on frequency encodes the physical properties of local many-body systems and distinguishes them from structureless, rotationally invariant ensembles of random matrices.}, archive = {J_PRL}, author = {Silvia Pappalardi and Felix Fritzsch and Tomaž Prosen}, doi = {10.1103/PhysRevLett.134.140404}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {140404}, shortjournal = {Phys. Rev. Lett.}, title = {Full eigenstate thermalization via free cumulants in quantum lattice systems}, volume = {134}, year = {2025}, }
• (2025). Operational work fluctuation theorem for open quantum systems. PRL, 134(14), 140403. (www)

  @article{ , abstract = {The classical Jarzynski equality establishes an exact relation between the stochastic work performed on a system driven out of thermal equilibrium and the free energy difference in a corresponding quasistatic process. This fluctuation theorem bears experimental relevance, as it enables the determination of the free energy difference through the measurement of externally applied work in a nonequilibrium process. In the quantum case, the Jarzynski equality only holds if the measurement procedure of the stochastic work is drastically changed: it is replaced by a so-called two-point measurement scheme that requires the knowledge of the initial and final Hamiltonian and therefore lacks the predictive power for the free energy difference that the classical Jarzynski equation is known for. Here, we propose a quantum fluctuation theorem that is valid for externally measurable quantum work determined during the driving protocol. In contrast to the two-point measurement case, the theorem also applies to open quantum systems and the scenario can be realized without knowing the system Hamiltonian. Our fluctuation theorem comes in the form of an inequality and therefore only yields bounds to the true free energy difference. The inequality is saturated in the quasiclassical case of vanishing energy coherences at the beginning and at the end of the protocol. Thus, there is a clear quantum disadvantage.}, archive = {J_PRL}, author = {Konstantin Beyer and Walter T. Strunz}, doi = {10.1103/PhysRevLett.134.140403}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {140403}, shortjournal = {Phys. Rev. Lett.}, title = {Operational work fluctuation theorem for open quantum systems}, volume = {134}, year = {2025}, }
• (2025). Quantum trails and memory effects in the phase space of chaotic quantum systems. PRL, 134(14), 140402. (www)

  @article{ , abstract = {The eigenstates of a chaotic system can be enhanced along underlying unstable periodic orbits in so-called quantum scars, making it more likely for a particle launched along one such orbits to be found still there at long times. Unstable periodic orbits are, however, a negligible part of the phase space, and a question arises regarding the structure of the wave function elsewhere. Here, we address this question and show that a weakly dispersing dynamics of a localized wave packet in phase space leaves a “quantum trail” on the eigenstates, that is, makes them vary slowly when moving along trajectories in phase space, even if not periodic. The quantum trails underpin a remarkable dynamical effect: for a system initialized in a localized wave packet, the long-time phase-space distribution is enhanced along the short-time trajectory, which can result in ergodicity breaking. We provide the general intuition for these effects and prove them in the stadium billiard, for which an unwarping procedure allows us to visualize the phase space on the two-dimensional space of the page.}, archive = {J_PRL}, author = {Andrea Pizzi}, doi = {10.1103/PhysRevLett.134.140402}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {140402}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum trails and memory effects in the phase space of chaotic quantum systems}, volume = {134}, year = {2025}, }
• (2025). Universal stochastic equations of monitored quantum dynamics. PRL, 134(14), 140401. (www)

  @article{ , abstract = {We investigate the monitored quantum dynamics of Gaussian mixed states and derive the universal Fokker-Planck equations that govern the stochastic time evolution of entire density-matrix spectra, obtaining their exact solutions. From these equations, we reveal an even-odd effect in purification dynamics: whereas entropy exhibits exponential decay for an even number N of complex fermions, algebraic decay with divergent purification time occurs for odd N as a manifestation of dynamical criticality. Additionally, we identify the universal fluctuations of entropy in the chaotic regime, serving as a nonunitary counterpart of the universal conductance fluctuations in mesoscopic electronic transport phenomena. Furthermore, we elucidate and classify the universality classes of nonunitary quantum dynamics based on fundamental symmetry. We also validate the universality of these analytical results through extensive numerical simulations across different types of models.}, archive = {J_PRL}, author = {Zhenyu Xiao and Tomi Ohtsuki and Kohei Kawabata}, doi = {10.1103/PhysRevLett.134.140401}, journal = {Physical Review Letters}, month = {4}, number = {14}, pages = {140401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal stochastic equations of monitored quantum dynamics}, volume = {134}, year = {2025}, }
• (2025). Erratum: Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at sNN=27, 54.4, and 200 GeV at RHIC [Phys. rev. lett. 127, 262301 (2021)]. PRL, 134(13), 139903. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 139903 (2025)}, archive = {J_PRL}, author = {STAR Collaboration and M. S. Abdallah and J. Adam and L. Adamczyk and J. R. Adams and J. K. Adkins and G. Agakishiev and I. Aggarwal and M. M. Aggarwal and Z. Ahammed and I. Alekseev and D. M. Anderson and A. Aparin and E. C. Aschenauer and M. U. Ashraf and F. G. Atetalla and A. Attri and G. S. Averichev and V. Bairathi and W. Baker and J. G. Ball Cap and K. Barish and A. Behera and R. Bellwied and P. Bhagat and A. Bhasin and J. Bielcik and J. Bielcikova and I. G. Bordyuzhin and J. D. Brandenburg and A. V. Brandin and I. Bunzarov and J. Butterworth and X. Z. Cai and H. Caines and M. Calderón de la Barca Sánchez and D. Cebra and I. Chakaberia and P. Chaloupka and B. K. Chan and F-H. Chang and Z. Chang and N. Chankova-Bunzarova and A. Chatterjee and S. Chattopadhyay and D. Chen and J. Chen and J. H. Chen and X. Chen and Z. Chen and J. Cheng and M. Chevalier and S. Choudhury and W. Christie and X. Chu and H. J. Crawford and M. Csanád and M. Daugherity and T. G. Dedovich and I. M. Deppner and A. A. Derevschikov and A. Dhamija and L. Di Carlo and L. Didenko and X. Dong and J. L. Drachenberg and E. Duckworth and J. C. Dunlop and N. Elsey and J. Engelage and G. Eppley and S. Esumi and O. Evdokimov and A. Ewigleben and O. Eyser and R. Fatemi and F. M. Fawzi and S. Fazio and P. Federic and J. Fedorisin and C. J. Feng and Y. Feng and P. Filip and E. Finch and Y. Fisyak and A. Francisco and C. Fu and L. Fulek and C. A. Gagliardi and T. Galatyuk and F. Geurts and N. Ghimire and A. Gibson and K. Gopal and X. Gou and D. Grosnick and A. Gupta and W. Guryn and A. I. Hamad and A. Hamed and Y. Han and S. Harabasz and M. D. Harasty and J. W. Harris and H. Harrison and S. He and W. He and X. H. He and Y. He and S. Heppelmann and N. Herrmann and E. Hoffman and L. Holub and Y. Hu and H. Huang and H. Z. Huang and S. L. Huang and T. Huang and X. Huang and Y. Huang and T. J. Humanic and G. Igo and D. Isenhower and W. W. Jacobs and C. Jena and A. Jentsch and Y. Ji and J. Jia and K. Jiang and X. Ju and E. G. Judd and S. Kabana and M. L. Kabir and S. Kagamaster and D. Kalinkin and K. Kang and D. Kapukchyan and K. Kauder and H. W. Ke and D. Keane and A. Kechechyan and Y. V. Khyzhniak and D. P. Kikoła and C. Kim and B. Kimelman and D. Kincses and I. Kisel and A. Kiselev and A. G. Knospe and L. Kochenda and L. K. Kosarzewski and L. Kramarik and P. Kravtsov and L. Kumar and S. Kumar and R. Kunnawalkam Elayavalli and J. H. Kwasizur and R. Lacey and S. Lan and J. M. Landgraf and J. Lauret and A. Lebedev and R. Lednicky and J. H. Lee and Y. H. Leung and C. Li and W. Li and X. Li and Y. Li and X. Liang and Y. Liang and R. Licenik and T. Lin and Y. Lin and M. A. Lisa and F. Liu and H. Liu and P. Liu and T. Liu and X. Liu and Y. Liu and Z. Liu and T. Ljubicic and W. J. Llope and R. S. Longacre and E. Loyd and N. S. Lukow and X. Luo and L. Ma and R. Ma and Y. G. Ma and N. Magdy and R. Majka and D. Mallick and S. Margetis and C. Markert and H. S. Matis and J. A. Mazer and N. G. Minaev and S. Mioduszewski and B. Mohanty and M. M. Mondal and I. Mooney and D. A. Morozov and A. Mukherjee and M. Nagy and J. D. Nam and Md. Nasim and K. Nayak and D. Neff and J. M. Nelson and D. B. Nemes and M. Nie and G. Nigmatkulov and T. Niida and R. Nishitani and L. V. Nogach and T. Nonaka and A. S. Nunes and G. Odyniec and A. Ogawa and S. Oh and V. A. Okorokov and B. S. Page and R. Pak and A. Pandav and A. K. Pandey and Y. Panebratsev and P. Parfenov and B. Pawlik and D. Pawlowska and H. Pei and C. Perkins and L. Pinsky and R. L. Pintér and J. Pluta and B. R. Pokhrel and G. Ponimatkin and J. Porter and M. Posik and V. Prozorova and N. K. Pruthi and M. Przybycien and J. Putschke and H. Qiu and A. Quintero and C. Racz and S. K. Radhakrishnan and N. Raha and R. L. Ray and R. Reed and H. G. Ritter and M. Robotkova and O. V. Rogachevskiy and J. L. Romero and L. Ruan and J. Rusnak and N. R. Sahoo and H. Sako and S. Salur and J. Sandweiss and S. Sato and W. B. Schmidke and N. Schmitz and B. R. Schweid and F. Seck and J. Seger and M. Sergeeva and R. Seto and P. Seyboth and N. Shah and E. Shahaliev and P. V. Shanmuganathan and M. Shao and T. Shao and A. I. Sheikh and D. Shen and S. S. Shi and Y. Shi and Q. Y. Shou and E. P. Sichtermann and R. Sikora and M. Simko and J. Singh and S. Singha and M. J. Skoby and N. Smirnov and Y. Söhngen and W. Solyst and P. Sorensen and H. M. Spinka and B. Srivastava and T. D. S. Stanislaus and M. Stefaniak and D. J. Stewart and M. Strikhanov and B. Stringfellow and A. A. P. Suaide and M. Sumbera and B. Summa and X. M. Sun and X. Sun and Y. Sun and B. Surrow and D. N. Svirida and Z. W. Sweger and P. Szymanski and A. H. Tang and Z. Tang and A. Taranenko and T. Tarnowsky and J. H. Thomas and A. R. Timmins and D. Tlusty and T. Todoroki and M. Tokarev and C. A. Tomkiel and S. Trentalange and R. E. Tribble and P. Tribedy and S. K. Tripathy and T. Truhlar and B. A. Trzeciak and O. D. Tsai and Z. Tu and T. Ullrich and D. G. Underwood and I. Upsal and G. Van Buren and J. Vanek and A. N. Vasiliev and I. Vassiliev and V. Verkest and F. Videbæk and S. Vokal and S. A. Voloshin and F. Wang and G. Wang and J. S. Wang and P. Wang and Y. Wang and Z. Wang and J. C. Webb and P. C. Weidenkaff and L. Wen and G. D. Westfall and H. Wieman and S. W. Wissink and J. Wu and Y. Wu and B. Xi and Z. G. Xiao and G. Xie and W. Xie and H. Xu and N. Xu and Q. H. Xu and Y. Xu and Z. Xu and C. Yang and Q. Yang and S. Yang and Y. Yang and Z. Ye and L. Yi and K. Yip and Y. Yu and H. Zbroszczyk and W. Zha and C. Zhang and D. Zhang and J. Zhang and S. Zhang and X. P. Zhang and Y. Zhang and Z. J. Zhang and Z. Zhang and J. Zhao and C. Zhou and X. Zhu and Z. Zhu and M. Zurek and M. Zyzak}, doi = {10.1103/PhysRevLett.134.139903}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {139903}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at sNN=27, 54.4, and 200 GeV at RHIC [Phys. rev. lett. 127, 262301 (2021)]}, volume = {134}, year = {2025}, }
• (2025). Erratum: Beam energy dependence of fifth- and sixth-order net-proton number fluctuations in Au+Au collisions at RHIC [Phys. rev. lett. 130, 082301 (2023)]. PRL, 134(13), 139901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 139901 (2025)}, archive = {J_PRL}, author = {STAR Collaboration and B. E. Aboona and et al}, doi = {10.1103/PhysRevLett.134.139901}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {139901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Beam energy dependence of fifth- and sixth-order net-proton number fluctuations in Au+Au collisions at RHIC [Phys. rev. lett. 130, 082301 (2023)]}, volume = {134}, year = {2025}, }
• (2025). Numerical simulations reveal complementary function of blood-brain barrier and glymphatic transport in the brain. PRL, 134(13), 138403. (www)

  @article{ , abstract = {The brain accounts for approximately 20% of metabolism and, as a result, generates protein waste which requires efficient clearance. Failure to clear such waste leads to formation of toxic protein aggregates implicated in a variety of neurodegenerative diseases, including Alzheimer’s and Parkinson’s. The blood-brain barrier and the glymphatic system are two parallel transport pathways that remove waste from the brain, but very few studies have investigated their interactions or complementary function. Herein, we develop a Lattice Boltzmann simulation of waste clearance from an idealized segment of brain tissue and test the effects of selectively activating or deactivating each pathway. We model clearance of the peptide amyloid- , long recognized as critical in Alzheimer’s pathology, and calibrate our model against limited experimental data. This approach uncovers critical parameters that have eluded prior experimental measurement. Our study also reveals complementary functionality of the blood-brain barrier and glymphatic system that are likely generic features applicable to the transport of large molecules (e.g., proteins) in the brain.}, archive = {J_PRL}, author = {Reza Yousofvand and Jeffrey Tithof}, doi = {10.1103/PhysRevLett.134.138403}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {138403}, shortjournal = {Phys. Rev. Lett.}, title = {Numerical simulations reveal complementary function of blood-brain barrier and glymphatic transport in the brain}, volume = {134}, year = {2025}, }
• (2025). Epithelial layer fluidization by curvature-induced unjamming. PRL, 134(13), 138402. (www)

  @article{ , abstract = {The transition of an epithelial layer from a stationary, quiescent state to a highly migratory, dynamic state is required for wound healing, development, and regeneration. This transition, known as the unjamming transition (UJT), is responsible for epithelial fluidization and collective migration. Previous theoretical models have primarily focused on the UJT in flat epithelial layers, neglecting the effects of strong surface curvature characteristic of the epithelium in vivo . In this Letter, we investigate the role of surface curvature on tissue plasticity and cellular migration using a vertex model embedded on a spherical surface. Our findings reveal that increasing curvature promotes the UJT by reducing the energy barriers to cellular rearrangements. Higher curvature favors cell intercalation, mobility, and self-diffusivity, resulting in epithelial structures that are malleable and migratory when small, but become more rigid and stationary as they grow. Together, these results provide a conceptual framework to better understand how cell shape, cell propulsion, and tissue geometry contribute to tissue malleability, remodeling, and stabilization.}, archive = {J_PRL}, author = {Margherita De Marzio and Amit Das and Jeffrey J. Fredberg and Dapeng Bi}, doi = {10.1103/PhysRevLett.134.138402}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {138402}, shortjournal = {Phys. Rev. Lett.}, title = {Epithelial layer fluidization by curvature-induced unjamming}, volume = {134}, year = {2025}, }
• (2025). Active fluids form system-spanning filamentary networks. PRL, 134(13), 138301. (www)

  @article{ , abstract = {Recent experimental realizations of liquid-liquid phase separation of active liquid crystals have offered an insight into the interaction between phase separation, ubiquitous in soft matter and biology, and chaotic active flows. In this Letter, we use continuum theory to examine phase separation of an active liquid crystal and a passive fluid and report two new results. First, we provide an analytical derivation of the activity-induced suppression of the phase boundary of the coexistence region—a result first reported in simulations and experiments. We show that the shift in the critical point is a result of the balance between self-stirring active flows and phase-separating diffusive fluxes. Second, we show that this same balance is responsible for dramatically changing the morphology of the phase separated state, resulting in the emergence of a new mixed active phase consisting of a dynamical filamentous active network that invades the entire system area, trapping droplets of passive material. This structure exists even for very low volume fractions of active material. Our work provides an important step towards the goal of understanding how to use activity as a new handle for sculpting interfaces.}, archive = {J_PRL}, author = {Paarth Gulati and Fernando Caballero and M. Cristina Marchetti}, doi = {10.1103/PhysRevLett.134.138301}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {138301}, shortjournal = {Phys. Rev. Lett.}, title = {Active fluids form system-spanning filamentary networks}, volume = {134}, year = {2025}, }
• (2025). High reconstructability of degree-heterogeneous networks. PRL, 134(13), 137402. (www)

  @article{ , abstract = {Reconstructing complex networks from observed, often noisy data is a fundamental task crucial for understanding complex systems across various domains. Despite numerous methods proposed for network reconstruction, little attention has been given to the relationship between reconstructability and the intrinsic properties of hidden networks. Here, we present a mathematical proof that, for scale-free networks, the reconstruction accuracy increases as the exponent of the power-law degree distribution decreases. This suggests that degree heterogeneity contributes to higher reconstructability. We validate this conclusion in empirical networks, where nodal degrees may not strictly adhere to power laws. Our results demonstrate that the reconstruction accuracy of degree-heterogeneous networks is indeed significantly higher than that of their randomized counterparts.}, archive = {J_PRL}, author = {Jia-Jie Qin and Gang Yan}, doi = {10.1103/PhysRevLett.134.137402}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {137402}, shortjournal = {Phys. Rev. Lett.}, title = {High reconstructability of degree-heterogeneous networks}, volume = {134}, year = {2025}, }
• (2025). Electromagnetic raman enhancement beyond gap limit. PRL, 134(13), 136902. (www)

  @article{ , abstract = {Surface-enhanced Raman scattering is of great importance to trace-level detection with fingerprint information of analytes. However, there is no room for electric dipole enhancement mechanism to further improve the enhancement factor and detect macromolecules. Here, we break the limits by electric multipoles with anapole states, as well as bound states in the continuum, providing a degree of freedom to control field confinement in time and in space. The increases of gap size will benefit to both improve enhancement factor in the order of 1 0 1 2 and take in large molecules over 100 nm. Our findings open a pathway towards promoting practical applications of surface-enhanced Raman scattering by virtue of the excitation of high-order electromagnetic multipoles in arrayed structures, and harnessing other light-matter interaction processes, such as light emission, photodetection, photocatalysis, nonlinear optics, and quantum optics.}, archive = {J_PRL}, author = {Qi-hang Zhang and Kai Liu and Kang Qin and Shao-jie Fu and Jun Du and Yan-qing Lu and Yong-yuan Zhu and Yan-feng Chen and Xue-jin Zhang}, doi = {10.1103/PhysRevLett.134.136902}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136902}, shortjournal = {Phys. Rev. Lett.}, title = {Electromagnetic raman enhancement beyond gap limit}, volume = {134}, year = {2025}, }
• (2025). Bound states to bands in the continuum in cylindrical granular crystals. PRL, 134(13), 136901. (www)

  @article{ , abstract = {We theoretically investigate and experimentally demonstrate that genuine bound states in the continuum (BICs)—polarization-protected BICs—can be completely localized within compact solid resonators. This bound mode is realized in a highly tunable mechanical system made of cylindrical granular crystals, where tuning the contact boundaries enables the in situ transition from the BICs to quasi-BICs in a controllable manner. Since a single-particle resonator can itself support BICs, these bound states can extend to form bound bands within periodic structures composed of such resonators. We experimentally demonstrate the emergence of a quasibound (flat) band in a finite chain with broken resonator symmetry, using a laser Doppler vibrometer. Remarkably, we show that all cylindrical resonators within the entire chain exhibit high- and dispersionless resonance.}, archive = {J_PRL}, author = {Yeongtae Jang and Seokwoo Kim and Dongwoo Lee and Eunho Kim and Junsuk Rho}, doi = {10.1103/PhysRevLett.134.136901}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136901}, shortjournal = {Phys. Rev. Lett.}, title = {Bound states to bands in the continuum in cylindrical granular crystals}, volume = {134}, year = {2025}, }
• (2025). Domain wall reactions in multiple-order parameter ferroelectrics. PRL, 134(13), 136802. (www)

  @article{ , abstract = {The motion of domain walls is crucial for ferroelectric switching. Conventionally, the switching dynamics is believed to be determined by the motion of one or a few low-energy domain wall types of dominant population. Here, we challenge this conventional idea in multiple-order-parameter ferroelectrics. Using hafnia as example, we show that the multiple-order-parameter nature not only provides various mobile domain walls and defectlike immobile domain walls, but also enables the domain wall reactions. In analogy with chemical reactions where substances react to form new substances, domain walls could also react to form other domain walls during switching. We identify several elementary domain wall reaction types including synthesis, decomposition, and exchange reactions. Domain walls are continually changed by these reactions during switching so that the switching behavior reflects the statistical average of many domain wall types with distinct mobility and stability. These reactions also lead to phenomenon like remanent nuclei and defect-site nucleation that facilitate switching and lower coercive field. Finally, the concept of domain wall reaction is not limited to hafnia but can be generalized to any multiple-order-parameter ferroelectric. This Letter conceptualizes domain wall reaction, expands the theory of ferroelectric switching, and suggests a practical way for defect engineering to control switching behavior.}, archive = {J_PRL}, author = {Songsong Zhou and Shihan Qin and Andrew M. Rappe}, doi = {10.1103/PhysRevLett.134.136802}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136802}, shortjournal = {Phys. Rev. Lett.}, title = {Domain wall reactions in multiple-order parameter ferroelectrics}, volume = {134}, year = {2025}, }
• (2025). Prediction of room temperature electric field reversal of magnetization in the family of A4B3O9 layered oxides. PRL, 134(13), 136801. (www)

  @article{ , abstract = {The promise of a strong magnetoelectric coupling in a multiferroic material is not only of fundamental interest, but also forms the basis of next generation memory devices where the direction of magnetization can be reversed by an external electric field. Using group-theory led first-principles calculations, we have identified a hitherto unknown polar phase of the A 4 B 3 O 9 layered oxides, where the polar mode couples to the magnetic modes through a rare Γ -point magnetoelectric-multiferroic coupling scheme such that the net magnetization can be directly reversed by an electric field switching of the polar mode. Furthermore, in agreement with previous experimental observations, we predict room temperature magnetism in A 4 B 3 O 9 oxides that indicates the promising practical applications of these compounds in the next generation memory devices.}, archive = {J_PRL}, author = {Urmimala Dey and Emma E. McCabe and Jorge Íñiguez-González and Nicholas C. Bristowe}, doi = {10.1103/PhysRevLett.134.136801}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136801}, shortjournal = {Phys. Rev. Lett.}, title = {Prediction of room temperature electric field reversal of magnetization in the family of A4B3O9 layered oxides}, volume = {134}, year = {2025}, }
• (2025). Topological defect mediated helical phase reorientation by uniaxial stress. PRL, 134(13), 136704. (www)

  @article{ , abstract = {Strain engineering enables precise, energy-efficient control of nanoscale magnetism. However, unlike well-studied strain-dislocation interactions in mechanical deformation, the spatial evolution of strain-induced spin rearrangement remains poorly understood. Using in situ Lorentz transmission electron microscopy, we manipulate and observe helical domain reorientation under quantitatively applied uniaxial tensile stress. Our findings reveal striking similarity to plastic deformation in metals, where the critical stress for propagation vector ( ) reorientation depends on its angle with the stress direction. Magnetic defects mediate reorientation via “break-and-reconnect” or “dislocation gliding–annihilation” processes. Simulations confirm that strain-induced anisotropic Dzyaloshinskii-Moriya interaction may play a key role. These insights advance strain-driven magnetism and offer a promising route for energy-efficient magnetic nanophase control in next-generation information technology.}, archive = {J_PRL}, author = {Tae-Hoon Kim and Haijun Zhao and Brandt A. Jensen and Liqin Ke and Lin Zhou}, doi = {10.1103/PhysRevLett.134.136704}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136704}, shortjournal = {Phys. Rev. Lett.}, title = {Topological defect mediated helical phase reorientation by uniaxial stress}, volume = {134}, year = {2025}, }
• (2025). Zeeman split kramers doublets in spin-supersolid candidate Na2BaCo(PO4)2. PRL, 134(13), 136703. (www)

  @article{ , abstract = {Na 2 BaCo ( PO 4 ) 2 is a triangular antiferromagnet that displays highly efficient adiabatic demagnetization cooling [Junsen Xiang et al. , Nature (London) 625 , 270 (2024) ] near a quantum critical point at μ 0 H c ∼ 1.6 T , separating a low-field magnetically disordered from a high-field fully polarized ferromagnetic phase. We apply high resolution backscattering neutron spectroscopy in an applied field to study the magnetic excitations near μ 0 H c . At large fields we observe ferromagnetic fluctuations that gradually transition to being overdamped in energy below μ 0 H c where the magnetism is spatially disordered. We parametrize the excitations in the high-field polarized phase in terms of coupled Zeeman split Kramers doublets originating from the presence of spin-orbit coupling. On reducing the field, the splitting between the Kramers doublets is reduced and if done adiabatically, provides a mechanism for reducing temperature. On lowering the applied field through the μ 0 H c the excitations characterize a textured phase that we suggest is inefficient for cooling. Low temperature disordered frustrated magnets built on Kramers doublets with nearby quantum critical points provide a route for efficient magnetocalorics.}, archive = {J_PRL}, author = {T. I. Popescu and N. Gora and F. Demmel and Z. Xu and R. Zhong and T. J. Williams and R. J. Cava and G. Xu and C. Stock}, doi = {10.1103/PhysRevLett.134.136703}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136703}, shortjournal = {Phys. Rev. Lett.}, title = {Zeeman split kramers doublets in spin-supersolid candidate Na2BaCo(PO4)2}, volume = {134}, year = {2025}, }
• (2025). Impact of planar defects on the reversal time of single magnetic domain nanoparticles. PRL, 134(13), 136702. (www)

  @article{ , abstract = {Recent experimental investigations of individual magnetic nanoparticles reveal a diverse range of magnetic relaxation times which cannot be explained by considering their size, shape, and surface anisotropy, suggesting other factors associated with the internal microstructure of the particles are at play. In this Letter, we apply Langer’s theory of thermal activation to fcc Co nanoparticles exhibiting single domain magnetism, whose experimentally observed microstructure contain planar defects. Our analytical derivation yields an expression for the activation rate as a function of the particle size and the defect fraction, enabling a quantitative understanding of the experimental findings. These dependencies, which are exponential for both the Arrhenius exponential and its prefactor, demonstrate the critical role that structural defects can play in the magnetic stability of nanoparticles.}, archive = {J_PRL}, author = {Hugo Bocquet and Armin Kleibert and Peter M. Derlet}, doi = {10.1103/PhysRevLett.134.136702}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136702}, shortjournal = {Phys. Rev. Lett.}, title = {Impact of planar defects on the reversal time of single magnetic domain nanoparticles}, volume = {134}, year = {2025}, }
• (2025). Direct measurement of topological invariants through temporal adiabatic evolution of bulk states in the synthetic brillouin zone. PRL, 134(13), 136601. (www)

  @article{ , abstract = {Mathematically, topological invariants arise from the parallel transport of eigenstates on the energy bands, which, in physics, correspond to the adiabatic dynamical evolution of transient states. It determines the presence of boundary states, while lacking direct measurements. Here, we develop time-varying programmable coupling circuits between acoustic cavities to mimic the Hamiltonians in the Brillouin zone, with which excitation and adiabatic evolution of bulk states are realized in a unit cell. By extracting the Berry phases of the bulk band, topological invariants, including the Zak phase for the SSH model and the Chern number for the AAH model, are obtained convincingly. The bulk state evolution also provides insight into the topological charges of the newly developed non-Abelian models, which are also verified by observing the adiabatic eigenframe rotation. Our Letter not only provides a general recipe for telling various topological invariants but also sheds light on transient acoustic wave manipulations.}, archive = {J_PRL}, author = {Zhao-Xian Chen and Yuan-Hong Zhang and Xiao-Chen Sun and Ruo-Yang Zhang and Jiang-Shan Tang and Xin Yang and Xue-Feng Zhu and Yan-Qing Lu}, doi = {10.1103/PhysRevLett.134.136601}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136601}, shortjournal = {Phys. Rev. Lett.}, title = {Direct measurement of topological invariants through temporal adiabatic evolution of bulk states in the synthetic brillouin zone}, volume = {134}, year = {2025}, }
• (2025). Fractionalized kohn-sham scheme for strongly correlated electrons. PRL, 134(13), 136505. (www)

  @article{ , abstract = {We propose to expand the territory of density functional theory to strongly correlated electrons by reformulating the Kohn-Sham scheme in the representation of fractionalized particles. We call it the “ KS * scheme.” Using inhomogeneous t − J chains as a test bed, we show that the KS * scheme with simple local density approximation is able to achieve accurate ground-state energy and density distribution comparable to the density matrix renormalization group method, while the computational complexity is much lower.}, archive = {J_PRL}, author = {Bo Zhao and Jing-Yu Zhao and Zheng Zhu and Jian Wu and Zheng Liu}, doi = {10.1103/PhysRevLett.134.136505}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136505}, shortjournal = {Phys. Rev. Lett.}, title = {Fractionalized kohn-sham scheme for strongly correlated electrons}, volume = {134}, year = {2025}, }
• (2025). Anomalous acoustocurrent within quantum hall plateaus. PRL, 134(13), 136504. (www)

  @article{ , abstract = {We systematically study the acoustocurrent of two-dimensional electron systems in the integer and fractional quantum Hall regimes using surface acoustic waves. We are able to separate the coexisting acoustic scattering and drag, when phonons induce a drag current and tune the electron conductivity, respectively. At large acoustic power, the drag current is finite when the system is compressible and exhibits minima when incompressible quantum Hall states appear. Surprisingly, it exhibits anomalously large bipolar spikes within the quantum Hall plateaus while it vanishes linearly with reduced acoustic power at compressible phases. The current peaks reverse their polarity at the two flanks of exact integer or fractional fillings, consistent with the opposite electric charge of the quasiparticle and quasihole.}, archive = {J_PRL}, author = {Renfei Wang and Xiao Liu and Mengmeng Wu and Yoon Jang Chung and Adbhut Gupta and Kirk W. Baldwin and Mansour Shayegan and Loren Pfeiffer and Xi Lin and Yang Liu}, doi = {10.1103/PhysRevLett.134.136504}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136504}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous acoustocurrent within quantum hall plateaus}, volume = {134}, year = {2025}, }
• (2025). Coulomb drag in altermagnets. PRL, 134(13), 136301. (www)

  @article{ , abstract = {An altermagnet is a newly discovered antiferromagnet, characterized by unique anisotropic spin-split energy bands. It has attracted tremendous interest because of its promising potential in information storage and processing. However, measuring the distinctive spin-split energy bands arising from altermagnetism remains a challenge. Here, we propose to employ the Coulomb drag to probe altermagnetism. In the Coulomb drag, an electric current in an active layer of electron gases can induce currents in a close but well-isolated passive layer, due to interlayer Coulomb interactions. We find that the Coulomb drag effects in altermagnets are highly sensitive to the orientation of the spin-split Fermi surfaces. As a result, transverse currents can be dragged in the passive layer, leading to Hall drag effects even in the absence of spin-orbit coupling, a feature quite different from all previous systems. More importantly, all the drag effects of altermagnets have unique angle dependence, which can be measured in a multiterminal setup to serve as signatures for altermagnetism. This proposal will inspire increasing explorations on emergent magnetism.}, archive = {J_PRL}, author = {Hao-Jie Lin and Song-Bo Zhang and Hai-Zhou Lu and X. C. Xie}, doi = {10.1103/PhysRevLett.134.136301}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136301}, shortjournal = {Phys. Rev. Lett.}, title = {Coulomb drag in altermagnets}, volume = {134}, year = {2025}, }
• (2025). Extrinsic orbital hall effect: Orbital skew scattering and crossover between diffusive and intrinsic orbital transport. PRL, 134(13), 136201. (www)

  @article{ , abstract = {Despite the recent success of identifying experimental signatures of the orbital Hall effect (OHE), the research on the microscopic mechanisms behind this unique phenomenon is still in its infancy. Here, using a gapped 2D Dirac material as a model system of the OHE, we develop a microscopic theory of orbital transport which captures extrinsic disorder effects nonperturbatively. We show that it predicts several hitherto unknown effects, including (i) a strong dependence of the orbital Hall conductivity with the strength and symmetry of the impurity scattering potential, and (ii) a smooth crossover from intrinsic to extrinsic OHE as a function of the Fermi energy and impurity density. In contrast to previous (perturbative) studies, the OHE is found to exhibit bona fide diffusive behavior in the dilute impurity limit, which we trace back to the dominance of skew scattering–type processes. More generally, we argue that the newly unveiled orbital skew scattering mechanism governs the diffusive OHEs of a large class of 2D materials even when the crystal structure is inversion symmetric. Our work unveils the crucial nature of nonperturbative vertex corrections for a complete description of orbital transport and confirms common short-range impurities as key enablers of the OHE.}, archive = {J_PRL}, author = {Alessandro Veneri and Tatiana G. Rappoport and Aires Ferreira}, doi = {10.1103/PhysRevLett.134.136201}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136201}, shortjournal = {Phys. Rev. Lett.}, title = {Extrinsic orbital hall effect: Orbital skew scattering and crossover between diffusive and intrinsic orbital transport}, volume = {134}, year = {2025}, }
• (2025). Melting, bubblelike expansion, and explosion of superheated plasmonic nanoparticles. PRL, 134(13), 136101. (www)

  @article{ , abstract = {We report on time-resolved coherent diffraction imaging of gas-phase silver nanoparticles, strongly heated via their plasmon resonance. The x-ray diffraction images reveal a broad range of phenomena for different excitation strengths, from simple melting over strong cavitation to explosive disintegration. Molecular dynamics simulations fully reproduce this behavior and show that the heating induces rather similar trajectories through the phase diagram in all cases, with the very different outcomes resulting solely from whether and where the stability limit of the metastable superheated liquid is crossed.}, archive = {J_PRL}, author = {Simon Dold and Thomas Reichenbach and Alessandro Colombo and Jakob Jordan and Ingo Barke and Patrick Behrens and Nils Bernhardt and Jonathan Correa and Stefan Düsterer and Benjamin Erk and Thomas Fennel and Linos Hecht and Andrea Heilrath and Robert Irsig and Norman Iwe and Patrice Kolb and Björn Kruse and Bruno Langbehn and Bastian Manschwetus and Philipp Marienhagen and Franklin Martinez and Karl-Heinz Meiwes-Broer and Kevin Oldenburg and Christopher Passow and Christian Peltz and Mario Sauppe and Fabian Seel and Rico Mayro P. Tanyag and Rolf Treusch and Anatoli Ulmer and Saida Walz and Michael Moseler and Thomas Möller and Daniela Rupp and Bernd von Issendorff}, doi = {10.1103/PhysRevLett.134.136101}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136101}, shortjournal = {Phys. Rev. Lett.}, title = {Melting, bubblelike expansion, and explosion of superheated plasmonic nanoparticles}, volume = {134}, year = {2025}, }
• (2025). Low-energy excitations in bosonic quantum quasicrystals. PRL, 134(13), 136003. (www)

  @article{ , abstract = {We present the first principles construction of the low energy effective action for bosonic self-organized quantum quasicrystals. Our generalized elasticity approach retains the appropriate number of phase and corresponding conjugate density degrees of freedom required for a proper description of the gapless modes. For the dodecagonal and decagonal quasicrystal structures we obtain collective longitudinal and transverse excitations with an isotropic speed of sound. Meanwhile, for the octagonal structure, the coupling between phononic and phasonic degrees of freedom leads in turn to hybridization of the latter with the condensate sound mode, producing collective excitations with a longitudinal and transverse component and an anisotropic speed of sound. Finally, we discuss the fate of each excitation mode at the low and high density phase transitions limiting the quantum quasicrystal phase.}, archive = {J_PRL}, author = {A. Mendoza-Coto and M. Bonifacio and F. Piazza}, doi = {10.1103/PhysRevLett.134.136003}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {136003}, shortjournal = {Phys. Rev. Lett.}, title = {Low-energy excitations in bosonic quantum quasicrystals}, volume = {134}, year = {2025}, }
• (2025). Kinetic structure of strong-field QED showers in crossed electromagnetic fields. PRL, 134(13), 135001. (www)

  @article{ , abstract = {A complete, kinetic description of electron-seeded strong-field QED showers in crossed electromagnetic fields is derived. The kinetic structure of the shower and its temporal evolution are shown to be a function of two parameters: the initial shower quantum parameter and radiation time. The latter determines the short and long time evolution of the shower. Explicit solutions for the shower multiplicity (number of pairs per seed electron) and the emitted photon spectrum are obtained for both timescales. Our approach is first derived considering showers in a constant, homogeneous magnetic field. We find that our results are valid for any crossed fields and we apply them to laboratory settings for which we obtain fully analytical, predictive scaling laws.}, archive = {J_PRL}, author = {M. Pouyez and T. Grismayer and M. Grech and C. Riconda}, doi = {10.1103/PhysRevLett.134.135001}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {135001}, shortjournal = {Phys. Rev. Lett.}, title = {Kinetic structure of strong-field QED showers in crossed electromagnetic fields}, volume = {134}, year = {2025}, }
• (2025). Shear and bulk viscosities of water up to 1.6 GPa and anomaly in the structural relaxation time. PRL, 134(13), 134101. (www)

  @article{ , abstract = {Deep in Earth’s crust, pressure exceeds 1000 times the atmospheric pressure. Water still flows under these conditions, but experiences dramatic changes in structure and fluidity. Using combined dynamic and inelastic light scattering techniques, we simultaneously measure the shear and bulk viscosities of water as a function of pressure. The former increases faster than the latter, so that their ratio shows a twofold decrease from 0 to 1.6 GPa; we confirm this trend with simulations. We analyze our results in terms of the structural relaxation time . Contrary to other liquids, pressure initially accelerates relaxation in water. Our measurements reveal that reaches a minimum close to 1 ps around 0.5 GPa. We interpret as the equilibration time of hydrogen bonds and propose that the minimum in arises from a structural anomaly that allows fastest interconversion between local structures in water and generates a cascade of thermodynamic and dynamic anomalies.}, archive = {J_PRL}, author = {Jan Eichler and Johannes Stefanski and José Martin Roca and Isabelle Daniel and Bruno Issenmann and Chantal Valeriani and Frédéric Caupin}, doi = {10.1103/PhysRevLett.134.134101}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {134101}, shortjournal = {Phys. Rev. Lett.}, title = {Shear and bulk viscosities of water up to 1.6 GPa and anomaly in the structural relaxation time}, volume = {134}, year = {2025}, }
• (2025). Universal scaling laws for a generic swimmer model. PRL, 134(13), 134002. (www)

  @article{ , abstract = {We introduce a minimal model of a swimmer without body deformation based on force and torque dipoles which allows accurate and efficient 3D Navier-Stokes calculations. Our model can reproduce swimmer propulsion for a large range of Reynolds numbers and generate wake vortices in the inertial regime, reminiscent of the flow generated by the flapping tail of real fish. We perform a numerical exploration of the model from low to high Reynolds numbers and obtain universal laws using scaling arguments. Collecting data from a wide variety of microswimmers, we show that our theoretical scaling laws compare very well with experimental swimming performances across the different hydrodynamic regimes, from Stokes to turbulent flows. The simple design of our generic swimmer model paves the way for efficient large-scale simulations of hundreds of individuals, crucial for understanding collective effects within assemblies of aquatic animals.}, archive = {J_PRL}, author = {Bruno Ventéjou and Thibaut Métivet and Aurélie Dupont and Philippe Peyla}, doi = {10.1103/PhysRevLett.134.134002}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {134002}, shortjournal = {Phys. Rev. Lett.}, title = {Universal scaling laws for a generic swimmer model}, volume = {134}, year = {2025}, }
• (2025). Why charged drops do not splash. PRL, 134(13), 134001. (www)

  @article{ , abstract = {The dynamics of charged drops, especially in the context of drop splashing, remains largely uncharted despite its prevalence in both natural phenomena and technological applications. Our research uncovers the ability of charged drops to suppress splashing effectively. The electric charges surrounding drops exert a force that pulls the ejecting lamella toward the substrate, resulting in a thinner lubrication air film at the solid-liquid interface. We further develop a theoretical framework to relate splash threshold velocity with drop charges and surface dielectric constant. Our results extend the scope of drop-splashing studies beyond the assumption of electric neutrality and highlight the potential of controlling splashing by manipulating drop charges.}, archive = {J_PRL}, author = {Fanfei Yu and Aaron D. Ratschow and Ran Tao and Xiaomei Li and Yuankai Jin and Jinpei Wang and Zuankai Wang}, doi = {10.1103/PhysRevLett.134.134001}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {134001}, shortjournal = {Phys. Rev. Lett.}, title = {Why charged drops do not splash}, volume = {134}, year = {2025}, }
• (2025). Inherent spin-orbit locking in topological lasing via bound state in the continuum. PRL, 134(13), 133802. (www)

  @article{ , abstract = {Bound states in the continuum (BICs) are exotic optical topological singularities that defy the typical radiation within the continuum of radiative modes and carry topological polarization vortices in momentum space. Enabling ultrahigh quality factors, BICs have been applied in realizing lasing and Bose-Einstein condensation, and their momentum-space vortex topologies have been exploited in passive systems, revealing novel spin-orbit photonic effects. Here, we demonstrate the inherent spin-orbit locking in topological BIC lasing. Utilizing C 4 v and C 6 v photonic crystal slabs, we achieve distinct spin-orbit locking combinations in BIC lasing of + 1 and − 2 topological charges. Spin-orbit locking phenomena are directly observed by momentum-space spin-dependent self-interference patterns. Real-space spin separations, as a counterpart of the momentum-space spin-orbit locking, are also revealed. Our results reveal new spin-orbit locking phenomena in BIC lasing, presenting significant potential for advancements in topological photonic source applications.}, archive = {J_PRL}, author = {Jiajun Wang and Xinhao Wang and Zhaochen Wu and Xingqi Zhao and Shunben Wu and Lei Shi and Yuri Kivshar and Jian Zi}, doi = {10.1103/PhysRevLett.134.133802}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {133802}, shortjournal = {Phys. Rev. Lett.}, title = {Inherent spin-orbit locking in topological lasing via bound state in the continuum}, volume = {134}, year = {2025}, }
• (2025). Noise constraints for nonlinear exceptional point sensing. PRL, 134(13), 133801. (www)

  @article{ , abstract = {Exceptional points (EPs) are singularities in the parameter space of a non-Hermitian system where eigenenergies and eigenstates coincide. They hold promise for enhancing sensing applications, but this is limited by the divergence of shot noise near EPs. According to recent studies, EP sensors operating in the nonlinear regime may avoid these limitations. By analyzing an exemplary nonlinear system, we show that the interplay of noise and nonlinearity introduces previously unidentified obstacles to enhanced sensing. The noise effectively displaces the EP in parameter space and reduces its order, thereby eliminating the sought-for divergence in the signal-to-noise ratio. Moreover, the noise near the nonlinear EP experiences a stronger divergence than predicted by standard calculations of the Petermann noise factor, due to the properties of the Bogoliubov–de Gennes Hamiltonian governing the fluctuations. Our semianalytical estimates for the noise level agree quantitatively with the results of stochastic numerical simulations.}, archive = {J_PRL}, author = {Xu Zheng and Y. D. Chong}, doi = {10.1103/PhysRevLett.134.133801}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {133801}, shortjournal = {Phys. Rev. Lett.}, title = {Noise constraints for nonlinear exceptional point sensing}, volume = {134}, year = {2025}, }
• (2025). Quantum-enhanced weak absorption estimation with correlated photons. PRL, 134(13), 133604. (www)

  @article{ , abstract = {Conventional absorption spectroscopy relies on coherent laser sources, and in turn suffers from the inherent limitation of shot noise, especially in estimating weak absorption. Here, we propose a measurement strategy with correlated photons to determine the weak absorption by distinguishing the output with and without photons, dubbed as the on-off measurement. We demonstrate that absorption spectroscopy that incorporates quantum correlations is capable of estimating weak absorption down to a single-photon level, even in noisy environments, achieving a precision comparable to that obtained through 1000 photons in conventional absorption spectroscopy. Our strategy provides a new method to probe fragile systems with weak absorption, avoiding the occurrence of light-induced damage.}, archive = {J_PRL}, author = {Zhucheng Zhang and Xue Zhang and Jing Liu and Hui Dong}, doi = {10.1103/PhysRevLett.134.133604}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {133604}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum-enhanced weak absorption estimation with correlated photons}, volume = {134}, year = {2025}, }
• (2025). Bright and dark states of light: The quantum origin of classical interference. PRL, 134(13), 133603. (www)

  @article{ , abstract = {Classical theory asserts that several electromagnetic waves cannot interact with matter if they interfere destructively to zero, whereas quantum mechanics predicts a nontrivial light-matter dynamics even when the average electric field vanishes. Here, we show that in quantum optics, classical interference emerges from collective bright and dark states of light, i.e., particular cases of two-mode binomial states, which are entangled superpositions of multimode photon-number states. This makes it possible to explain wave interference using the particle description of light and the superposition principle for linear systems only. It also sheds new light on an old debate concerning the origin of complementarity.}, archive = {J_PRL}, author = {Celso J. Villas-Boas and Carlos E. Máximo and Paulo J. Paulino and Romain P. Bachelard and Gerhard Rempe}, doi = {10.1103/PhysRevLett.134.133603}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {133603}, shortjournal = {Phys. Rev. Lett.}, title = {Bright and dark states of light: The quantum origin of classical interference}, volume = {134}, year = {2025}, }
• (2025). Individual assembly of two-species rydberg molecules using optical tweezers. PRL, 134(13), 133401. (www)

  @article{ , abstract = {We present a new approach to investigating Rydberg molecules by demonstrating the formation and characterization of individual Rb * Cs Rydberg molecules using optical tweezers. By employing single-atom detection of Rb and Cs, we observe molecule formation via correlated loss of both species and study the formation dynamics with single-particle resolution. We control the interatomic distances by manipulating the relative wave function of atom pairs using the tweezer intensity, optimizing the coupling to molecular states and exploring the effect of the tweezer on these states. Additionally, we demonstrate molecule association with atoms trapped in separate tweezers, paving the way for state-selective assembly of polyatomic molecules. The observed binding energies, molecular alignment, and bond lengths are in good agreement with theory. Our approach is broadly applicable to Rydberg tweezer platforms, expanding the range of available molecular systems and enabling the integration of Rydberg molecules into existing quantum science platforms.}, archive = {J_PRL}, author = {Alexander Guttridge and Tom R. Hepworth and Daniel K. Ruttley and Aileen A. T. Durst and Matthew T. Eiles and Simon L. Cornish}, doi = {10.1103/PhysRevLett.134.133401}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {133401}, shortjournal = {Phys. Rev. Lett.}, title = {Individual assembly of two-species rydberg molecules using optical tweezers}, volume = {134}, year = {2025}, }
• (2025). Evidence for two excited Ω− hyperons. PRL, 134(13), 131903. (www)

  @article{ , abstract = {Using e + e − collision data corresponding to an integrated luminosity of 19 fb − 1 collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70 GeV, we report the first evidence for a new excited Ω − hyperon, the Ω ( 2109 ) − , through the process e + e − → Ω ( 2109 ) − Ω ¯ + + c . c . with a significance of 4.1 σ . The mass and width of Ω ( 2109 ) − are measured to be 2108.5 ± 5.2 stat ± 0.9 syst MeV / c 2 and 18.3 ± 16.4 stat ± 5.7 syst MeV , respectively. We also present evidence for a new production mechanism for the previously identified Ω ( 2012 ) − via the process e + e − → Ω ( 2012 ) − Ω ¯ + + c . c . with a significance of 3.5 σ .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and X. Y. Chai and J. F. Chang and G. R. Che and Y. Z. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and Q. P. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and L. Lavezzi and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and K. L. Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and T. Y. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and C. X. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. M. Ma and F. E. Maas and I. MacKay and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Y. H. Meng and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and M. Q. Ruan and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. H. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and H. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and J. H. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. X. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and Z. Z. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.131903}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {131903}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence for two excited Ω− hyperons}, volume = {134}, year = {2025}, }
• (2025). Search for fractionally charged particles in proton-proton collisions at s=13 TeV. PRL, 134(13), 131802. (www)

  @article{ , abstract = {A search is presented for fractionally charged particles with charges below , using their small energy loss in the tracking detector as a key variable to observe a signal. The analyzed dataset corresponds to an integrated luminosity of of proton-proton collisions collected at in 2016–2018 at the CERN LHC. This is the first search at the LHC for new particles with a charge between and , including an extension of previous results at a charge of . Masses up to 640 GeV and charges as low as are excluded at 95% confidence level. These are the most stringent limits to date for the considered Drell-Yan-like production mode.}, archive = {J_PRL}, author = {CMS Collaboration and A. Hayrapetyan and A. Tumasyan and W. Adam and J. W. Andrejkovic and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and A. Escalante Del Valle and P. S. Hussain and M. Jeitler and N. Krammer and L. Lechner and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and S. Templ and W. Waltenberger and C.-E. Wulz and M. R. Darwish and T. Janssen and P. Van Mechelen and E. S. Bols and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and H. El Faham and S. Lowette and I. Makarenko and A. Morton and D. Müller and A. R. Sahasransu and S. Tavernier and M. Tytgat and S. Van Putte and D. Vannerom and B. Clerbaux and G. De Lentdecker and L. Favart and D. Hohov and J. Jaramillo and A. Khalilzadeh and K. Lee and M. Mahdavikhorrami and A. Malara and S. Paredes and L. Pétré and N. Postiau and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and J. Knolle and L. Lambrecht and G. Mestdach and C. Rendón and A. Samalan and K. Skovpen and N. Van Den Bossche and B. Vermassen and L. Wezenbeek and A. Benecke and G. Bruno and C. Caputo and C. Delaere and I. S. Donertas and A. Giammanco and K. Jaffel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and K. Mondal and T. T. Tran and S. Wertz and G. A. Alves and E. Coelho and C. Hensel and T. Menezes De Oliveira and A. Moraes and P. Rebello Teles and M. Soeiro and W. L. Aldá Júnior and M. Alves Gallo Pereira and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and J. Martins and C. Mora Herrera and K. Mota Amarilo and L. Mundim and H. Nogima and A. Santoro and S. M. Silva Do Amaral and A. Sznajder and M. Thiel and A. Vilela Pereira and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and T. Ivanov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and S. Thakur and T. Cheng and Q. Guo and T. Javaid and M. Mittal and L. Yuan and G. Bauer and Z. Hu and K. Yi and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and F. Monti and R. Sharma and J. N. Song and J. Tao and J. Wang and H. Zhang and A. Agapitos and Y. Ban and A. Levin and C. Li and Q. Li and X. Lyu and Y. Mao and S. J. Qian and X. Sun and D. Wang and H. Yang and C. Zhou and Z. You and N. Lu and X. Gao and D. Leggat and H. Okawa and Y. Zhang and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and J. Mejia Guisao and F. Ramirez and M. Rodriguez and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and S. Mishra and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and S. Konstantinou and J. Mousa and C. Nicolaou and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and Y. Assran and S. Elgammal and A. Lotfy and M. A. Mahmoud and R. K. Dewanjee and K. Ehataht and M. Kadastik and T. Lange and S. Nandan and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and H. Kirschenmann and K. Osterberg and M. Voutilainen and S. Bharthuar and E. Brücken and F. Garcia and J. Havukainen and K. T. S. Kallonen and M. S. Kim and R. Kinnunen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and M. Lotti and L. Martikainen and M. Myllymäki and M. m. Rantanen and H. Siikonen and E. Tuominen and J. Tuominiemi and P. Luukka and H. Petrow and T. Tuuva and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and V. Lohezic and J. Malcles and J. Rander and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and C. Baldenegro Barrera and F. Beaudette and A. Buchot Perraguin and P. Busson and A. Cappati and C. Charlot and F. Damas and O. Davignon and B. Diab and G. Falmagne and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and J. Motta and M. Nguyen and C. Ochando and L. Portales and R. Salerno and U. Sarkar and J. B. Sauvan and Y. Sirois and A. Tarabini and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and C. Grimault and R. Haeberle and A.-C. Le Bihan and M. A. Sessini and P. Van Hove and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and J. Choi and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and M. Vander Donckt and P. Verdier and J. Xiao and D. Chokheli and I. Lomidze and Z. Tsamalaidze and V. Botta and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and M. y. Lee and L. Mastrolorenzo and M. Merschmeyer and A. Meyer and S. Mondal and S. Mukherjee and D. Noll and A. Novak and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and S. C. Schuler and A. Sharma and A. Stein and F. Torres Da Silva De Araujo and L. Vigilante and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and W. Haj Ahmad and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and S. Bhattacharya and F. Blekman and K. Borras and D. Brunner and A. Campbell and A. Cardini and C. Cheng and F. Colombina and S. Consuegra Rodríguez and G. Correia Silva and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and O. Filatov and E. Gallo and A. Geiser and A. Giraldi and G. Greau and V. Guglielmi and M. Guthoff and A. Hinzmann and A. Jafari and L. Jeppe and N. Z. Jomhari and H. Jung and B. Kaech and M. Kasemann and H. Kaveh and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and J. Metwally and A. B. Meyer and G. Milella and M. Mormile and A. Mussgiller and A. Nürnberg and Y. Otarid and D. Pérez Adán and E. Ranken and A. Raspereza and B. Ribeiro Lopes and J. Rübenach and A. Saggio and M. Scham and V. Scheurer and S. Schnake and P. Schütze and C. Schwanenberger and M. Shchedrolosiev and R. E. Sosa Ricardo and L. P. Sreelatha Pramod and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and Y. Wen and K. Wichmann and L. Wiens and C. Wissing and S. Wuchterl and Y. Yang and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bein and L. Benato and M. Bonanomi and P. Connor and M. Eich and K. El Morabit and Y. Fischer and A. Fröhlich and C. Garbers and E. Garutti and A. Grohsjean and M. Hajheidari and J. Haller and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and A. Mehta and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and M. Wolf and S. Brommer and M. Burkart and E. Butz and T. Chwalek and A. Dierlamm and A. Droll and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and M. Horzela and U. Husemann and M. Klute and R. Koppenhöfer and M. Link and A. Lintuluoto and S. Maier and S. Mitra and Th. Müller and M. Neukum and M. Oh and G. Quast and K. Rabbertz and I. Shvetsov and H. J. Simonis and N. Trevisani and R. Ulrich and J. van der Linden and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and S. Wunsch and X. Zuo and G. Anagnostou and P. Assiouras and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and D. Karasavvas and P. Kontaxakis and G. Melachroinos and A. Panagiotou and I. Papavergou and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and K. Adamidis and I. Bestintzanos and I. Evangelou and C. Foudas and P. Gianneios and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and M. Bartók and C. Hajdu and D. Horvath and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and M. M. A. Gadallah and Á. Kadlecsik and P. Major and K. Mandal and G. Pásztor and A. J. Rádl and O. Surányi and G. I. Veres and G. Bencze and S. Czellar and J. Karancsi and J. Molnar and Z. Szillasi and P. Raics and B. Ujvari and G. Zilizi and T. Csorgo and F. Nemes and T. Novak and J. Babbar and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and R. Gupta and A. Kaur and H. Kaur and M. Kaur and S. Kumar and P. Kumari and M. Meena and K. Sandeep and T. Sheokand and J. B. Singh and A. Singla and A. Ahmed and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and S. Saumya and S. Baradia and S. Barman and D. Bhowmik and S. Dutta and B. Gomber and P. Palit and G. Saha and B. Sahu and S. Sarkar and P. K. Behera and S. C. Behera and P. Jana and P. Kalbhor and J. R. Komaragiri and D. Kumar and M. Mohammad Mobassir Ameen and A. Muhammad and L. Panwar and R. Pradhan and P. R. Pujahari and N. R. Saha and A. K. Sikdar and S. Verma and T. Aziz and I. Das and S. Dugad and M. Kumar and G. B. Mohanty and P. Suryadevara and A. Bala and S. Banerjee and M. Guchait and S. Karmakar and G. Majumder and K. Mazumdar and A. Thachayath and S. Bahinipati and A. K. Das and C. Kar and D. Maity and P. Mal and T. Mishra and V. K. Muraleedharan Nair Bindhu and K. Naskar and A. Nayak and P. Sadangi and P. Saha and S. K. Swain and S. Varghese and D. Vats and A. Alpana and S. Dube and B. Kansal and A. Laha and S. Pandey and A. Rastogi and S. Sharma and H. Bakhshiansohi and E. Khazaie and M. Zeinali and S. Chenarani and S. M. Etesami and M. Khakzad and M. Mohammadi Najafabadi and M. Grunewald and M. Abbrescia and R. Aly and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and A. Di Florio and W. Elmetenawee and L. Fiore and G. Iaselli and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and G. Ramirez-Sanchez and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and L. Borgonovi and R. Campanini and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and L. Lunerti and G. Masetti and F. L. Navarria and A. Perrotta and F. Primavera and A. M. Rossi and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and R. Potenza and A. Tricomi and C. Tuve and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and P. Chatagnon and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and G. Boldrini and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and D. Pedrini and B. S. Pinolini and S. Ragazzi and N. Redaelli and T. Tabarelli de Fatis and D. Zuolo and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and A. De Iorio and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and C. Sciacca and R. Ardino and P. Azzi and N. Bacchetta and M. Bellato and M. Benettoni and D. Bisello and P. Bortignon and A. Bragagnolo and R. Carlin and T. Dorigo and F. Gasparini and U. Gasparini and G. Grosso and L. Layer and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and G. Strong and M. Tosi and A. Triossi and S. Ventura and H. Yarar and M. Zanetti and P. Zotto and A. Zucchetta and S. Abu Zeid and C. Aimè and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and P. Asenov and G. M. Bilei and D. Ciangottini and L. Fanò and M. Magherini and G. Mantovani and V. Mariani and M. Menichelli and F. Moscatelli and A. Piccinelli and M. Presilla and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and D. Matos Figueiredo and A. Messineo and M. Musich and F. Palla and S. Parolia and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and A. Venturi and P. G. Verdini and P. Barria and M. Campana and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and E. Longo and P. Meridiani and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and R. Tramontano and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and S. Maselli and A. Mecca and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and D. Soldi and A. Staiano and C. Tarricone and M. Tornago and D. Trocino and G. Umoret and A. Vagnerini and E. Vlasov and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and G. Sorrentino and S. Dogra and C. Huh and B. Kim and D. H. Kim and J. Kim and J. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and S. I. Pak and M. S. Ryu and S. Sekmen and Y. C. Yang and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and D. Kim and T. J. Kim and J. A. Merlin and J. Park and S. Choi and S. Han and B. Hong and K. S. Lee and S. K. Park and J. Yoo and J. Goh and H. S. Kim and Y. Kim and S. Lee and J. Almond and J. H. Bhyun and S. Jeon and W. Jun and J. S. Kim and S. Ko and H. Kwon and H. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Yang and S. Ha and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Maghrbi and K. Dreimanis and A. Gaile and G. Pikurs and A. Potrebko and M. Seidel and V. Veckalns and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and N. Bin Norjoharuddeen and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and C. A. Mondragon Herrera and D. A. Perez Navarro and A. Sánchez Hernández and C. Oropeza Barrera and M. Ramírez García and I. Bautista and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and L. Grzanka and M. Malawski and H. Bialkowska and M. Bluj and B. Boimska and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and T. Niknejad and M. Pisano and J. Seixas and J. Varela and P. Adzic and P. Milenovic and M. Dordevic and J. Milosevic and V. Rekovic and M. Aguilar-Benitez and J. Alcaraz Maestre and M. Barrio Luna and Cristina F. Bedoya and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and J. León Holgado and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and D. D. Redondo Ferrero and L. Romero and S. Sánchez Navas and L. Urda Gómez and J. Vazquez Escobar and C. Willmott and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and J. R. González Fernández and E. Palencia Cortezon and C. Ramón Álvarez and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Bhowmik and S. Blanco Fernández and J. A. Brochero Cifuentes and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and C. Fernandez Madrazo and G. Gomez and C. Lasaosa García and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and C. Prieels and L. Scodellaro and I. Vila and J. M. Vizan Garcia and M. K. Jayananda and B. Kailasapathy and D. U. J. Sonnadara and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and N. Wickramage and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and B. Bilin and A. A. Bin Anuar and A. Bocci and E. Brondolin and C. Caillol and T. Camporesi and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and F. Fallavollita and L. Forthomme and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and L. Gouskos and M. Haranko and J. Hegeman and V. Innocente and T. James and P. Janot and J. Kieseler and N. Kratochwil and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and B. Maier and L. Malgeri and M. Mannelli and A. C. Marini and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Moortgat and M. Mulders and S. Orfanelli and F. Pantaleo and M. Peruzzi and A. Petrilli and G. Petrucciani and A. Pfeiffer and M. Pierini and D. Piparo and H. Qu and D. Rabady and G. Reales Gutiérrez and M. Rovere and H. Sakulin and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and A. Tsirou and D. Walter and J. Wanczyk and K. A. Wozniak and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and T. K. Aarrestad and K. Androsov and M. Backhaus and A. Calandri and K. Datta and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and L. Marchese and C. Martin Perez and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and M. G. Ratti and M. Reichmann and C. Reissel and T. Reitenspiess and B. Ristic and F. Riti and D. Ruini and D. A. Sanz Becerra and R. Seidita and J. Steggemann and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and C. Botta and D. Brzhechko and M. F. Canelli and K. Cormier and A. De Wit and R. Del Burgo and J. K. Heikkilä and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and V. M. Mikuni and U. Molinatti and I. Neutelings and A. Reimers and P. Robmann and S. Sanchez Cruz and K. Schweiger and M. Senger and Y. Takahashi and C. Adloff and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and S. S. Yu and L. Ceard and Y. Chao and K. F. Chen and P. s. Chen and Z. g. Chen and W.-S. Hou and T. h. Hsu and Y. w. Kao and R. Khurana and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and A. Psallidas and X. f. Su and J. Thomas-Wilsker and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and D. Agyel and F. Boran and Z. S. Demiroglu and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and U. Kiminsu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and S. Turkcapar and E. Uslan and I. S. Zorbakir and K. Ocalan and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and Y. Komurcu and S. Sen and O. Aydilek and S. Cerci and V. Epshteyn and B. Hacisahinoglu and I. Hos and B. Isildak and B. Kaynak and S. Ozkorucuklu and H. Sert and C. Simsek and D. Sunar Cerci and C. Zorbilmez and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and L. Kreczko and B. Krikler and S. Paramesvaran and S. Seif El Nasr-Storey and V. J. Smith and N. Stylianou and K. Walkingshaw Pass and R. White and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and K. V. Ellis and K. Harder and S. Harper and M.-L. Holmberg and Sh. Jain and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and T. Williams and R. Bainbridge and P. Bloch and C. E. Brown and O. Buchmuller and V. Cacchio and C. A. Carrillo Montoya and V. Cepaitis and G. S. Chahal and D. Colling and J. S. Dancu and P. Dauncey and G. Davies and J. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and M. H. Hassanshahi and A. Howard and G. Iles and M. Knight and J. Langford and L. Lyons and A.-M. Magnan and S. Malik and A. Martelli and M. Mieskolainen and J. Nash and M. Pesaresi and B. C. Radburn-Smith and A. Richards and A. Rose and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and L. H. Vage and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and K. Coldham and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and B. Caraway and J. Dittmann and K. Hatakeyama and J. Hiltbrand and A. R. Kanuganti and B. McMaster and M. Saunders and S. Sawant and C. Sutantawibul and M. Toms and J. Wilson and R. Bartek and A. Dominguez and C. Huerta Escamilla and A. E. Simsek and R. Uniyal and A. M. Vargas Hernandez and R. Chudasama and S. I. Cooper and S. V. Gleyzer and C. U. Perez and P. Rumerio and E. Usai and C. West and A. Akpinar and A. Albert and D. Arcaro and C. Cosby and Z. Demiragli and C. Erice and E. Fontanesi and D. Gastler and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and S. Yuan and G. Benelli and X. Coubez and D. Cutts and M. Hadley and U. Heintz and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and D. Li and J. Luo and M. Narain and N. Pervan and S. Sagir and F. Simpson and W. Y. Wong and X. Yan and D. Yu and W. Zhang and S. Abbott and J. Bonilla and C. Brainerd and R. Breedon and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and G. Haza and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and D. Pellett and B. Regnery and W. Wei and Y. Yao and F. Zhang and M. Bachtis and R. Cousins and A. Datta and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and E. Manca and W. A. Nash and D. Saltzberg and B. Stone and V. Valuev and R. Clare and M. Gordon and G. Hanson and W. Si and S. Wimpenny and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and R. Gerosa and L. Giannini and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and M. Quinnan and B. V. Sathia Narayanan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and L. Brennan and C. Campagnari and G. Collura and A. Dorsett and J. Incandela and M. Kilpatrick and A. J. Li and P. Masterson and H. Mei and M. Oshiro and J. Richman and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and S. Wang and A. Bornheim and O. Cerri and A. Latorre and J. M. Lawhorn and J. Mao and H. B. Newman and T. Q. Nguyen and M. Spiropulu and J. R. Vlimant and C. Wang and S. Xie and R. Y. Zhu and J. Alison and S. An and M. B. Andrews and P. Bryant and V. Dutta and T. Ferguson and A. Harilal and C. Liu and T. Mudholkar and S. Murthy and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hassani and G. Karathanasis and E. MacDonald and N. Manganelli and F. Marini and A. Perloff and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and J. Alexander and S. Bright-Thonney and X. Chen and D. J. Cranshaw and J. Fan and X. Fan and D. Gadkari and S. Hogan and J. Monroy and J. R. Patterson and J. Reichert and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and J. Dickinson and I. Dutta and V. D. Elvira and Y. Feng and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and R. Heller and T. C. Herwig and J. Hirschauer and L. Horyn and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and D. Lincoln and R. Lipton and T. Liu and C. Madrid and K. Maeshima and C. Mantilla and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and L. Cadamuro and P. Chang and V. Cherepanov and R. D. Field and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. H. Lo and K. Matchev and N. Menendez and G. Mitselmakher and A. Muthirakalayil Madhu and N. Rawal and D. Rosenzweig and S. Rosenzweig and K. Shi and T. Adams and A. Al Kadhim and A. Askew and N. Bower and R. Habibullah and V. Hagopian and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and O. Viazlo and M. Wulansatiti and R. Yohay and J. Zhang and B. Alsufyani and M. M. Baarmand and S. Butalla and T. Elkafrawy and M. Hohlmann and R. Kumar Verma and M. Rahmani and F. Yumiceva and M. R. Adams and C. Bennett and R. Cavanaugh and S. Dittmer and R. Escobar Franco and O. Evdokimov and C. E. Gerber and D. J. Hofman and J. h. Lee and D. S. Lemos and A. H. Merrit and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and T. Roy and S. Rudrabhatla and M. B. Tonjes and N. Varelas and X. Wang and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and J. Nachtman and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and T. Á. Vámi and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and C. Lindsey and J. Marquez and N. Minafra and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and R. Salvatico and S. Sanders and C. Smith and G. Wilson and B. Allmond and A. Ivanov and K. Kaadze and A. Kalogeropoulos and Y. Maravin and K. Nam and J. Natoli and D. Roy and F. Rebassoo and D. Wright and E. Adams and A. Baden and O. Baron and A. Belloni and A. Bethani and Y. m. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and L. Wang and K. Wong and J. Bendavid and W. Busza and I. A. Cali and Y. Chen and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mironov and C. Paus and D. Rankin and C. Roland and G. Roland and S. Rothman and Z. Shi and G. S. F. Stephans and Z. Wang and B. Wyslouch and T. J. Yang and R. M. Chatterjee and B. Crossman and B. M. Joshi and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and M. Revering and R. Rusack and R. Saradhy and N. Schroeder and N. Strobbe and M. A. Wadud and L. M. Cremaldi and K. Bloom and M. Bryson and D. R. Claes and C. Fangmeier and F. Golf and C. Joo and I. Kravchenko and I. Reed and J. E. Siado and G. R. Snow and W. Tabb and A. Wightman and F. Yan and A. G. Zecchinelli and G. Agarwal and H. Bandyopadhyay and L. Hay and I. Iashvili and A. Kharchilava and C. McLean and M. Morris and D. Nguyen and J. Pekkanen and S. Rappoccio and H. Rejeb Sfar and A. Williams and G. Alverson and E. Barberis and Y. Haddad and Y. Han and A. Krishna and J. Li and M. Lu and G. Madigan and B. Marzocchi and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and A. Tishelman-Charny and B. Wang and D. Wood and J. Bueghly and Z. Chen and K. A. Hahn and Y. Liu and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and R. Band and R. Bucci and S. Castells and M. Cremonesi and A. Das and R. Goldouzian and M. Hildreth and K. W. Ho and K. Hurtado Anampa and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and K. Mohrman and C. Moore and Y. Musienko and H. Nelson and M. Osherson and R. Ruchti and A. Townsend and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and B. Bylsma and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and A. Lesauvage and M. Nunez Ornelas and K. Wei and B. L. Winer and B. R. Yates and F. M. Addesa and H. Bouchamaoui and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and S. Higginbotham and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and D. Stickland and C. Tully and A. S. Bakshi and V. E. Barnes and S. Chandra and R. Chawla and S. Das and A. Gu and L. Gutay and M. Jones and A. W. Jung and D. Kondratyev and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and A. Purohit and J. F. Schulte and M. Stojanovic and J. Thieman and A. K. Virdi and F. Wang and W. Xie and J. Dolen and N. Parashar and A. Pathak and D. Acosta and A. Baty and T. Carnahan and S. Dildick and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and W. Li and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and C. Fallon and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and P. Parygin and E. Popova and R. Taus and G. P. Van Onsem and K. Goulianos and B. Chiarito and J. P. Chou and Y. Gershtein and E. Halkiadakis and A. Hart and M. Heindl and D. Jaroslawski and O. Karacheban and I. Laflotte and A. Lath and R. Montalvo and K. Nash and H. Routray and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and H. Wang and H. Acharya and A. G. Delannoy and S. Fiorendi and T. Holmes and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and O. Bouhali and M. Dalchenko and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and S. Malhotra and R. Mueller and D. Overton and D. Rathjens and A. Safonov and N. Akchurin and J. Damgov and V. Hegde and A. Hussain and Y. Kazhykarim and K. Lamichhane and A. Mankel and T. Mengke and S. Muthumuni and T. Peltola and I. Volobouev and A. Whitbeck and E. Appelt and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and A. Li and C. Neu and C. E. Perez Lara and P. E. Karchin and A. Aravind and K. Black and T. Bose and S. Dasu and I. De Bruyn and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Andreev and Yu. Andreev and T. Aushev and M. Azarkin and A. Babaev and V. Blinov and E. Boos and V. Borshch and D. Budkouski and V. Bunichev and V. Chekhovsky and R. Chistov and M. Danilov and A. Dermenev and T. Dimova and D. Druzhkin and M. Dubinin and L. Dudko and A. Ershov and G. Gavrilov and V. Gavrilov and S. Gninenko and V. Golovtcov and N. Golubev and I. Golutvin and I. Gorbunov and A. Gribushin and Y. Ivanov and V. Kachanov and L. Kardapoltsev and V. Karjavine and A. Karneyeu and V. Kim and M. Kirakosyan and D. Kirpichnikov and M. Kirsanov and V. Klyukhin and O. Kodolova and D. Konstantinov and V. Korenkov and A. Kozyrev and N. Krasnikov and A. Lanev and P. Levchenko and N. Lychkovskaya and V. Makarenko and A. Malakhov and V. Matveev and V. Murzin and A. Nikitenko and S. Obraztsov and V. Oreshkin and A. Oskin and V. Palichik and V. Perelygin and S. Polikarpov and V. Popov and O. Radchenko and M. Savina and V. Savrin and D. Selivanova and V. Shalaev and S. Shmatov and S. Shulha and Y. Skovpen and S. Slabospitskii and V. Smirnov and A. Snigirev and D. Sosnov and V. Sulimov and E. Tcherniaev and A. Terkulov and O. Teryaev and I. Tlisova and A. Toropin and L. Uvarov and A. Uzunian and A. Vorobyev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and A. Zhokin}, doi = {10.1103/PhysRevLett.134.131802}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {131802}, shortjournal = {Phys. Rev. Lett.}, title = {Search for fractionally charged particles in proton-proton collisions at s=13 TeV}, volume = {134}, year = {2025}, }
• (2025). Measurements of pion and muon nuclear capture at rest on argon in the LArIAT experiment. PRL, 134(13), 131801. (www)

  @article{ , abstract = {We report the measurement of the final-state products of negative pion and muon nuclear capture at rest on argon by the LArIAT experiment at the Fermilab Test Beam Facility. We measure a population of isolated MeV-scale energy depositions, or blips, in 296 LArIAT events containing tracks from stopping low-momentum pions and muons. The average numbers of visible blips are measured to be 0.74 ± 0.19 and 1.86 ± 0.17 near muon and pion track endpoints, respectively. The 3.6 σ statistically significant difference in blip content between muons and pions provides the first demonstration of a new method of pion-muon discrimination in neutrino liquid argon time projection chamber experiments. LArIAT Monte Carlo simulations predict substantially higher average blip counts for negative muon ( 1.22 ± 0.08 ) and pion ( 2.34 ± 0.09 ) nuclear captures. We attribute this difference to geant 4’s inaccurate simulation of the nuclear capture process.}, archive = {J_PRL}, author = {LArIAT Collaboration and M. A. Hernandez-Morquecho and R. Acciarri and J. Asaadi and M. Backfish and W. Badgett and V. Basque and F. d. M. Blaszczyk and W. Foreman and R. A. Gomes and E. Gramellini and J. Ho and E. Kearns and E. Kemp and T. Kobilarcik and M. King and B. R. Littlejohn and X. Luo and A. Marchionni and C. A. Moura and J. L. Raaf and D. W. Schmitz and M. Soderberg and J. M. St. John and A. M. Szelc and T. Yang}, doi = {10.1103/PhysRevLett.134.131801}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {131801}, shortjournal = {Phys. Rev. Lett.}, title = {Measurements of pion and muon nuclear capture at rest on argon in the LArIAT experiment}, volume = {134}, year = {2025}, }
• (2025). Parisi-sourlas supertranslation and scale invariance without conformal symmetry. PRL, 134(13), 131602. (www)

  @article{ , abstract = {Inspired by the possibility of emergent supersymmetry in critical random systems, we study a field theory model with a quartic potential of one superfield, possessing the Parisi-Sourlas supertranslation symmetry. Within perturbative ε expansion, we find nine nontrivial scale-invariant renormalization group fixed points, but only one of them is conformal. We, however, believe scale invariance without conformal invariance cannot occur without a sophisticated mechanism because it predicts the existence of a nonconserved but nonrenormalized vector operator called virial current, whose existence must be nongeneric. We show that the virial current in this model is related to the supercurrent by supertranslation. The supertranslation Ward-Takahashi identity circumvents the genericity argument, explaining its nonrenormalization property.}, archive = {J_PRL}, author = {Yu Nakayama}, doi = {10.1103/PhysRevLett.134.131602}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {131602}, shortjournal = {Phys. Rev. Lett.}, title = {Parisi-sourlas supertranslation and scale invariance without conformal symmetry}, volume = {134}, year = {2025}, }
• (2025). Measuring cosmic expansion with diffractive gravitational scintillation of nanohertz gravitational waves. PRL, 134(13), 131001. (www)

  @article{ , abstract = {The recent discovery of ultralong wavelength gravitational waves through the advent of pulsar timing arrays (PTA) has opened up new avenues for fundamental science. Here we show that every PTA source will be diffractively lensed by potentially hundreds of galactic disks transverse to its line of sight, leading to modest modulations in the strain, Δ h / h ∼ 10 − 3 λ 1 pc − 1 , due to wave lensing effects. The induced interference, or scintillation, pattern will be resolvable by coherent PTAs and may be leveraged, alongside foreground redshift information, to make precise measurements of cosmic expansion. If future PTA experiments can achieve enough signal to noise to detect these small modulations, hundreds of redshift-distance pairs may be inferred from the diffractive lensing of an individual PTA source.}, archive = {J_PRL}, author = {Dylan L. Jow and Ue-Li Pen}, doi = {10.1103/PhysRevLett.134.131001}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {131001}, shortjournal = {Phys. Rev. Lett.}, title = {Measuring cosmic expansion with diffractive gravitational scintillation of nanohertz gravitational waves}, volume = {134}, year = {2025}, }
• (2025). Fast and accurate greenberger-horne-zeilinger encoding using all-to-all interactions. PRL, 134(13), 130604. (www)

  @article{ , abstract = {The -qubit Greenberger-Horne-Zeilinger (GHZ) state is an important resource for quantum technologies. We consider the task of GHZ encoding using all-to-all interactions, which prepares the GHZ state in a special case, and is furthermore useful for quantum error correction, interaction-rate enhancement, and transmitting information using power-law interactions. The naive protocol based on parallelizing cnot gates takes O(1)-time of Hamiltonian evolution. In this work, we propose a fast protocol that achieves GHZ encoding with high accuracy. The evolution time almost saturates the theoretical limit . Moreover, the final state is close to the ideal encoded one with high fidelity , up to large system sizes . The protocol only requires a few stages of time-independent Hamiltonian evolution; the key idea is to use the data qubit as control, and to use fast spin-squeezing dynamics generated by e.g., two-axis twisting.}, archive = {J_PRL}, author = {Chao Yin}, doi = {10.1103/PhysRevLett.134.130604}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {130604}, shortjournal = {Phys. Rev. Lett.}, title = {Fast and accurate greenberger-horne-zeilinger encoding using all-to-all interactions}, volume = {134}, year = {2025}, }
• (2025). Mechanical multiplexer of nuclear spin states. PRL, 134(13), 130603. (www)

  @article{ , abstract = {A spin 1 / 2 is the simplest system that has been believed to support a single two-level quantum system, represented by a single resonance. We experimentally demonstrate that a spin- 1 / 2 nucleus of F 19 in C 6 F 6 exhibits an extra resonance corresponding to the emergence of the states, by mechanically rotating a sample and a coil in nuclear magnetic resonance (NMR) measurements. On the basis of the Floquet formalism, we identify the emergence of the extra two-level state due to the temporal periodicity generated by the mechanical rotation (mechanical spin multiplexing) and derive an operator algebra analogous to the planar rotor algebra in an effective description of the system. The observed multiplexing allows a single spin 1 / 2 to carry more than two states and potentially enabling the processing of multiple quantum bits on a single spin.}, archive = {J_PRL}, author = {Hiroyuki Chudo and Naoto Yokoi and Mamoru Matsuo and Kazuya Harii and Jun Suzuki and Masaki Imai and Masahiro Sato and Sadamichi Maekawa and Eiji Saitoh}, doi = {10.1103/PhysRevLett.134.130603}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {130603}, shortjournal = {Phys. Rev. Lett.}, title = {Mechanical multiplexer of nuclear spin states}, volume = {134}, year = {2025}, }
• (2025). Hidden time reversal in driven XXZ spin chains: Exact solutions and new dissipative phase transitions. PRL, 134(13), 130404. (www)

  @article{ , abstract = {We show that several models of interacting X X Z spin chains subject to boundary driving and dissipation possess a subtle kind of time-reversal symmetry, making their steady states exactly solvable. We focus on a model with a coherent boundary drive, showing that it exhibits a unique continuous dissipative phase transition as a function of the boundary drive amplitude. This transition has no analog in the bulk closed system or in incoherently driven models. We also show the steady-state magnetization exhibits a surprising fractal dependence on interaction strength, something previously associated with less easily measured infinite-temperature transport quantities (the Drude weight). Our exact solution also directly yields driven-dissipative double-chain models that have pure, entangled steady states that are current carrying.}, archive = {J_PRL}, author = {Mingxing Yao and Andrew Lingenfelter and Ron Belyansky and David Roberts and Aashish A. Clerk}, doi = {10.1103/PhysRevLett.134.130404}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {130404}, shortjournal = {Phys. Rev. Lett.}, title = {Hidden time reversal in driven XXZ spin chains: Exact solutions and new dissipative phase transitions}, volume = {134}, year = {2025}, }
• (2025). Low-depth unitary quantum circuits for dualities in one-dimensional quantum lattice models. PRL, 134(13), 130403. (www)

  @article{ , abstract = {A systematic approach to dualities in symmetric ( 1 + 1 ) d quantum lattice models has recently been proposed in terms of module categories over the symmetry fusion categories. By characterizing the nontrivial way in which dualities intertwine closed boundary conditions and charge sectors, these can be implemented by unitary matrix product operators. In this Letter, we explain how to turn such duality operators into unitary linear depth quantum circuits via the introduction of ancillary degrees of freedom that keep track of the various sectors. The linear depth is consistent with the fact that these dualities change the phase of the states on which they act. When supplemented with measurements, we show that dualities with respect to symmetries encoded into nilpotent fusion categories can be realized in constant depth. The resulting circuits can for instance be used to efficiently prepare short- and long-range entangled states or map between different gapped boundaries of ( 2 + 1 ) d topological models.}, archive = {J_PRL}, author = {Laurens Lootens and Clement Delcamp and Dominic Williamson and Frank Verstraete}, doi = {10.1103/PhysRevLett.134.130403}, journal = {Physical Review Letters}, month = {4}, number = {13}, pages = {130403}, shortjournal = {Phys. Rev. Lett.}, title = {Low-depth unitary quantum circuits for dualities in one-dimensional quantum lattice models}, volume = {134}, year = {2025}, }
• (2025). Erratum: Nonmonotonic energy dependence of net-proton number fluctuations [Phys. rev. lett. 126, 092301 (2021)]. PRL, 134(13), 139902. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 139902 (2025)}, archive = {J_PRL}, author = {STAR Collaboration and J. Adam and L. Adamczyk and J. R. Adams and J. K. Adkins and G. Agakishiev and M. M. Aggarwal and Z. Ahammed and I. Alekseev and D. M. Anderson and A. Aparin and E. C. Aschenauer and M. U. Ashraf and F. G. Atetalla and A. Attri and G. S. Averichev and V. Bairathi and K. Barish and A. Behera and R. Bellwied and A. Bhasin and J. Bielcik and J. Bielcikova and L. C. Bland and I. G. Bordyuzhin and J. D. Brandenburg and A. V. Brandin and J. Butterworth and H. Caines and M. Calderón de la Barca Sánchez and D. Cebra and I. Chakaberia and P. Chaloupka and B. K. Chan and F-H. Chang and Z. Chang and N. Chankova-Bunzarova and A. Chatterjee and D. Chen and J. Chen and J. H. Chen and X. Chen and Z. Chen and J. Cheng and M. Cherney and M. Chevalier and S. Choudhury and W. Christie and X. Chu and H. J. Crawford and M. Csanád and M. Daugherity and T. G. Dedovich and I. M. Deppner and A. A. Derevschikov and L. Didenko and X. Dong and J. L. Drachenberg and J. C. Dunlop and T. Edmonds and N. Elsey and J. Engelage and G. Eppley and S. Esumi and O. Evdokimov and A. Ewigleben and O. Eyser and R. Fatemi and S. Fazio and P. Federic and J. Fedorisin and C. J. Feng and Y. Feng and P. Filip and E. Finch and Y. Fisyak and A. Francisco and L. Fulek and C. A. Gagliardi and T. Galatyuk and F. Geurts and A. Gibson and K. Gopal and X. Gou and D. Grosnick and W. Guryn and A. I. Hamad and A. Hamed and S. Harabasz and J. W. Harris and S. He and W. He and X. H. He and Y. He and S. Heppelmann and N. Herrmann and E. Hoffman and L. Holub and Y. Hong and S. Horvat and Y. Hu and H. Z. Huang and S. L. Huang and T. Huang and X. Huang and T. J. Humanic and P. Huo and G. Igo and D. Isenhower and W. W. Jacobs and C. Jena and A. Jentsch and Y. JI and J. Jia and K. Jiang and S. Jowzaee and X. Ju and E. G. Judd and S. Kabana and M. L. Kabir and S. Kagamaster and D. Kalinkin and K. Kang and D. Kapukchyan and K. Kauder and H. W. Ke and D. Keane and A. Kechechyan and M. Kelsey and Y. V. Khyzhniak and D. P. Kikoła and C. Kim and B. Kimelman and D. Kincses and T. A. Kinghorn and I. Kisel and A. Kiselev and M. Kocan and L. Kochenda and L. K. Kosarzewski and L. Kramarik and P. Kravtsov and K. Krueger and N. Kulathunga Mudiyanselage and L. Kumar and S. Kumar and R. Kunnawalkam Elayavalli and J. H. Kwasizur and R. Lacey and S. Lan and J. M. Landgraf and J. Lauret and A. Lebedev and R. Lednicky and J. H. Lee and Y. H. Leung and C. Li and W. Li and X. Li and Y. Li and Y. Liang and R. Licenik and T. Lin and Y. Lin and M. A. Lisa and F. Liu and H. Liu and P. Liu and T. Liu and X. Liu and Y. Liu and Z. Liu and T. Ljubicic and W. J. Llope and R. S. Longacre and N. S. Lukow and S. Luo and X. Luo and G. L. Ma and L. Ma and R. Ma and Y. G. Ma and N. Magdy and R. Majka and D. Mallick and S. Margetis and C. Markert and H. S. Matis and J. A. Mazer and N. G. Minaev and S. Mioduszewski and B. Mohanty and I. Mooney and Z. Moravcova and D. A. Morozov and M. Nagy and J. D. Nam and Md. Nasim and K. Nayak and D. Neff and J. M. Nelson and D. B. Nemes and M. Nie and G. Nigmatkulov and T. Niida and L. V. Nogach and T. Nonaka and A. S. Nunes and G. Odyniec and A. Ogawa and S. Oh and V. A. Okorokov and B. S. Page and R. Pak and A. Pandav and Y. Panebratsev and B. Pawlik and D. Pawlowska and H. Pei and C. Perkins and L. Pinsky and R. L. Pintér and J. Pluta and J. Porter and M. Posik and N. K. Pruthi and M. Przybycien and J. Putschke and H. Qiu and A. Quintero and S. K. Radhakrishnan and S. Ramachandran and R. L. Ray and R. Reed and H. G. Ritter and O. V. Rogachevskiy and J. L. Romero and L. Ruan and J. Rusnak and N. R. Sahoo and H. Sako and S. Salur and J. Sandweiss and S. Sato and W. B. Schmidke and N. Schmitz and B. R. Schweid and F. Seck and J. Seger and M. Sergeeva and R. Seto and P. Seyboth and N. Shah and E. Shahaliev and P. V. Shanmuganathan and M. Shao and A. I. Sheikh and W. Q. Shen and S. S. Shi and Y. Shi and Q. Y. Shou and E. P. Sichtermann and R. Sikora and M. Simko and J. Singh and S. Singha and N. Smirnov and W. Solyst and P. Sorensen and H. M. Spinka and B. Srivastava and T. D. S. Stanislaus and M. Stefaniak and D. J. Stewart and M. Strikhanov and B. Stringfellow and A. A. P. Suaide and M. Sumbera and B. Summa and X. M. Sun and X. Sun and Y. Sun and B. Surrow and D. N. Svirida and P. Szymanski and A. H. Tang and Z. Tang and A. Taranenko and T. Tarnowsky and J. H. Thomas and A. R. Timmins and D. Tlusty and M. Tokarev and C. A. Tomkiel and S. Trentalange and R. E. Tribble and P. Tribedy and S. K. Tripathy and O. D. Tsai and Z. Tu and T. Ullrich and D. G. Underwood and I. Upsal and G. Van Buren and J. Vanek and A. N. Vasiliev and I. Vassiliev and F. Videbæk and S. Vokal and S. A. Voloshin and F. Wang and G. Wang and J. S. Wang and P. Wang and Y. Wang and Z. Wang and J. C. Webb and P. C. Weidenkaff and L. Wen and G. D. Westfall and H. Wieman and S. W. Wissink and R. Witt and Y. Wu and Z. G. Xiao and G. Xie and W. Xie and H. Xu and N. Xu and Q. H. Xu and Y. F. Xu and Y. Xu and Z. Xu and C. Yang and Q. Yang and S. Yang and Y. Yang and Z. Yang and Z. Ye and L. Yi and K. Yip and Y. Yu and H. Zbroszczyk and W. Zha and C. Zhang and D. Zhang and S. Zhang and X. P. Zhang and Y. Zhang and Z. J. Zhang and Z. Zhang and J. Zhao and C. Zhong and C. Zhou and X. Zhu and Z. Zhu and M. Zurek and M. Zyzak}, doi = {10.1103/PhysRevLett.134.139902}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {139902}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Nonmonotonic energy dependence of net-proton number fluctuations [Phys. rev. lett. 126, 092301 (2021)]}, volume = {134}, year = {2025}, }
• (2025). Segregation in binary mixture with differential contraction among active rings. PRL, 134(13), 138401. (www)

  @article{ , abstract = {Cell cortex contraction is vital for shaping cells, enabling movement, division, and responding to mechanical signals–processes crucial for multicellular organisms. Differential membrane contractions between cells significantly influence segregation. We present a model where active particle rings interact through differential contraction, showing that segregation arises from this mechanism, with ring activity functioning as an effective temperature. The interface decay exponent is close to λ ∼ 1 / 3 , differing from previous cluster fusion and diffusion model predictions.}, archive = {J_PRL}, author = {Emanuel F. Teixeira and Carine P. Beatrici and Heitor C. M. Fernandes and Leonardo G. Brunnet}, doi = {10.1103/PhysRevLett.134.138401}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {138401}, shortjournal = {Phys. Rev. Lett.}, title = {Segregation in binary mixture with differential contraction among active rings}, volume = {134}, year = {2025}, }
• (2025). Liquid-liquid phase transition in simulated supercooled water nanodroplets. PRL, 134(13), 138001. (www)

  @article{ , abstract = {Using simulations, we demonstrate how a liquid-liquid phase transition (LLPT) manifests in supercooled water nanodroplets. Selecting an interaction potential for which a LLPT occurs in the bulk liquid, we conduct simulations of supercooled water nanodroplets having between 1000 and 80000 molecules. We show that as the droplet size decreases, the Laplace pressure grows large enough to drive the droplets through the transition from the low-density to the high-density liquid phase, and that all droplets in this size range are large enough to have cores exhibiting the structure and properties of bulk water. To guide experiments, we estimate the range of values for the critical pressure of the LLPT in real water that can be observed using nanodroplets, and propose structural and dynamical measures by which the LLPT in nanodroplets can be detected.}, archive = {J_PRL}, author = {Shahrazad M. A. Malek and Francesco Sciortino and Peter H. Poole and Ivan Saika-Voivod}, doi = {10.1103/PhysRevLett.134.138001}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {138001}, shortjournal = {Phys. Rev. Lett.}, title = {Liquid-liquid phase transition in simulated supercooled water nanodroplets}, volume = {134}, year = {2025}, }
• (2025). Synergistic signatures of group mechanisms in higher-order systems. PRL, 134(13), 137401. (www)

  @article{ , abstract = {The interplay between causal mechanisms and emerging collective behaviors is a central aspect of understanding, controlling, and predicting complex networked systems. In our work, we investigate the relationship between higher-order mechanisms and higher-order behavioral observables in two representative models with group interactions: a simplicial Ising model and a social contagion model. In both systems, we find that group (higher-order) interactions show emergent synergistic (higher-order) behavior. The emergent synergy appears only at the group level and depends in a complex, nonlinear way on the trade-off between the strengths of the low- and higher-order mechanisms and is invisible to low-order behavioral observables. Our work sets the basis for systematically investigating the relation between causal mechanisms and behavioral patterns in complex networked systems with group interactions, offering a robust methodological framework to tackle this challenging task.}, archive = {J_PRL}, author = {Thomas Robiglio and Matteo Neri and Davide Coppes and Cosimo Agostinelli and Federico Battiston and Maxime Lucas and Giovanni Petri}, doi = {10.1103/PhysRevLett.134.137401}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {137401}, shortjournal = {Phys. Rev. Lett.}, title = {Synergistic signatures of group mechanisms in higher-order systems}, volume = {134}, year = {2025}, }
• (2025). Synthesized acoustic vortex-frequency comb via rotational doppler effect. PRL, 134(13), 137001. (www)

  @article{ , abstract = {The synergistic control of light’s frequency and orbital angular momentum (OAM) via integrated nonlinear ring microresonators is crucial for creating spatiotemporal optical waveforms and advancing optical metrology. A direct analog of this capability in acoustics is challenging due to the nonlinearity-based mechanisms’ dependence on external driving and limited frequency conversion efficiency. Here, we present an acoustic synthesized comb structure derived from spatiotemporal metasurfaces, concurrently controlling frequency and OAM characteristics with high conversion efficiency and removing the constraints of critical driving frequency and power level in nonlinear mechanisms. By optimizing comb structures, energy distributions among OAM modes are adjusted to different frequency lines. We finally propose spatiotemporal metalens devices based on vortex-frequency combs, enabling synchronously multiple-order spatial differential operations for parallel data processing. This Letter is groundbreaking in integrating spectral- and spatial-domain acoustic waves, promising multifunctional imaging and advantages in spatiotemporal beams.}, archive = {J_PRL}, author = {Yurou Jia and Xuan Zhang and Suying Zhang and Guoqiang Xu and Taoyu Chen and Hongtao Zhou and Yechao Bai and Ying Cheng and Dajian Wu and Xiaojun Liu and Cheng-Wei Qiu}, doi = {10.1103/PhysRevLett.134.137001}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {137001}, shortjournal = {Phys. Rev. Lett.}, title = {Synthesized acoustic vortex-frequency comb via rotational doppler effect}, volume = {134}, year = {2025}, }
• (2025). Orbital-excitation-dominated magnetization dissipation and quantum oscillation of gilbert damping in fe films. PRL, 134(13), 136701. (www)

  @article{ , abstract = {Using first-principles electronic structure calculation, we demonstrate the spin dissipation process in bulk Fe by orbital excitations within the energy bands of pure spin character. The variation of orbitals in the intraband transitions provides an efficient channel to convert spin to orbital angular momentum with spin-orbit interaction. This mechanism dominates the Gilbert damping of Fe below room temperature. The theoretical prediction is confirmed by the ferromagnetic resonance experiment performed on single-crystal Fe(001) films. A significant thickness-dependent damping oscillation is found at low temperature induced by the quantum well states of the corresponding energy bands. Our findings not only explain the microscopic nature of the recently reported ultralow damping of Fe-based alloys but also help for the understanding of the transport and dissipation process of orbital currents.}, archive = {J_PRL}, author = {Yue Chen and Haoran Chen and Xi Shen and Weizhao Chen and Yi Liu and Yizheng Wu and Zhe Yuan}, doi = {10.1103/PhysRevLett.134.136701}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {136701}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital-excitation-dominated magnetization dissipation and quantum oscillation of gilbert damping in fe films}, volume = {134}, year = {2025}, }
• (2025). Superconductivity in twisted WSe2 from topology-induced quantum fluctuations. PRL, 134(13), 136503. (www)

  @article{ , abstract = {Recently, superconductivity has been observed in twisted WSe 2 moiré structures (Xia et al. , Nature (London) 637 , 833 (2025) ; Guo et al. , Nature (London) 637 , 839 (2025) ). Its transition temperature is high, reaching a few percent of the Fermi temperature scale. Here, we advance a mechanism for superconductivity based on the notion that electronic topology enables quantum fluctuations in a suitable regime of intermediate correlations. In this regime, the Coulomb interaction requires that an active topological flat band and nearby wider bands are considered together. Compact molecular orbitals arise, which give rise to quantum fluctuations through topology-dictated hybridization with the other molecular orbitals. The hybridization competes with the active flat band’s natural tendency toward static electronic ordering, thereby weakening the latter; we link this effect with certain salient observations by experiments. Furthermore, the competition yields a quantum critical regime where quasiparticles are lost. The corresponding quantum critical fluctuations drive superconductivity. Broader implications and new connections among correlated materials platforms are discussed.}, archive = {J_PRL}, author = {Fang Xie and Lei Chen and Shouvik Sur and Yuan Fang and Jennifer Cano and Qimiao Si}, doi = {10.1103/PhysRevLett.134.136503}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {136503}, shortjournal = {Phys. Rev. Lett.}, title = {Superconductivity in twisted WSe2 from topology-induced quantum fluctuations}, volume = {134}, year = {2025}, }
• (2025). Closed band-projected density algebra must be girvin-MacDonald-platzman. PRL, 134(13), 136502. (www)

  @article{ , abstract = {The band-projected density operators in a Landau level obey the Girvin-MacDonald-Platzman (GMP) algebra, and a large amount of effort in the study of fractional Chern insulators has been directed toward approximating this algebra in a Chern band. In this Letter, we prove that the GMP algebra, up to form factors, is the only closed algebra that projected density operators can satisfy in two and three dimensions, highlighting the central place it occupies in the study of Chern bands in general. A number of interesting corollaries follow.}, archive = {J_PRL}, author = {Ziwei Wang and Steven H. Simon}, doi = {10.1103/PhysRevLett.134.136502}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {136502}, shortjournal = {Phys. Rev. Lett.}, title = {Closed band-projected density algebra must be girvin-MacDonald-platzman}, volume = {134}, year = {2025}, }
• (2025). Cooperation between electron-phonon coupling and electronic interaction in bilayer nickelates La3Ni2O7. PRL, 134(13), 136002. (www)

  @article{ , abstract = {The recent observation of high- T c superconductivity in the bilayer nickelate La 3 Ni 2 O 7 under pressure has garnered significant interest. While researches have predominantly focused on the role of electron-electron interactions in the superconducting mechanism, the impact of electron-phonon coupling (EPC) has remained elusive and unexplored. In this Letter, we perform first-principles calculations to study the phonon spectrum and electron-phonon coupling within La 3 Ni 2 O 7 under pressure and explore the interplay between EPC and electronic interactions on the superconductivity by employing functional renormalization group (FRG) approach. Our calculations reveal that EPC alone is insufficient to trigger superconductivity in La 3 Ni 2 O 7 under pressure. We identify unique out-of-plane and in-plane breathing phonon modes which selectively couple with the Ni d z 2 and d x 2 − y 2 orbitals, showcasing an orbital-selective EPC. Within the bilayer two-orbital model, it is revealed that solely electronic interactions foster s ± -wave pairing characterized by notable frustration in the band space, leading to a relatively low transition temperature. Remarkably, we find that the out-of-plane EPC can act in concert with electronic interactions to promote the interlayer pairing in the d z 2 orbital, partially releasing the pairing frustration and thus elevating T c . In contrast, the inclusion of in-plane EPC only marginally affects the superconductivity, distinct from the cuprates. Potential experimental implications in La 3 Ni 2 O 7 are also discussed.}, archive = {J_PRL}, author = {Jun Zhan and Yuhao Gu and Xianxin Wu and Jiangping Hu}, doi = {10.1103/PhysRevLett.134.136002}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {136002}, shortjournal = {Phys. Rev. Lett.}, title = {Cooperation between electron-phonon coupling and electronic interaction in bilayer nickelates La3Ni2O7}, volume = {134}, year = {2025}, }
• (2025). Chiral superfluid helium-3 in the quasi-two-dimensional limit. PRL, 134(13), 136001. (www)

  @article{ , abstract = {Anisotropic pair breaking close to surfaces favors the chiral A phase of the superfluid He 3 over the time-reversal invariant B phase. Confining the superfluid He 3 into a cavity of height D of the order of the Cooper pair size characterized by the coherence length ξ 0 —ranging between 16 nm (34 bar) and 77 nm (0 bar)—extends the surface effects over the whole sample volume, thus allowing stabilization of the A phase at pressures P and temperatures T where otherwise the B phase would be stable. In this Letter, the surfaces of such a confined sample are covered with a superfluid He 4 film to create specular quasiparticle scattering boundary conditions, preventing the suppression of the superfluid order parameter. We show that the chiral A phase is the stable superfluid phase under strong confinement over the full P − T phase diagram down to a quasi-two-dimensional limit D / ξ 0 = 1 , where D = 80 nm . The planar phase, which is degenerate with the chiral A phase in the weak-coupling limit, is not observed. The gap inferred from measurements over the wide pressure range from 0.2 to 21.0 bar leads to an empirical ansatz for temperature-dependent strong-coupling effects. We discuss how these results pave the way for the realization of the fully gapped two-dimensional p x + i p y superfluid under more extreme confinement.}, archive = {J_PRL}, author = {Petri J. Heikkinen and Lev V. Levitin and Xavier Rojas and Angadjit Singh and Nathan Eng and Andrew Casey and John Saunders and Anton Vorontsov and Nikolay Zhelev and Abhilash Thanniyil Sebastian and Jeevak M. Parpia}, doi = {10.1103/PhysRevLett.134.136001}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {136001}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral superfluid helium-3 in the quasi-two-dimensional limit}, volume = {134}, year = {2025}, }
• (2025). Observation of nonaxisymmetric standard magnetorotational instability induced by a free-shear layer. PRL, 134(13), 135101. (www)

  @article{ , abstract = {The standard magnetorotational instability (SMRI) with a magnetic field component parallel to the rotation axis is widely believed to be responsible for the fast accretion in astronomical disks. In conventional base flows with a Keplerian profile or an ideal Couette profile, most studies focus on axisymmetric SMRI, since excitation of nonaxisymmetric SMRI in such flows requires a magnetic Reynolds number (Rm) more than an order of magnitude larger. Here, we report that, in a magnetized Taylor-Couette flow, nonaxisymmetric SMRI with an azimuthal mode number m = 1 can be triggered by a free-shear layer in the base flow at Rm ≳ 1 , the same threshold as for axisymmetric SMRI. Global linear analysis reveals that the free-shear layer reduces the required Rm, possibly by introducing an extremum in the vorticity of the base flow. Nonlinear simulations validate the results from linear analysis and confirm that a novel instability recently discovered experimentally [Wang et al. , Nat. Commun. 13 , 4679 (2022) ] is the nonaxisymmetric m = 1 SMRI. Our finding has astronomical implications as free-shear layers are ubiquitous in celestial systems, such as the disk-star boundary layer, the solar tachocline, and the edge of planet-opened gaps in protoplanetary disks.}, archive = {J_PRL}, author = {Yin Wang and Fatima Ebrahimi and Hongke Lu and Jeremy Goodman and Erik P. Gilson and Hantao Ji}, doi = {10.1103/PhysRevLett.134.135101}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {135101}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of nonaxisymmetric standard magnetorotational instability induced by a free-shear layer}, volume = {134}, year = {2025}, }
• (2025). Fluctuation-induced bistability of fermionic atoms coupled to a dissipative cavity. PRL, 134(13), 133602. (www)

  @article{ , abstract = {We investigate the steady state phase diagram of fermionic atoms subjected to an optical lattice and coupled to a high finesse optical cavity with photon losses. The coupling between the atoms and the cavity field is induced by a transverse pump beam. Taking fluctuations around the mean-field solutions into account, we find that a transition to a self-organized phase takes place at a critical value of the pump strength. In the self-organized phase the cavity field takes a finite expectation value and the atoms show a modulation in the density. Surprisingly, at even larger pump strengths two self-organized stable solutions of the cavity field and the atoms occur, signaling the presence of a bistability. We show that the bistable behavior is induced by the atoms-cavity fluctuations and is not captured by the mean-field approach.}, archive = {J_PRL}, author = {Luisa Tolle and Ameneh Sheikhan and Thierry Giamarchi and Corinna Kollath and Catalin-Mihai Halati}, doi = {10.1103/PhysRevLett.134.133602}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {133602}, shortjournal = {Phys. Rev. Lett.}, title = {Fluctuation-induced bistability of fermionic atoms coupled to a dissipative cavity}, volume = {134}, year = {2025}, }
• (2025). Dynamical excitation control and multimode emission of an atom-photon bound state. PRL, 134(13), 133601. (www)

  @article{ , abstract = {Atom-photon bound states arise from the coupling of quantum emitters to the band edge of dispersion-engineered waveguides. Thanks to their tunable-range interactions, they are promising building blocks for quantum simulators. Here, we study the dynamics of an atom-photon bound state emerging from coupling a frequency-tunable quantum emitter—a transmon-type superconducting circuit—to the band edge of a microwave metamaterial. Employing precise temporal control over the frequency detuning of the emitter from the band edge, we examine the transition from adiabatic to nonadiabatic behavior in the formation of the bound state and its melting into the propagating modes of the metamaterial. Moreover, we experimentally observe multimode emission from the bound state, triggered by a fast change of the emitter’s frequency. Our Letter offers insight into the dynamic preparation of APBS and provides a method to characterize their photonic content, with implications in quantum optics and quantum simulation.}, archive = {J_PRL}, author = {Claudia Castillo-Moreno and Kazi Rafsanjani Amin and Ingrid Strandberg and Mikael Kervinen and Amr Osman and Simone Gasparinetti}, doi = {10.1103/PhysRevLett.134.133601}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {133601}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical excitation control and multimode emission of an atom-photon bound state}, volume = {134}, year = {2025}, }
• (2025). Autoionization-enhanced rydberg dressing by fast contaminant removal. PRL, 134(13), 133201. (www)

  @article{ , abstract = {Rydberg dressing is a powerful tool for entanglement generation in long-lived atomic states. While already employed effectively in several demonstrations, a key challenge for this technique is the collective loss triggered by blackbody-radiation-driven transitions to contaminant Rydberg states of opposite parity. We demonstrate the rapid removal of such contaminants using autoionization (AI) transitions found in alkaline-earth-like atoms. The AI is shown to be compatible with coherent operation of an array of optical clock qubits. By incorporating AI pulses into a stroboscopic Rydberg dressing (SRD) sequence, we enhance lifetimes by an order of magnitude for system sizes of up to 144 atoms, while maintaining an order of magnitude larger duty cycle than previously achieved. To highlight the utility of our approach, we use the AI-enhanced SRD protocol to improve the degree of achieved spin-squeezing during early time dressing dynamics. These results bring Rydberg dressing lifetimes closer to fundamental limits, opening the door to previously infeasible dressing proposals.}, archive = {J_PRL}, author = {Alec Cao and Theodor Lukin Yelin and William J. Eckner and Nelson Darkwah Oppong and Adam M. Kaufman}, doi = {10.1103/PhysRevLett.134.133201}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {133201}, shortjournal = {Phys. Rev. Lett.}, title = {Autoionization-enhanced rydberg dressing by fast contaminant removal}, volume = {134}, year = {2025}, }
• (2025). Quark and gluon momentum fractions in the pion and in the kaon. PRL, 134(13), 131902. (www)

  @article{ , abstract = {We present the full decomposition of the momentum fraction carried by quarks and gluons in the pion and the kaon. We employ three gauge ensembles generated with N f = 2 + 1 + 1 Wilson twisted-mass clover-improved fermions at the physical quark masses. For both mesons we perform a continuum extrapolation directly at the physical pion mass, which allows us to determine for the first time the momentum decomposition at the physical point. We find that the total momentum fraction carried by quarks is 0.575(79) and 0.683(50) and by gluons 0.402(53) and 0.422(67) in the pion and in the kaon, respectively, in the MS ¯ scheme and at the renormalization scale of 2 GeV. Having computed both the quark and gluon contributions in the continuum limit, we find that the momentum sum is 0.984(89) for the pion and 1.13(11) for the kaon, verifying the momentum sum rule.}, archive = {J_PRL}, author = {Extended Twisted Mass Collaboration and Constantia Alexandrou and Simone Bacchio and Martha Constantinou and Joseph Delmar and Jacob Finkenrath and Bartosz Kostrzewa and Marcus Petschlies and Luis Alberto Rodriguez Chacon and Gregoris Spanoudes and Fernanda Steffens and Carsten Urbach and Urs Wenger}, doi = {10.1103/PhysRevLett.134.131902}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {131902}, shortjournal = {Phys. Rev. Lett.}, title = {Quark and gluon momentum fractions in the pion and in the kaon}, volume = {134}, year = {2025}, }
• (2025). Four-loop anomalous dimension of flavor nonsinglet twist-two operator of general lorentz spin in QCD: ζ(3) term. PRL, 134(13), 131901. (www)

  @article{ , abstract = {We consider the anomalous dimension of the flavor nonsinglet twist-two quark operator of arbitrary Lorentz spin N at four loops in QCD and construct its contribution proportional to ζ ( 3 ) in analytic form by applying advanced methods of number theory on the available knowledge of low- N moments. In conjunction with similar results on the ζ ( 5 ) and ζ ( 4 ) contributions, this completes our knowledge of the transcendental part of the considered anomalous dimension. This also provides important constraints on the as-yet elusive all- N form of the rational part. Via Mellin transformation, we thus obtain the exact functional form in x of the respective piece of the nonsinglet Dokshitzer-Gribov-Lipatov-Altarelli-Parisi splitting function at four loops. This allows us to appreciably reduce the theoretical uncertainty in the approximation of that splitting function otherwise amenable from the first few low- N moments.}, archive = {J_PRL}, author = {B. A. Kniehl and V. N. Velizhanin}, doi = {10.1103/PhysRevLett.134.131901}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {131901}, shortjournal = {Phys. Rev. Lett.}, title = {Four-loop anomalous dimension of flavor nonsinglet twist-two operator of general lorentz spin in QCD: ζ(3) term}, volume = {134}, year = {2025}, }
• (2025). Geometric interpretation of timelike entanglement entropy. PRL, 134(13), 131601. (www)

  @article{ , abstract = {Analytic continuations of holographic entanglement entropy in which the boundary subregion extends along a timelike direction have brought a promise of a novel, time-centric probe of the emergence of spacetime. We propose that the bulk carriers of this holographic timelike entanglement entropy are boundary-anchored extremal surfaces probing analytic continuation of holographic spacetimes into complex coordinates. This proposal not only provides a geometric interpretation of all the known cases obtained by direct analytic continuation of closed-form expressions of holographic entanglement entropy of a strip subregion but crucially also opens a window to study holographic timelike entanglement entropy in full generality. We initialize the investigation of complex extremal surfaces anchored on a timelike strip at the boundary of anti-de Sitter black branes. We find multiple complex extremal surfaces and discuss possible principles singling out the physical contribution.}, archive = {J_PRL}, author = {Michal P. Heller and Fabio Ori and Alexandre Serantes}, doi = {10.1103/PhysRevLett.134.131601}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {131601}, shortjournal = {Phys. Rev. Lett.}, title = {Geometric interpretation of timelike entanglement entropy}, volume = {134}, year = {2025}, }
• (2025). Hidden multidimensional modulation side channels in quantum protocols. PRL, 134(13), 130802. (www)

  @article{ , abstract = {Quantum protocols including quantum key distribution and blind quantum computing often require the preparation of quantum states of known dimensions. Here, we show that, rather surprisingly, hidden multidimensional modulation is often performed by practical devices. This violates the dimensional assumption in quantum protocols, thus creating side channels and security loopholes. Our work has important impacts on the security of quantum cryptographic protocols.}, archive = {J_PRL}, author = {Amita Gnanapandithan and Li Qian and Hoi-Kwong Lo}, doi = {10.1103/PhysRevLett.134.130802}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {130802}, shortjournal = {Phys. Rev. Lett.}, title = {Hidden multidimensional modulation side channels in quantum protocols}, volume = {134}, year = {2025}, }
• (2025). Parallel accelerated electron paramagnetic resonance spectroscopy using diamond sensors. PRL, 134(13), 130801. (www)

  @article{ , abstract = {The nitrogen-vacancy (NV) center can serve as a magnetic sensor for electron paramagnetic resonance (EPR) measurements. Benefiting from its atomic size, the diamond chip can integrate a tremendous amount of NV centers to improve the magnetic-field sensitivity. However, EPR spectroscopy using NV ensembles is less efficient due to inhomogeneities in both sensors and targets. Spectral line broadening induced by ensemble averaging is even detrimental to spectroscopy. Here we show a kind of cross-relaxation EPR spectroscopy at zero field, where the sensor is tuned by an amplitude-modulated control field to match the target. The modulation makes detection robust to the sensors inhomogeneity, while zero-field EPR is naturally robust to the targets inhomogeneity. We demonstrate an efficient EPR measurement on an ensemble of ∼ 30 000 NV centers. Our method shows the ability to not only acquire unambiguous EPR spectra of free radicals, but also monitor their spectroscopic dynamics in real time.}, archive = {J_PRL}, author = {Zhehua Huang and Zhengze Zhao and Fei Kong and Zhecheng Wang and Pengju Zhao and Xiangtian Gong and Xiangyu Ye and Ya Wang and Fazhan Shi and Jiangfeng Du}, doi = {10.1103/PhysRevLett.134.130801}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {130801}, shortjournal = {Phys. Rev. Lett.}, title = {Parallel accelerated electron paramagnetic resonance spectroscopy using diamond sensors}, volume = {134}, year = {2025}, }
• (2025). Playing nonlocal games across a topological phase transition on a quantum computer. PRL, 134(13), 130602. (www)

  @article{ , abstract = {Many-body quantum games provide a natural perspective on phases of matter in quantum hardware, crisply relating the quantum correlations inherent in phases of matter to the securing of quantum advantage at a device-oriented task. In this Letter, we introduce a family of multiplayer quantum games for which topologically ordered phases of matter are a resource yielding quantum advantage. Unlike previous examples, quantum advantage persists away from the exactly solvable point and is robust to arbitrary local perturbations, irrespective of system size. We demonstrate this robustness experimentally on Quantinuum’s H1-1 quantum computer by playing the game with a continuous family of randomly deformed toric code states that can be created with constant-depth circuits leveraging midcircuit measurements and unitary feedback. We are thus able to tune through a topological phase transition—witnessed by the loss of robust quantum advantage—on currently available quantum hardware. This behavior is contrasted with an analogous family of deformed Greenberger-Horne-Zeilinger states, for which arbitrarily weak local perturbations destroy quantum advantage in the thermodynamic limit. Finally, we discuss a topological interpretation of the game, which leads to a natural generalization involving an arbitrary number of players.}, archive = {J_PRL}, author = {Oliver Hart and David T. Stephen and Dominic J. Williamson and Michael Foss-Feig and Rahul Nandkishore}, doi = {10.1103/PhysRevLett.134.130602}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {130602}, shortjournal = {Phys. Rev. Lett.}, title = {Playing nonlocal games across a topological phase transition on a quantum computer}, volume = {134}, year = {2025}, }
• (2025). Variational ground-state quantum adiabatic theorem. PRL, 134(13), 130601. (www)

  @article{ , abstract = {We present a variational quantum adiabatic theorem, which states that, under certain assumptions, the adiabatic dynamics projected onto a variational manifold follow the instantaneous variational ground state. We focus on low-entanglement variational manifolds and target Hamiltonians with classical ground states. Despite highly entangled intermediate states along the exact adiabatic path, the variational evolution converges to the target ground state. We demonstrate this approach with several examples that align with our theoretical analysis.}, archive = {J_PRL}, author = {Bojan Žunkovič and Pietro Torta and Giovanni Pecci and Guglielmo Lami and Mario Collura}, doi = {10.1103/PhysRevLett.134.130601}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {130601}, shortjournal = {Phys. Rev. Lett.}, title = {Variational ground-state quantum adiabatic theorem}, volume = {134}, year = {2025}, }
• (2025). Correspondence principle, ergodicity, and finite-time dynamics. PRL, 134(13), 130402. (www)

  @article{ , abstract = {The quantum-classical correspondence stands out as one of the most intriguing challenges in the realm of quantum mechanics. Within the context of quantum chaos, the conventional approach, which relies on spectral statistics to infer distinct classical dynamical properties, fails in typical scenarios, such as slow relaxation processes, dynamical localization, or other deviations from ergodicity. To address this difficulty, we propose a novel approach, the essence of which lies in associating a quantum energy shell with classical finite-time trajectories. Our results extend the knowledge of quantum-classical correspondence, offer explanations for previously conflicting findings, and also bear significance for applications in quantum metrology, sensing, and computation when the determination of the ergodicity degree of the quantum states is in need.}, archive = {J_PRL}, author = {Zhen-Qi Chen and Rui-Hua Ni and Yalei Song and Liang Huang and Jiao Wang and Giulio Casati}, doi = {10.1103/PhysRevLett.134.130402}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {130402}, shortjournal = {Phys. Rev. Lett.}, title = {Correspondence principle, ergodicity, and finite-time dynamics}, volume = {134}, year = {2025}, }
• (2025). Large collective power enhancement in dissipative charging of a quantum battery. PRL, 134(13), 130401. (www)

  @article{ , abstract = {We consider a model for a quantum battery consisting of a collection of N two-level atoms driven by a classical field and decaying to a common reservoir. In the extensive regime, where the energy E scales as N and the fluctuations Δ E / E → 0 , our dissipative charging protocol yields a power proportional to N 2 , a scaling that cannot be achieved in this regime by Hamiltonian protocols. The trade-off for this enhanced charging power is a relative inefficiency since a large fraction of the incoming energy is lost through spontaneous emission to the environment. Nevertheless, we find that the system can store a large amount of coherence and release the stored energy coherently through spontaneous emission, again with a power scaling as N 2 .}, archive = {J_PRL}, author = {Sagar Pokhrel and Julio Gea-Banacloche}, doi = {10.1103/PhysRevLett.134.130401}, journal = {Physical Review Letters}, month = {3}, number = {13}, pages = {130401}, shortjournal = {Phys. Rev. Lett.}, title = {Large collective power enhancement in dissipative charging of a quantum battery}, volume = {134}, year = {2025}, }
• (2025). Erratum: Minimum scaling model and exact exponents for the nambu-goldstone modes in the vicsek model [Phys. rev. lett. 133, 258301 (2024)]. PRL, 134(12), 129901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 129901 (2025)}, archive = {J_PRL}, author = {Harukuni Ikeda}, doi = {10.1103/PhysRevLett.134.129901}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {129901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Minimum scaling model and exact exponents for the nambu-goldstone modes in the vicsek model [Phys. rev. lett. 133, 258301 (2024)]}, volume = {134}, year = {2025}, }
• (2025). Protein structure classification based on X-ray-laser-induced coulomb explosion. PRL, 134(12), 128403. (www)

  @article{ , abstract = {We simulated Coulomb explosion dynamics due to fast ionization induced by high-intensity x-rays in six proteins that share similar atomic content and shape. We followed and projected the trajectory of the fragments onto a virtual detector, providing a unique explosion footprint. After collecting 500 explosion footprints for each protein, we utilized principal component analysis and t -distributed stochastic neighbor embedding to classify these. Results show that the classification algorithms were able to separate proteins on the basis of explosion footprints from structurally similar proteins into distinct groups. The explosion footprints, therefore, provide a unique identifier for each protein. We envision that method could be used concurrently with single-particle coherent imaging experiments to provide additional information on shape, mass, or conformation.}, archive = {J_PRL}, author = {Tomas André and Ibrahim Dawod and Sebastian Cardoch and Emiliano De Santis and Nicuşor Tîmneanu and Carl Caleman}, doi = {10.1103/PhysRevLett.134.128403}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128403}, shortjournal = {Phys. Rev. Lett.}, title = {Protein structure classification based on X-ray-laser-induced coulomb explosion}, volume = {134}, year = {2025}, }
• (2025). Self-organized coexistence of phage and a population of host colonies. PRL, 134(12), 128402. (www)

  @article{ , abstract = {Phages and bacteria coexist under widely different conditions, ranging from liquid cultures to oceans, soil, and the human gut. However, our models are typically limited to well-mixed liquid cultures governed by mass-action kinetics. Here, we suggest a modification to the Lotka-Volterra dynamics by including the formation of microcolonies. By analyzing the model in an open system with a steady influx of bacteria, we predict that the colony size distribution is power-low distributed with steeper exponents for the stronger external influx. In the realistic case where the phage attack rate to individual colonies is proportional to their radius, we obtain self-organization to a steady state where the maximal colony size is smaller for stronger external driving.}, archive = {J_PRL}, author = {Anjali Yadav and Namiko Mitarai and Kim Sneppen}, doi = {10.1103/PhysRevLett.134.128402}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128402}, shortjournal = {Phys. Rev. Lett.}, title = {Self-organized coexistence of phage and a population of host colonies}, volume = {134}, year = {2025}, }
• (2025). Active loop extrusion guides DNA-protein condensation. PRL, 134(12), 128401. (www)

  @article{ , abstract = {The spatial organization of DNA involves DNA loop extrusion and the formation of protein-DNA condensates. While the significance of each process is increasingly recognized, their interplay remains unexplored. Using molecular dynamics simulation and theory we investigate this interplay. Our findings reveal that loop extrusion can enhance the dynamics of condensation and promotes coalescence and ripening of condensates. Further, the DNA loop enables condensate formation under DNA tension and position condensates. The concurrent presence of loop extrusion and condensate formation results in the formation of distinct domains similar to TADs, an outcome not achieved by either process alone.}, archive = {J_PRL}, author = {Ryota Takaki and Yahor Savich and Jan Brugués and Frank Jülicher}, doi = {10.1103/PhysRevLett.134.128401}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128401}, shortjournal = {Phys. Rev. Lett.}, title = {Active loop extrusion guides DNA-protein condensation}, volume = {134}, year = {2025}, }
• (2025). Quasi-long-ranged order in two-dimensional active liquid crystals. PRL, 134(12), 128304. (www)

  @article{ , abstract = {Quasi-long-ranged order is the hallmark of two-dimensional liquid crystals. At equilibrium, this property implies that the correlation function of the local orientational order parameter decays with distance as a power law: i.e., ∼ | r | − η p , with η p a temperature-dependent exponent. While in general nonuniversal, η p = 1 / 4 universally at the Berezinskii-Kosterlitz-Thouless transition, where orientational order is lost because of the unbinding of disclinations. Here, we demonstrate that, in active liquid crystals, the notion of quasi-long-ranged order fundamentally differs from its equilibrium counterpart, and the exponent η p is allowed to vary in the range 0 < η p ≤ 2 , with the upper bound corresponding to the isotropic phase. Our theoretical predictions are supported by a survey of a variety of experimental realizations of two-dimensional active liquid crystals.}, archive = {J_PRL}, author = {Livio Nicola Carenza and Josep-Maria Armengol-Collado and Dimitrios Krommydas and Luca Giomi}, doi = {10.1103/PhysRevLett.134.128304}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128304}, shortjournal = {Phys. Rev. Lett.}, title = {Quasi-long-ranged order in two-dimensional active liquid crystals}, volume = {134}, year = {2025}, }
• (2025). Locomotion of active polymerlike worms in porous media. PRL, 134(12), 128303. (www)

  @article{ , abstract = {We investigate the locomotion of thin, living T. Tubifex worms, which display active polymerlike behavior, within quasi-2D arrays of cylindrical pillars, examining varying spatial arrangements and densities. These active worms spread in crowded environments, with a dynamics dependent on both the concentration and arrangement of obstacles. In contrast to passive polymers, our results reveal that in disordered configurations, increasing the pillar density enhances the long-time diffusion of our active polymerlike worms, while we observe the opposite trend in ordered pillar arrays. We found that in disordered media, living worms reptate through available curvilinear tubes, whereas they become trapped within pores of ordered media. Intriguingly, we show that reducing the worm’s activity significantly boosts its spread, enabling passive sorting of worms by activity level. Our experimental observations are corroborated through simulations of the tangentially driven polymer model with matched persistence length predicting the same trends.}, archive = {J_PRL}, author = {R. Sinaasappel and M. Fazelzadeh and T. Hooijschuur and Q. Di and S. Jabbari-Farouji and A. Deblais}, doi = {10.1103/PhysRevLett.134.128303}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128303}, shortjournal = {Phys. Rev. Lett.}, title = {Locomotion of active polymerlike worms in porous media}, volume = {134}, year = {2025}, }
• (2025). Cooperativity of confined nematic microswimmers: From one to many. PRL, 134(12), 128302. (www)

  @article{ , abstract = {Controlling the behavior of microswimmers is a major challenge to extract work for novel active matter applications. Geometric confinement is often used for controlling soft matter systems. However, in comparison to the case of Newtonian fluids, the effects of solid interfaces on microswimmers moving through an anisotropic fluid are far less understood. By means of nematic multiparticle collision dynamics simulations and analytical modeling, we investigate the dynamical behavior of swimmers immersed in a nematic liquid crystal and confined by solid walls. For isolated squirmers, we find a rich phase diagram including oscillatory dynamics for weak pushers, depending on the strength of their propulsion and degree of confinement. Our theoretical model shows that, unlike in the isotropic case, in a nematic fluid, force dipole, source dipole, and source quadrupole singularities all are required for the onset of oscillations. Increasing the number of squirmers shows the emergence of cooperativity in pusher-type squirmers, while pullers’ flow fields hinder each other’s motion. The interplay of nematodynamic torque, wall-induced elastic repulsion, and active flows thus offers the opportunity for both control and transport in active nematic systems.}, archive = {J_PRL}, author = {Shubhadeep Mandal and Thomas J. Mason and Anthony C. Croft and Marco G. Mazza}, doi = {10.1103/PhysRevLett.134.128302}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128302}, shortjournal = {Phys. Rev. Lett.}, title = {Cooperativity of confined nematic microswimmers: From one to many}, volume = {134}, year = {2025}, }
• (2025). Active saffman-taylor viscous fingering. PRL, 134(12), 128301. (www)

  @article{ , abstract = {Adding swimming bacteria to a liquid causes its effective shear viscosity to decrease, eventually reaching a regime of zero viscosity. We examined whether this property leads to viscous fingerlike displacement fronts like those observed when a less viscous fluid displaces a more viscous liquid. Our study revealed that this system exhibits more complex dynamic characteristics than the classical Saffman-Taylor instability. We discovered that this instability occurs when the bacterial volume fraction exceeds a critical value and the imposed shear rate is below critical value, for which the viscosity of the suspension is zero.}, archive = {J_PRL}, author = {Akash Ganesh and Carine Douarche and Harold Auradou}, doi = {10.1103/PhysRevLett.134.128301}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128301}, shortjournal = {Phys. Rev. Lett.}, title = {Active saffman-taylor viscous fingering}, volume = {134}, year = {2025}, }
• (2025). Generating ultrastable glasses by homogenizing the local virial stress. PRL, 134(12), 128201. (www)

  @article{ , abstract = {The algorithmic preparation of ultrastable glasses (UG) has considerably expanded our understanding of the glassy state. In this work, we report on a new protocol for UG preparation in a model colloidal glass that iteratively modifies particle diameters to reduce local virial stress fluctuations, effectively homogenizing the local mechanical environment of individual particles. We apply the algorithm to an additive Lennard-Jones mixture and show that, compared to the states obtained via thermal annealing, virial homogenized glasses are characterized by a considerable increase in both kinetic stability and the number of locally favored structures, and melt during heating ramps via an accumulation of localized events. Our results show that microscopic mechanical homogeneity, a widely applicable concept, can give rise to ultrastability.}, archive = {J_PRL}, author = {Fabio Leoni and John Russo and Francesco Sciortino and Taiki Yanagishima}, doi = {10.1103/PhysRevLett.134.128201}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {128201}, shortjournal = {Phys. Rev. Lett.}, title = {Generating ultrastable glasses by homogenizing the local virial stress}, volume = {134}, year = {2025}, }
• (2025). Universal and nonuniversal signatures in the scaling functions of critical variables. PRL, 134(12), 127102. (www)

  @article{ , abstract = {At criticality, the magnetization M of a d -dimensional Ising system with N spins is distributed such that the probability density function of m = M / N y H / d , with y H universal exponent, converges to a limit f ( m ) . The expectation that f should furnish a hallmark of universal behavior contrasts with its sensible dependence on nonuniversal features. We show that both nonuniversal amplitudes and universal exponents of leading power law singularities in all large deviation functions are determined by the fact that, due to extensivity, f ( m ) ∼ | m | ≫ 1 exp ( − c | m | δ + 1 ) , with δ = y H / ( d − y H ) and c a nonuniversal coefficient. This unexplored scenario implies a universal form of central limit theorem at criticality and is confirmed by exact calculations for mean field Ising models in equilibrium and for anomalous diffusion models, with M replaced by displacement and N by time.}, archive = {J_PRL}, author = {Gianluca Teza and Attilio L. Stella}, doi = {10.1103/PhysRevLett.134.127102}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {127102}, shortjournal = {Phys. Rev. Lett.}, title = {Universal and nonuniversal signatures in the scaling functions of critical variables}, volume = {134}, year = {2025}, }
• (2025). First passage times in compact domains exhibit biscaling. PRL, 134(12), 127101. (www)

  @article{ , abstract = {The study of first passage time for diffusing particles reaching target states is foundational in various practical applications, including diffusion-controlled reactions. In large systems, first passage times statistics exhibit a biscaling behavior, challenging the use of a single timescale. In this work, we present a biscaling theory for the probability density function of first passage times in confined compact processes, applicable to both Euclidean and fractal domains and for diverse geometries. Our theory employs two distinct scaling functions: one for short times, capturing initial dynamics in unbounded systems, and the other for long times, which is sensitive to finite size effects. The combined framework is argued to provide a complete expression for first passage time statistics across all timescales. As our detailed calculations show, the theory describes various scenarios with and without external force fields, for active and thermal settings, and in the presence of resetting when a nonequilibrium steady state emerges.}, archive = {J_PRL}, author = {Talia Baravi and David A. Kessler and Eli Barkai}, doi = {10.1103/PhysRevLett.134.127101}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {127101}, shortjournal = {Phys. Rev. Lett.}, title = {First passage times in compact domains exhibit biscaling}, volume = {134}, year = {2025}, }
• (2025). Direct measurement of the lifetime and coherence time of Cu2O rydberg excitons. PRL, 134(12), 126902. (www)

  @article{ , abstract = {Rydberg states of excitons are promising quantum objects to engineer giant nonlinearities in a solid-state system. For this purpose, a deeper understanding of the dynamics of Rydberg excitons and of their potential for coherent manipulation becomes important. We report experimental results where two-photon absorption is resonant with various Rydberg states of excitons in copper oxide and we detect their emission dynamics on a streak camera with subpicosecond resolution. This technique enables the direct measurement of the Rydberg states lifetimes, which are in good agreement with the expected Rydberg scaling law. Moreover, we observe several intriguing dynamics including the presence of long-lived coherent oscillations. Finally, we independently measure the coherence time of the Rydberg states using a modified Michelson interferometer and find a good agreement with the coherent oscillations detected in the exciton emission dynamics. The lifetimes also reveal the absence of inhomogeneous broadening in the current high-precision spectroscopic data for the S series, which together with the presence of significant coherence time confirms the suitability of the system for coherent engineering.}, archive = {J_PRL}, author = {Poulab Chakrabarti and Kerwan Morin and Delphine Lagarde and Xavier Marie and Thomas Boulier}, doi = {10.1103/PhysRevLett.134.126902}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126902}, shortjournal = {Phys. Rev. Lett.}, title = {Direct measurement of the lifetime and coherence time of Cu2O rydberg excitons}, volume = {134}, year = {2025}, }
• (2025). Superradiance of strongly interacting dipolar excitons in moiré quantum materials. PRL, 134(12), 126901. (www)

  @article{ , abstract = {Moiré lattices created in two-dimensional heterostructures exhibit rich many-body physics of interacting electrons and excitons and, at the same time, suggest promising optoelectronic applications. Here, we study the cooperative radiance of moiré excitons that is demonstrated to emerge from the deep subwavelength nature of the moiré lattice and the strong excitonic on-site interaction. In particular, we show that the static dipole-dipole interaction between interlayer excitons can strongly affect their cooperative optical properties, suppressing superradiance of disordered states while enhancing superradiance of ordered phases of moiré excitons. Moreover, we show that doping permits direct control of optical cooperativity, e.g., by generating superradiant dynamics of otherwise subradiant states of excitons. Our results show that interlayer moiré excitons offer a unique platform for exploring cooperative optical phenomena in strongly interacting many-body systems, thus holding promise for applications in quantum nonlinear optics.}, archive = {J_PRL}, author = {Jan Kumlin and Ajit Srivastava and Thomas Pohl}, doi = {10.1103/PhysRevLett.134.126901}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126901}, shortjournal = {Phys. Rev. Lett.}, title = {Superradiance of strongly interacting dipolar excitons in moiré quantum materials}, volume = {134}, year = {2025}, }
• (2025). Dynamically tunable magnon-magnon coupling in a perpendicular anisotropy magnetic garnet-ferromagnet bilayer. PRL, 134(12), 126702. (www)

  @article{ , abstract = {We experimentally explore the interfacial coherent spin pumping in the magnon-magnon hybridized regime of a perpendicular anisotropy ferrimagnetic insulator (Bi-substituted yttrium iron garnet, or BiYIG) and ferromagnetic metal (permalloy, or Py) bilayer. In addition to the interfacial exchange coupling-induced avoided crossings between the uniform modes of BiYIG and Py, we observe that the gap opening can be tailored by changing the relative orientations of the BiYIG and Py magnetizations due to a purely dynamic interaction. The avoided-crossing gap opening is small (large) when BiYIG and Py magnetizations are nearly perpendicular (partially collinear) to each other, indicating that interfacial fieldlike torque from spin pumping plays a dominant role. Macrospin simulations with a sizable fieldlike spin-pumping torque agree with the gap opening trend observed in the experiments.}, archive = {J_PRL}, author = {Yabin Fan and Takian Fakhrul and Justin T. Hou and Chung-Tao Chou and Bharat Khurana and Yaroslav Tserkovnyak and Luqiao Liu and Caroline A. Ross}, doi = {10.1103/PhysRevLett.134.126702}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126702}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamically tunable magnon-magnon coupling in a perpendicular anisotropy magnetic garnet-ferromagnet bilayer}, volume = {134}, year = {2025}, }
• (2025). Orbital pumping in ferrimagnetic insulators. PRL, 134(12), 126701. (www)

  @article{ , abstract = {We report the detection of pure orbital currents generated by both coherent and thermal magnons in the magnetic insulator Bi-doped yttrium iron garnet (BiYIG). The pumping of orbital and spin currents is jointly investigated in nanodevices made of naturally oxidized Cu, pure Cu, Pt, and Cr. The absence of charge conduction in BiYIG and the negligible spin-to-charge conversion of oxidized Cu allows us to disambiguate the orbital current contribution. Comparative measurements on YIG and BiYIG show that the origin of the orbital pumping in BiYIG/oxidized Cu is the dynamics of the orbital magnetization in the magnetic insulator. In Cr, the pumping signal is dominated by the negative spin Hall effect rather than the positive orbital Hall effect, indicating that orbital currents represent a minority of the total angular momentum current pumped from the magnetic insulator. Our results also evidence that improving the interfacial transparency significantly enhances pumping efficiencies, not only for spin but also for orbital currents.}, archive = {J_PRL}, author = {Hanchen Wang and Min-Gu Kang and Davit Petrosyan and Shilei Ding and Richard Schlitz and Lauren J. Riddiford and William Legrand and Pietro Gambardella}, doi = {10.1103/PhysRevLett.134.126701}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126701}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital pumping in ferrimagnetic insulators}, volume = {134}, year = {2025}, }
• (2025). Observation of floquet-bloch braids in non-hermitian spatiotemporal lattices. PRL, 134(12), 126603. (www)

  @article{ , abstract = {The formation of nontrivial braid structures of complex energies enables a new topological classification beyond conventional topological band theory. In this Letter, we introduce the concept of braiding topology to dynamic systems and reveal novel Floquet-Bloch braids in non-Hermitian spatiotemporal lattices. This nonequilibrium braiding topology, closely related to the breakdown of continuous time translation symmetry, is characterized by an invariant derived from Floquet operators. In sharp contrast to static lattices, the Floquet-Bloch braids can be directly manipulated using temporal engineering, enabling an arbitrary braiding degree even in a two-band lattice without long-range hopping. Experimentally, we synthesize Floquet-Bloch bands in an acoustic platform with time-modulated unidirectional couplers. We not only realize a series of Floquet-Bloch braids with distinct topologies, but also observe the transition states featuring state-coalesced Floquet exceptional points. Our findings reveal a fundamental interplay between non-Hermiticity and Floquet engineering, and pave the way for experimentally exploring the rich and uncharted territory of nonequilibrium non-Hermitian physics.}, archive = {J_PRL}, author = {Shuaishuai Tong and Qicheng Zhang and Liangjun Qi and Gaohan Li and Xiling Feng and Chunyin Qiu}, doi = {10.1103/PhysRevLett.134.126603}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126603}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of floquet-bloch braids in non-hermitian spatiotemporal lattices}, volume = {134}, year = {2025}, }
• (2025). Anomalous hall effect due to magnetic fluctuations in a ferromagnetic weyl semimetal. PRL, 134(12), 126602. (www)

  @article{ , abstract = {The anomalous Hall effect (AHE) has emerged as a key indicator of time-reversal symmetry breaking (TRSB) and topological features in electronic band structures. Absent of a magnetic field, the AHE requires spontaneous TRSB but has proven hard to probe due to averaging over domains. The anomalous component of the Hall effect is thus frequently derived from extrapolating the magnetic field dependence of the Hall response. We show that discerning whether the AHE is an intrinsic property of the field-free system becomes intricate in the presence of strong magnetic fluctuations. As a study case, we use the Weyl semimetal PrAlGe, where TRSB can be toggled via a ferromagnetic transition, providing a transparent view of the AHE’s topological origin. Through a combination of thermodynamic, transport, and muon spin relaxation measurements, we contrast the behavior below the ferromagnetic transition temperature to that of strong magnetic fluctuations above. Our results on PrAlGe provide general insights into the interpretation of anomalous Hall signals in systems where TRSB is debated, such as families of kagome metals or certain transition metal dichalcogenides.}, archive = {J_PRL}, author = {Ola Kenji Forslund and Xiaoxiong Liu and Soohyeon Shin and Chun Lin and Masafumi Horio and Qisi Wang and Kevin Kramer and Saumya Mukherjee and Timur Kim and Cephise Cacho and Chennan Wang and Tian Shang and Victor Ukleev and Jonathan S. White and Pascal Puphal and Yasmine Sassa and Ekaterina Pomjakushina and Titus Neupert and Johan Chang}, doi = {10.1103/PhysRevLett.134.126602}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126602}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous hall effect due to magnetic fluctuations in a ferromagnetic weyl semimetal}, volume = {134}, year = {2025}, }
• (2025). Topological phenomena in artificial quantum materials revealed by local chern markers. PRL, 134(12), 126601. (www)

  @article{ , abstract = {A striking example of frustration in physics is Hofstadter’s butterfly, a fractal structure that emerges from the competition between a crystal’s lattice periodicity and the magnetic length of an applied field. Current methods for predicting the topological invariants associated with Hofstadter’s butterfly are challenging or impossible to apply to a range of materials, including those that are disordered or lack a bulk spectral gap. Here, we demonstrate a framework for predicting a material’s local Chern markers using its position-space description and validate it against experimental observations of quantum transport in artificial graphene in a semiconductor heterostructure, inherently accounting for fabrication disorder strong enough to close the bulk spectral gap. By resolving local changes in the system’s topology, we reveal the topological origins of antidot-localized states that appear in artificial graphene in the presence of a magnetic field. Moreover, we show the breadth of this framework by simulating how Hofstadter’s butterfly emerges from an initially unpatterned 2D electron gas as the system’s potential strength is increased and predict that artificial graphene becomes a topological insulator at the critical magnetic field. Overall, we anticipate that a position-space approach to determine a material’s Chern invariant without requiring prior knowledge of its occupied states or bulk spectral gaps will enable a broad array of fundamental inquiries and provide a novel route to material discovery, especially in metallic, aperiodic, and disordered systems.}, archive = {J_PRL}, author = {Catalin D. Spataru and Wei Pan and Alexander Cerjan}, doi = {10.1103/PhysRevLett.134.126601}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126601}, shortjournal = {Phys. Rev. Lett.}, title = {Topological phenomena in artificial quantum materials revealed by local chern markers}, volume = {134}, year = {2025}, }
• (2025). Unusual energy spectra of matrix product states. PRL, 134(12), 126503. (www)

  @article{ , abstract = {In approximate ground states obtained from imaginary-time evolution, the spectrum of the state—its decomposition into exact energy eigenstates—falls off exponentially with the energy. Here we consider the energy spectra of approximate matrix product ground states, such as those obtained with the density matrix renormalization group. Despite the high accuracy of these states, contributions to the spectra are roughly constant out to surprisingly high energy, with an increase in the bond dimension reducing the amplitude but not the extent of these high-energy tails. The unusual spectra appear to be a general feature of compressed wavefunctions, independent of boundary or dimensionality, and are also observed in neural network wavefunctions. The unusual spectra can have a strong effect on sampling-based methods, yielding large fluctuations. The energy variance, which can be used to extrapolate observables to eliminate truncation error, is subject to these large fluctuations when sampled. Nevertheless, we devise a sampling-based variance approach which gives excellent and efficient extrapolations.}, archive = {J_PRL}, author = {J. Maxwell Silvester and Giuseppe Carleo and Steven R. White}, doi = {10.1103/PhysRevLett.134.126503}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126503}, shortjournal = {Phys. Rev. Lett.}, title = {Unusual energy spectra of matrix product states}, volume = {134}, year = {2025}, }
• (2025). Tuning transport in solid-state bose-fermi mixtures by feshbach resonances. PRL, 134(12), 126502. (www)

  @article{ , abstract = {Transition-metal-dichalcogenide heterostructures have emerged as promising platforms for realizing tunable Bose–Fermi mixtures. Their constituents are fermionic charge carriers resonantly coupled to long-lived bosonic interlayer excitons, allowing them to form trion bound states. Such platforms promise to achieve comparable densities of fermions and bosons at low relative temperatures. Here, we predict the transport properties of correlated Bose–Fermi mixtures close to a narrow solid-state Feshbach resonance. When driving a hole current, the responses of doped holes, excitons, and trions are significantly modified by the resonant interactions, leading to deviations from the typical Drude behavior and to a sign change of the exciton drag. Our results on the temperature-dependent resistivities demonstrate that near resonance interaction effects dominate over established conventional scattering mechanisms in these solid-state Bose–Fermi mixtures.}, archive = {J_PRL}, author = {Caterina Zerba and Clemens Kuhlenkamp and Léo Mangeolle and Michael Knap}, doi = {10.1103/PhysRevLett.134.126502}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126502}, shortjournal = {Phys. Rev. Lett.}, title = {Tuning transport in solid-state bose-fermi mixtures by feshbach resonances}, volume = {134}, year = {2025}, }
• (2025). Quasiparticle interference in kitaev quantum spin liquids. PRL, 134(12), 126501. (www)

  @article{ , abstract = {We study quasiparticle interference (QPI) in the Kitaev quantum spin liquid (QSL) for electrons tunneling into the QSL. The local tunneling conductance around a spin vacancy or localized vison reveals unique features associated with fractionalized Majorana fermions, chargons, and visons. In certain parameter regimes, the single-spinon density of states and momentum dispersion can both be directly extracted from the tunneling conductance. Our results suggest that QPI is a promising tool for identifying the Kitaev QSL and its fractionalized excitations.}, archive = {J_PRL}, author = {Ammar Jahin and Hao Zhang and Gábor B. Halász and Shi-Zeng Lin}, doi = {10.1103/PhysRevLett.134.126501}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126501}, shortjournal = {Phys. Rev. Lett.}, title = {Quasiparticle interference in kitaev quantum spin liquids}, volume = {134}, year = {2025}, }
• (2025). Electronic structure dimensionality of the quantum-critical ferromagnet YbNi4P2. PRL, 134(12), 126401. (www)

  @article{ , abstract = {is the first known ferromagnetic metal showing a second-order quantum phase transition. Current theoretical understanding rules out second-order ferromagnetic quantum criticality in centrosymmetric two- and three-dimensional (2D and 3D) metals. Thus, studying the electronic structure of is of prime fundamental importance. Using angle-resolved photoemission spectroscopy, we experimentally prove the existence of 1D Fermi surface contours. In addition, our results demonstrate that part of the electronic structure of is made of states of higher dimensionality, thereby bringing into question the fact that ferromagnetic quantum criticality in centrosymmetric crystals is exclusively found in 1D systems. Our experimental data show that the electronic structure of is a playground of mixed dimensionality, electron correlations, strong hybridization, and spin-orbit coupling, all of them providing new insights in understanding the origin of ferromagnetic quantum criticality.}, archive = {J_PRL}, author = {J. Dai and A. Antezak and W. Broad and M. Thees and V. Zatko and R. L. Bouwmeester and F. Fortuna and P. Le Fèvre and J. E. Rault and K. Horiba and D. V. Vyalikh and H. Kumigashira and K. Kliemt and S. Friedemann and C. Krellner and E. Frantzeskakis and A. F. Santander-Syro}, doi = {10.1103/PhysRevLett.134.126401}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126401}, shortjournal = {Phys. Rev. Lett.}, title = {Electronic structure dimensionality of the quantum-critical ferromagnet YbNi4P2}, volume = {134}, year = {2025}, }
• (2025). Negative transit time in nontunneling electron transmission through graphene multilayers. PRL, 134(12), 126302. (www)

  @article{ , abstract = {Attosecond dynamics of electron transmission through atomically thin crystalline films is studied with an ab initio scattering theory. The temporal character of the electron propagation through graphene multilayers is traced to the band structure of bulk graphite: In the forbidden gaps the wave packet transit time τ T saturates with thickness and in the allowed bands τ T oscillates following transmission resonances. Hitherto unknown negative transit time due to in-plane scattering is discovered in monolayers of graphene, h-BN, and oxygen. Moreover, Wigner time delay is found to diverge at the scattering resonances caused by the emergence of secondary diffracted beams. This offers a way to manipulate the propagation timing of the wave packet without sacrificing the transmitted intensity. The spatial reshaping of the wave packet at the resonances may help elucidate details of the streaking by an inhomogeneous field at the surface.}, archive = {J_PRL}, author = {E. E. Krasovskii and R. O. Kuzian}, doi = {10.1103/PhysRevLett.134.126302}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126302}, shortjournal = {Phys. Rev. Lett.}, title = {Negative transit time in nontunneling electron transmission through graphene multilayers}, volume = {134}, year = {2025}, }
• (2025). Disorder-induced delocalization in magic-angle twisted bilayer graphene. PRL, 134(12), 126301. (www)

  @article{ , abstract = {Flat bands in moiré systems are exciting new playgrounds for the generation and study of exotic many-body physics phenomena in low-dimensional materials. Such physics is attributed to the vanishing kinetic energy and strong spatial localization of the flat-band states. Here, we use numerical simulations to examine the electronic transport properties of such flat bands in magic-angle twisted bilayer graphene in the presence of disorder. We find that while a conventional downscaling of the mean free path with increasing disorder strength occurs at higher energies, in the flat bands the mean free path can actually increase with increasing disorder strength. This phenomenon is also captured by the disorder-dependent quantum metric, which is directly linked to the ground state localization. This disorder-induced delocalization suggests that weak disorder may have a strong impact on the exotic physics of magic-angle bilayer graphene and other related moiré systems.}, archive = {J_PRL}, author = {Pedro Alcázar Guerrero and Viet-Hung Nguyen and Jorge Martínez Romeral and Aron W. Cummings and José-Hugo Garcia and Jean-Christophe Charlier and Stephan Roche}, doi = {10.1103/PhysRevLett.134.126301}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126301}, shortjournal = {Phys. Rev. Lett.}, title = {Disorder-induced delocalization in magic-angle twisted bilayer graphene}, volume = {134}, year = {2025}, }
• (2025). Giant negative linear compressibility in orthorhombic copper cyanide. PRL, 134(12), 126102. (www)

  @article{ , abstract = {Most reported negative linear compressibility (NLC) materials exhibit either a small NLC over a large pressure range or a high NLC over a very small pressure range. Here, we report the remarkable discovery of giant NLC in the low-temperature form of CuCN (LT-CuCN) over an unusually large pressure range. High-pressure XRD studies on LT-CuCN observed the NLC of − 2 0.5 TPa − 1 along the a axis at zero pressure, and the ambient orthorhombic phase remained stable up to 9.8 GPa. Pressure- and temperature-dependent Raman studies identified the phonon vibrations responsible for NLC and negative thermal expansion (NTE).}, archive = {J_PRL}, author = {Swayam Kesari and Alka B. Garg and Nilesh P. Salke and Rekha Rao}, doi = {10.1103/PhysRevLett.134.126102}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126102}, shortjournal = {Phys. Rev. Lett.}, title = {Giant negative linear compressibility in orthorhombic copper cyanide}, volume = {134}, year = {2025}, }
• (2025). Crystallization instead of amorphization in collision cascades in gallium oxide. PRL, 134(12), 126101. (www)

  @article{ , abstract = {Disordering of solids often leads to amorphization, but polymorph transitions, facilitated by favorable atomic rearrangements, may temporarily help to maintain long-range periodicity in the solid state. In far-from-equilibrium situations, such as atomic collision cascades, these rearrangements may not necessarily follow a thermodynamically gainful path, but may be kinetically limited. In this Letter, we focus on such crystallization instead of amorphization in collision cascades in gallium oxide ( ). We determine the disorder threshold for irreversible polymorph transition and explained why it results in elevating energy to that of the polymorph, which exhibits the highest polymorph energy in the system below the amorphous state. Specifically, we demonstrate that upon reaching the disorder transition threshold, the Ga sublattice kinetically favors transitioning to the -like configuration, requiring significantly less migration for Ga atoms to reach the lattice sites during postcascade processes. As such, our data provide a consistent explanation of this remarkable phenomenon and can serve as a toolbox for predictive multipolymorph fabrication.}, archive = {J_PRL}, author = {Junlei Zhao and Javier García Fernández and Alexander Azarov and Ru He and Øystein Prytz and Kai Nordlund and Mengyuan Hua and Flyura Djurabekova and Andrej Kuznetsov}, doi = {10.1103/PhysRevLett.134.126101}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126101}, shortjournal = {Phys. Rev. Lett.}, title = {Crystallization instead of amorphization in collision cascades in gallium oxide}, volume = {134}, year = {2025}, }
• (2025). Electronic structure of the alternating monolayer-trilayer phase of La3Ni2O7. PRL, 134(12), 126001. (www)

  @article{ , abstract = {Recent studies of have identified a bilayer (2222) structure and an unexpected alternating monolayer-trilayer (1313) structure, both of which feature signatures of superconductivity near 80 K under high pressures. Using angle-resolved photoemission spectroscopy, we measure the electronic structure of 1313 samples. In contrast to the previously studied 2222 structure, we find that the 1313 structure hosts a flat band with a markedly different binding energy, as well as an additional electron pocket and band splittings. By comparison to local-density approximation calculations, we find renormalizations of the and derived bands to be about 5 to 7 and about 4, respectively, suggesting strong correlation effects. These results reveal important differences in the electronic structure brought about by the distinct structural motifs with the same stoichiometry. Such differences may be relevant to the putative high temperature superconductivity.}, archive = {J_PRL}, author = {Sebastien Abadi and Ke-Jun Xu and Eder G. Lomeli and Pascal Puphal and Masahiko Isobe and Yong Zhong and Alexei V. Fedorov and Sung-Kwan Mo and Makoto Hashimoto and Dong-Hui Lu and Brian Moritz and Bernhard Keimer and Thomas P. Devereaux and Matthias Hepting and Zhi-Xun Shen}, doi = {10.1103/PhysRevLett.134.126001}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {126001}, shortjournal = {Phys. Rev. Lett.}, title = {Electronic structure of the alternating monolayer-trilayer phase of La3Ni2O7}, volume = {134}, year = {2025}, }
• (2025). Biermann-battery-driven magnetized collisionless shock precursors in laser-produced plasmas. PRL, 134(12), 125101. (www)

  @article{ , abstract = {This Letter reports the first complete observation of magnetized collisionless shock precursors formed through the compression of Biermann-battery magnetic fields in laser produced plasmas. At OMEGA, lasers produce a supersonic CH plasma flow which is magnetized with Biermann-battery magnetic fields. The plasma flow collides with an unmagnetized hydrogen gas jet plasma to create a magnetized shock precursor. The situation where the flowing plasma carries the magnetic field is similar to the Venusian bow shock. Imaging 2 ω Thomson scattering confirms that the interaction is collisionless and shows density and temperature jumps. Proton radiographs have regions of strong deflections and FLASH magnetohydrodynamic (MHD) simulations show the presence of Biermann fields in the Thomson scattering region. Electrons are accelerated to energies of up to 100 keV in a power-law spectrum. OSIRIS particle-in-cell (PIC) simulations, initialized with measured parameters, show the formation of a magnetized shock precursor and corroborate the experimental observables.}, archive = {J_PRL}, author = {T. M. Johnson and G. D. Sutcliffe and J. A. Pearcy and A. Birkel and G. Rigon and N. V. Kabadi and B. Lahmann and P. J. Adrian and B. L. Reichelt and J. H. Kunimune and S. G. Dannhoff and M. Cufari and C. K. Li and F. Tsung and H. Chen and J. Katz and V. T. Tikhonchuk}, doi = {10.1103/PhysRevLett.134.125101}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {125101}, shortjournal = {Phys. Rev. Lett.}, title = {Biermann-battery-driven magnetized collisionless shock precursors in laser-produced plasmas}, volume = {134}, year = {2025}, }
• (2025). 4D topological textures in light. PRL, 134(12), 123805. (www)

  @article{ , abstract = {We present 4D topological textures in (quasi)monochromatic nonparaxial optical lattices that contain all possible polarization ellipses with every combination of ellipticity and orientation in 3D space. These fields span the nonparaxial polarization space (a complex projective plane) and a 4-sphere within specific spatiotemporal regions, forming 4D skyrmionic structures. Constructed from five plane waves with adiabatically varying relative amplitudes, they are experimentally realizable in free space by focusing a temporally variant beam with a high numerical aperture lens.}, archive = {J_PRL}, author = {David Marco and Miguel A. Alonso}, doi = {10.1103/PhysRevLett.134.123805}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123805}, shortjournal = {Phys. Rev. Lett.}, title = {4D topological textures in light}, volume = {134}, year = {2025}, }
• (2025). Free-space optical modulation of free electrons in the continuous-wave regime. PRL, 134(12), 123804. (www)

  @article{ , abstract = {The coherent interaction between free electrons and optical fields can produce free-electron compression and push the temporal resolution of ultrafast electron microscopy to the attosecond regime. However, a large electron-light interaction is required to attain a strong compression, generally necessitating short light and electron pulses combined with optical scattering at nanostructures. Here, we theoretically investigate an alternative configuration based on stimulated Compton scattering, whereby two counterpropagating Gaussian light beams induce energy jumps in a collinear electron beam by multiples of their photon-energy difference. Strong recoil effects are produced by extending the electron-light interaction over millimetric distances, enabling a dramatic increase in temporal compression and substantially reshaping the electron spectra for affordable laser powers. Beyond its fundamental interest, our Letter introduces a practical scheme to achieve a large temporal compression of continuous electron beams without involving optical scattering by material structures.}, archive = {J_PRL}, author = {Cruz I. Velasco and F. Javier García de Abajo}, doi = {10.1103/PhysRevLett.134.123804}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123804}, shortjournal = {Phys. Rev. Lett.}, title = {Free-space optical modulation of free electrons in the continuous-wave regime}, volume = {134}, year = {2025}, }
• (2025). Pseudospin transverse localization of light in an optical disordered spin-glass phase. PRL, 134(12), 123803. (www)

  @article{ , abstract = {Localization phenomena during transport are typically associated with disordered scalar potentials. Here, we predict a universal pseudospin localization phenomenon driven by a disordered vectorial potential and experimentally observe its onset in an optical analog of a classical disordered spin-glass magnetic phase. In our system, disorder in the second-order nonlinear coupling of a nonlinear photonic crystal causes the idler-signal light beam, representing the pseudospin current, to approach localization in the transverse plane. This effect depends strongly on the nonlinear coupling strength, controlled by the optical pump power, revealing its inherently nonlinear nature. Furthermore, this phenomenon is marked by decaying Rabi oscillations between the idler and signal fields, linked to the disorder properties, suggesting an accompanied longitudinal decoherence effect. Our findings offer new insights into spin transport in disordered magnetic textures and open avenues for exploring complex magnetic phases and phase transitions using nonlinear optics.}, archive = {J_PRL}, author = {Shani Izhak and Aviv Karnieli and Ofir Yesharim and Shai Tsesses and Ady Arie}, doi = {10.1103/PhysRevLett.134.123803}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123803}, shortjournal = {Phys. Rev. Lett.}, title = {Pseudospin transverse localization of light in an optical disordered spin-glass phase}, volume = {134}, year = {2025}, }
• (2025). Nonlinear optical bistability in microring resonators for enhanced phase sensing. PRL, 134(12), 123802. (www)

  @article{ , abstract = {Photonic microring resonators are used in a variety of chip-integrated sensing applications where they allow one to measure transmission intensity changes upon external signals with a sensitivity that scales linearly with the Q factor. In this work, we suggest exploiting the nonlinear self-phase-modulation effect to increase the overall sensitivity by an additional gain factor appearing when the operational point of the nonlinear resonator is chosen just at the crossover from the monostable to the bistable regime. We present the theoretical idea together with a first proof of concept experiment displaying a gain factor of 22 on a chip-integrated silicon-nitride resonator.}, archive = {J_PRL}, author = {Patrick Tritschler and Christian Schweikert and Rouven H. Klenk and Simon Abdani and Onur Sözen and Wolfgang Vogel and Georg Rademacher and Torsten Ohms and André Zimmermann and Peter Degenfeld-Schonburg}, doi = {10.1103/PhysRevLett.134.123802}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123802}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear optical bistability in microring resonators for enhanced phase sensing}, volume = {134}, year = {2025}, }
• (2025). Nonlinear dynamics of coupled-resonator kerr combs. PRL, 134(12), 123801. (www)

  @article{ , abstract = {The nonlinear interaction of a microresonator pumped by a laser has revealed complex dynamics, including soliton formation and chaos. Initial studies of coupled-resonator systems reveal even more complicated dynamics that can lead to deterministic mode locking and efficient comb generation. Here, we perform theoretical analysis and experiments that provide insight into the dynamical behavior of coupled-resonator systems operating in the normal group-velocity-dispersion regime. Our stability analysis and simulations reveal that the strong mode-coupling regime, which gives rise to spectrally broad comb states, can lead to an instability mechanism in the auxiliary resonator that destabilizes the comb state and prevents mode locking. We find that this instability can be suppressed by introducing loss in the auxiliary resonator. We investigate the stability of both single- and multipulse solutions and verify our theoretical predictions by performing experiments in a silicon-nitride platform. Our results provide an understanding for accessing broad, efficient, relatively flat high-power mode-locked combs for numerous applications in spectroscopy, time-frequency metrology, and data communications.}, archive = {J_PRL}, author = {Swarnava Sanyal and Yoshitomo Okawachi and Yun Zhao and Bok Young Kim and Karl J. McNulty and Michal Lipson and Alexander L. Gaeta}, doi = {10.1103/PhysRevLett.134.123801}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123801}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear dynamics of coupled-resonator kerr combs}, volume = {134}, year = {2025}, }
• (2025). Long-range interactions in weyl-dense atomic arrays protected from dissipation and disorder. PRL, 134(12), 123602. (www)

  @article{ , abstract = {Long-range interactions are a key resource in many quantum phenomena and technologies. Free-space photons mediate power-law interactions but lack tunability and suffer from decoherence processes due to their omnidirectional emission. Engineered dielectrics can yield tunable and coherent interactions, but typically at the expense of making them both shorter ranged and sensitive to material disorder and photon loss. Here, we propose a platform that can circumvent all these limitations based on three-dimensional subwavelength atomic arrays subjected to magnetic fields. Our key result is to show how to design the polaritonic bands of these atomic metamaterials to feature a pair of frequency-isolated Weyl points, i.e., points in reciprocal space around which the bands disperse linearly and defining monopoles of the Berry curvature. As predicted by recent works, such Weyl excitations can mediate interactions that are simultaneously long range, due to their gapless nature; robust, due to the topological protection of Weyl points; and decoherence-free, due to their subradiant character. We demonstrate the robustness of these isolated Weyl points for a large regime of interatomic distances and magnetic field values and characterize the emergence of their corresponding Fermi arcs surface states. The latter can lead to two-dimensional, nonreciprocal atomic interactions with no analogue in other chiral quantum optical setups.}, archive = {J_PRL}, author = {Iñaki García-Elcano and Paloma A. Huidobro and Jorge Bravo-Abad and Alejandro González-Tudela}, doi = {10.1103/PhysRevLett.134.123602}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123602}, shortjournal = {Phys. Rev. Lett.}, title = {Long-range interactions in weyl-dense atomic arrays protected from dissipation and disorder}, volume = {134}, year = {2025}, }
• (2025). What is the spectral density of the reservoir for a lossy quantized cavity?. PRL, 134(12), 123601. (www)

  @article{ , abstract = {By considering a two-level system weakly coupled to a single lossy three-dimensional cavity mode, and using a quasinormal mode expansion for the photonic medium, we show that the frequency dependence of the quantum coupling interaction between the cavity and its photonic reservoir can not be simply constructed to be independent of the cavity contents. For the single quantum dipole case, we identify the correct form of the local spectral density, revealing a surprising gauge-dependent ∼ ω ± 1 prefactor scaling, as well as a spatially dependent correction. We thus establish the correct quantum form for the cavity-reservoir interaction, which so far has only been worked out rigorously for simple 1D geometries, and show its significant impact on broadband strong coupling.}, archive = {J_PRL}, author = {Chris Gustin and Juanjuan Ren and Stephen Hughes}, doi = {10.1103/PhysRevLett.134.123601}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123601}, shortjournal = {Phys. Rev. Lett.}, title = {What is the spectral density of the reservoir for a lossy quantized cavity?}, volume = {134}, year = {2025}, }
• (2025). Emergence of topological states in relaxation dynamics of interacting bosons. PRL, 134(12), 123405. (www)

  @article{ , abstract = {Topological concepts have been employed to understand a wide range of phenomena in physics. While a plethora of ground states are known to have topological underpinning, it is still quite unclear if and how topology manifests itself in the relaxation dynamics of strongly correlated many-body systems. In this Letter, we study time evolution of interacting bosons in a finite one-dimensional superlattice and uncover surprising emergent topological phenomena in the long-time stationary states. Beginning with simple product states, the system evolves into stationary states with high energy whose string correlation and entanglement are investigated. Based on extensive numerical simulations and effective-model analysis, it is demonstrated that the stationary states are nonthermal for a wide range of parameters, and they exhibit certain features that are characteristic of the symmetry-protected topological ground state of the Hamiltonian. In contrast, no topological feature is found in the stationary state as long as the system thermalizes. This difference is further corroborated by the distinct behavior of quantum entanglement and edge states of the system. Our theoretical prediction can be examined by current experimental techniques and paves the way for a more comprehensive understanding of topological phases in nonequilibrium settings.}, archive = {J_PRL}, author = {Wang Huang and Xu-Chen Yang and Rui Cao and Ying-Hai Wu and Jianmin Yuan and Yongqiang Li}, doi = {10.1103/PhysRevLett.134.123405}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123405}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of topological states in relaxation dynamics of interacting bosons}, volume = {134}, year = {2025}, }
• (2025). Enhancement of rydberg blockade via microwave dressing. PRL, 134(12), 123404. (www)

  @article{ , abstract = {Experimental control over the strength and angular dependence of interactions between atoms is a key capability for advancing quantum technologies. Here, we use microwave dressing to manipulate and enhance Rydberg-Rydberg interactions in an atomic ensemble. By varying the cloud length relative to the blockade radius and measuring the statistics of the light retrieved from the ensemble, we demonstrate a clear enhancement of the interaction strength due to microwave dressing. These results are successfully captured by a theoretical model that accounts for the excitation dynamics, atomic density distribution, and phase-matched retrieval efficiency. Our approach offers a versatile platform for further engineering interactions by exploiting additional features of the microwave fields, such as polarization and detuning, opening pathways for new quantum control strategies.}, archive = {J_PRL}, author = {Deniz Kurdak and Patrick R. Banner and Yaxin Li and Sean R. Muleady and Alexey V. Gorshkov and S. L. Rolston and J. V. Porto}, doi = {10.1103/PhysRevLett.134.123404}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123404}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancement of rydberg blockade via microwave dressing}, volume = {134}, year = {2025}, }
• (2025). Direct observation of time-dependent coherent chiral tunneling dynamics. PRL, 134(12), 123403. (www)

  @article{ , abstract = {Superpositions of handed molecular states give rise to achiral eigenstates, delocalized across a double-well potential via tunneling. A coherent superposition of these energy eigenstates could dynamically relocalize the molecules into chiral states, which has only been addressed theoretically. Here, we present a microwave pump-probe study to create and probe coherent chiral tunneling dynamics in a given rotational state. Through a time-resolved scheme, we uncover the periodic time evolution of the induced chiral wave packet under field-free conditions. Moreover, we demonstrate precise phase control of this coherence via phase modulation during pump excitation.}, archive = {J_PRL}, author = {Wenhao Sun and Denis S. Tikhonov and Melanie Schnell}, doi = {10.1103/PhysRevLett.134.123403}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123403}, shortjournal = {Phys. Rev. Lett.}, title = {Direct observation of time-dependent coherent chiral tunneling dynamics}, volume = {134}, year = {2025}, }
• (2025). Generic transverse stability of kink structures in atomic and optical nonlinear media with competing attractive and repulsive interactions. PRL, 134(12), 123402. (www)

  @article{ , abstract = {We demonstrate the existence and stability of one-dimensional (1D) topological kink configurations immersed in higher-dimensional bosonic gases and nonlinear optical setups. Our analysis pertains, in particular, to the two- and three-dimensional extended Gross-Pitaevskii models with quantum fluctuations describing droplet-bearing environments but also to the two-dimensional cubic-quintic nonlinear Schrödinger equation containing higher-order corrections to the nonlinear refractive index. Contrary to the generic dark soliton transverse instability, the kink structures are generically robust under the interplay of low-amplitude attractive and high-amplitude repulsive interactions. A quasi-1D effective potential picture dictates the existence of these defects, while their stability is obtained numerically and analytically through linearization analysis and direct dynamics in the presence of external fluctuations showcasing their unprecedented resilience. These “generic” (across different models) findings should be detectable in current cold atom and optics experiments, offering insights toward controlling topological excitations.}, archive = {J_PRL}, author = {S. I. Mistakidis and G. Bougas and G. C. Katsimiga and P. G. Kevrekidis}, doi = {10.1103/PhysRevLett.134.123402}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123402}, shortjournal = {Phys. Rev. Lett.}, title = {Generic transverse stability of kink structures in atomic and optical nonlinear media with competing attractive and repulsive interactions}, volume = {134}, year = {2025}, }
• (2025). Microwave-controlled cold chemistry. PRL, 134(12), 123401. (www)

  @article{ , abstract = {Ion-molecule reactions proceed with highly rotational-state-specific rate coefficients and are amenable to stereodynamical control at low temperatures. We introduce a scheme to control cold ion-molecule chemistry with microwaves based on the coherent transfer of molecular rotational-state populations. We use a merged-beam approach to reach collision energies in the range from ∼ 0 to k B × 10 K for the reaction between He + and rotationally cold CO molecules ( T rot ≈ 3 K ) and manipulate the rotational-state population of CO using microwave pulses. We achieve reaction inhibition by up to ∼ 40 % with microwave pulses resonant with pure-rotational transitions in CO, unambiguously demonstrating a nonthermal mechanism for microwave-assisted chemistry.}, archive = {J_PRL}, author = {Fernanda B. V. Martins and Hansjürg Schmutz and Josef A. Agner and Valentina Zhelyazkova and Frédéric Merkt}, doi = {10.1103/PhysRevLett.134.123401}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123401}, shortjournal = {Phys. Rev. Lett.}, title = {Microwave-controlled cold chemistry}, volume = {134}, year = {2025}, }
• (2025). Complete characterizations of intermediate and final state wave functions with photoionization of polarized rb. PRL, 134(12), 123204. (www)

  @article{ , abstract = {The amplitude and phase of a photoionization channel provide deep insights into the nature of ionization dynamics. Here, we propose a novel experimental approach to retrieve these parameters from the photoelectron momentum distribution (PMD), where a 400 nm femtosecond laser is used to ionize polarized Rb atoms prepared in the state. The magnetic quantum numbers of polarized atoms are well controlled by breaking down the symmetry of the cooling laser in a magneto-optical trap reaction microscope. From the tilt angle of the PMD and the interference structure of and ionization channels, we are able to extract their relative amplitude and phase shift, in good agreement with ab initio calculations. This exhibits a benchmark one-photon single ionization study of the hydrogen-like atom, providing a complete measurement with full characterizations of intermediate and final state wave functions.}, archive = {J_PRL}, author = {Huanyu Ma and Linxuan Zhang and Xincheng Wang and Zhihan Zou and Rujin Lv and Zhenjie Shen and Ahai Chen and Matthias Weidemüller and Kiyoshi Ueda and Difa Ye and Yuhai Jiang}, doi = {10.1103/PhysRevLett.134.123204}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123204}, shortjournal = {Phys. Rev. Lett.}, title = {Complete characterizations of intermediate and final state wave functions with photoionization of polarized rb}, volume = {134}, year = {2025}, }
• (2025). Resolving recapture dynamics of rydberg electrons via laser-driven frustrated tunneling ionization. PRL, 134(12), 123203. (www)

  @article{ , abstract = {By employing two-color counterrotating circularly polarized laser fields, we investigate the dynamics of electron recapture into Rydberg states under strong, ultrashort laser pulses, probed via coherent extreme-ultraviolet free-induction decay (XFID). Our study reveals significant distinctions between XFID and above-threshold high-order harmonic generation in terms of their ellipticity dependence on the driving-laser waveforms, yield variations with the laser-intensity ratios, and sensitivity to the driving-laser ellipticity. All these differences arise from the fundamentally distinct electron trajectories underlying the two processes. More importantly, our findings provide compelling evidence that Rydberg-electron recapture predominantly occurs at the end of the driving laser field, offering the first direct experimental confirmation of this long-proposed mechanism.}, archive = {J_PRL}, author = {Sainan Peng and Yudong Chen and Yang Li and Guangyu Fan and Xinhua Xie and Feng He and Zhensheng Tao}, doi = {10.1103/PhysRevLett.134.123203}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123203}, shortjournal = {Phys. Rev. Lett.}, title = {Resolving recapture dynamics of rydberg electrons via laser-driven frustrated tunneling ionization}, volume = {134}, year = {2025}, }
• (2025). Atomic double ionization with quantum light. PRL, 134(12), 123202. (www)

  @article{ , abstract = {Quantum light—specifically light in noncoherent quantum states—can now be generated with intensities high enough to induce nonlinear responses in atoms, marking the emergence of a new “quantum era” in strong-field atomic physics. In this Letter, we explore the influence of quantum states of light on one of the key processes in this field: atomic double ionization. We develop a theoretical framework to model the interaction between a two-electron atom and light in arbitrary quantum states, such as phase-squeezed coherent states or bright squeezed vacuum states. Our results reveal that the quantum state of light significantly impacts the atomic double ionization process, leading to substantial changes in ionization probability and correlated electron momentum distribution.}, archive = {J_PRL}, author = {Haoyu Liu and Hanxu Zhang and Xu Wang and Jianmin Yuan}, doi = {10.1103/PhysRevLett.134.123202}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123202}, shortjournal = {Phys. Rev. Lett.}, title = {Atomic double ionization with quantum light}, volume = {134}, year = {2025}, }
• (2025). G factor of boronlike tin. PRL, 134(12), 123201. (www)

  @article{ , abstract = {In the Alphatrap experiment, the factor of boronlike has been measured with a 0.5 ppb uncertainty. This is the first high-precision measurement of the factor of a heavy boronlike ion. The measured value of 0.6 447 038 265(4) is consistent with the presented ab initio state-of-the-art theory calculations, which predict a value of 0.64 470 29(8). So far, the only boronlike ion of which the factor was measured with high precision has been . The measurement presented here therefore tests quantum electrodynamics as well as many-electron interactions at much higher . Furthermore, we discuss the potential for an independent determination of the fine-structure constant , which can be achieved with a specific difference of factors, combining the presented results with the recent electron -factor measurement of hydrogenlike tin.}, archive = {J_PRL}, author = {J. Morgner and B. Tu and M. Moretti and C. M. König and F. Heiße and T. Sailer and V. A. Yerokhin and B. Sikora and N. S. Oreshkina and Z. Harman and C. H. Keitel and S. Sturm and K. Blaum}, doi = {10.1103/PhysRevLett.134.123201}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123201}, shortjournal = {Phys. Rev. Lett.}, title = {G factor of boronlike tin}, volume = {134}, year = {2025}, }
• (2025). Improved bound-electron g-factor theory through complete two-loop QED calculations. PRL, 134(12), 123001. (www)

  @article{ , abstract = {The two-loop self-energy correction to the bound-electron g factor in hydrogenlike ions is investigated, taking into account the electron-nucleus interaction exactly. This all-order calculation is required to improve the total theoretical uncertainty of the g factor, which is limited by the fact that two-loop self-energy corrections have only been calculated so far in the form of an expansion in Z α . Here, Z is the nuclear charge number and α is the fine-structure constant. In this work, we report calculations of the last missing parts of the total two-loop self-energy correction, exactly in Z α . We apply our theory to the recently measured g factor of the hydrogenlike Sn 118 49 + ion [J. Morgner et al. , Nature (London) 622 , 53 (2023) ] and, with a factor of 8, improve the accuracy of its state-of-the-art theoretical value by almost one order of magnitude, enabling more detailed tests of quantum electrodynamics and new physics in strong fields.}, archive = {J_PRL}, author = {B. Sikora and V. A. Yerokhin and C. H. Keitel and Z. Harman}, doi = {10.1103/PhysRevLett.134.123001}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {123001}, shortjournal = {Phys. Rev. Lett.}, title = {Improved bound-electron g-factor theory through complete two-loop QED calculations}, volume = {134}, year = {2025}, }
• (2025). First extraction of transverse-momentum dependent helicity distributions. PRL, 134(12), 121902. (www)

  @article{ , abstract = {We report on the first global analysis of transverse-momentum dependent helicity distributions of the proton. The analysis is performed at next-to-leading order with the evolution factor at next-to-next-to-leading-logarithmic accuracy. Nonzero signals are determined for up and down quarks, and their k T -integrated polarization is consistent with analyses in collinear factorization, while the distributions of other flavors are loosely constrained by existing data. With increasing transverse momentum, quarks at large x become less polarized while those at small x become more polarized.}, archive = {J_PRL}, author = {Transverse Nucleon Tomography Collaboration and Ke Yang and Tianbo Liu and Peng Sun and Yuxiang Zhao and Bo-Qiang Ma}, doi = {10.1103/PhysRevLett.134.121902}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121902}, shortjournal = {Phys. Rev. Lett.}, title = {First extraction of transverse-momentum dependent helicity distributions}, volume = {134}, year = {2025}, }
• (2025). Exploring the three-dimensional momentum distribution of longitudinally polarized quarks in the proton. PRL, 134(12), 121901. (www)

  @article{ , abstract = {By analyzing experimental data on semi-inclusive deep inelastic scattering off longitudinally polarized targets, we extract the transverse momentum dependence of the quark helicity distribution, i.e., the difference between the three-dimensional motion of quarks with polarization parallel or antiparallel to the longitudinal polarization of the parent hadron. We perform the analysis at next-to-leading and next-to-next-to-leading perturbative accuracy. The quality of the fit is very good for both cases, reaching a χ 2 per number of data points equal to 1.11 and 1.09, respectively. Although the limited number of data points leads to significant uncertainties, the data are consistent with an interpretation in which the helicity distribution is narrower in transverse momentum than the unpolarized distribution.}, archive = {J_PRL}, author = {MAP Collaboration and Alessandro Bacchetta and Alessia Bongallino and Matteo Cerutti and Marco Radici and Lorenzo Rossi}, doi = {10.1103/PhysRevLett.134.121901}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121901}, shortjournal = {Phys. Rev. Lett.}, title = {Exploring the three-dimensional momentum distribution of longitudinally polarized quarks in the proton}, volume = {134}, year = {2025}, }
• (2025). Test of lepton flavor universality with bs0→ϕℓ+ℓ− decays. PRL, 134(12), 121803. (www)

  @article{ , abstract = {Lepton flavor universality in rare transitions is tested for the first time using meson decays. The measurements are performed using collision data collected by the LHCb experiment between 2011 and 2018, corresponding to a total integrated luminosity of . Branching fraction ratios between the and decays are measured in three regions of dilepton mass squared, with , and . The results agree with the standard model expectation of lepton flavor universality.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and V. Bellee and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. C. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and P. Collins and T. Colombo and M. C. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. G. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and J. Haimberger and M. Hajheidari and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and D. Hill and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and J. Lomba Castro and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and B. Urbach and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and G. Vouters and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and D. Yang and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.121803}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121803}, shortjournal = {Phys. Rev. Lett.}, title = {Test of lepton flavor universality with bs0→ϕℓ+ℓ− decays}, volume = {134}, year = {2025}, }
• (2025). New limits on the coherent neutrino-nucleus elastic scattering cross section at the kuo-sheng reactor-neutrino laboratory. PRL, 134(12), 121802. (www)

  @article{ , abstract = {Neutrino-nucleus elastic scattering ( ) with partial quantum-mechanical coherency has been observed in several nuclei with neutrinos from decay-at-rest pions. This interaction with reactor neutrinos where coherency is has not yet been experimentally observed. We present new results on the studies of the cross section with an electrocooled -type point-contact germanium detector at the Kuo-Sheng Reactor Neutrino Laboratory. A total of 242(357) kg-days of Reactor ON(OFF) data at a detector threshold of 200 eV in ionization energy are analyzed. The Lindhard model parametrized by a single variable which characterizes the quenching function was used. A limit at 90% confidence level of at the predicted value of is derived, where is the ratio of the measured to standard model (SM) cross section. Conversely, at the SM value of .}, archive = {J_PRL}, author = {TEXONO Collaboration and S. Karmakar and M. K. Singh and V. Sharma and H. T. Wong and Greeshma C and H. B. Li and L. Singh and M. Agartioglu and J. H. Chen and C. I. Chiang and M. Deniz and H. C. Hsu and S. Karadaǧ and V. Kumar and C. H. Leung and J. Li and F. K. Lin and S. T. Lin and S. K. Liu and H. Ma and K. Saraswat and V. Singh and D. Tanabe and J. S. Wang and L. T. Yang and C. H. Yeh and Q. Yue}, doi = {10.1103/PhysRevLett.134.121802}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121802}, shortjournal = {Phys. Rev. Lett.}, title = {New limits on the coherent neutrino-nucleus elastic scattering cross section at the kuo-sheng reactor-neutrino laboratory}, volume = {134}, year = {2025}, }
• (2025). Search for dark matter produced in association with a dark higgs boson in the bb¯ final state using pp collisions at s=13 TeV with the ATLAS detector. PRL, 134(12), 121801. (www)

  @article{ , abstract = {A search is performed for dark matter particles produced in association with a resonantly produced pair of b -quarks with 30 < m b b < 150 GeV using 140 fb − 1 of proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This signature is expected in extensions of the standard model predicting the production of dark matter particles, in particular those containing a dark Higgs boson s that decays into b b ¯ . The highly boosted s → b b ¯ topology is reconstructed using jet reclustering and a new identification algorithm. This search places stringent constraints across regions of the dark Higgs model parameter space that satisfy the observed relic density, excluding dark Higgs bosons with masses between 30 and 150 GeV in benchmark scenarios with Z ′ mediator masses up to 4.8 TeV at 95% confidence level.}, archive = {J_PRL}, author = {ATLAS Collaboration and G. Aad and E. Aakvaag and B. Abbott and S. Abdelhameed and K. Abeling and N. J. Abicht and S. H. Abidi and M. Aboelela and A. Aboulhorma and H. Abramowicz and H. Abreu and Y. Abulaiti and B. S. Acharya and A. Ackermann and C. Adam Bourdarios and L. Adamczyk and S. V. Addepalli and M. J. Addison and J. Adelman and A. Adiguzel and T. Adye and A. A. Affolder and Y. Afik and M. N. Agaras and J. Agarwala and A. Aggarwal and C. Agheorghiesei and F. Ahmadov and W. S. Ahmed and S. Ahuja and X. Ai and G. Aielli and A. Aikot and M. Ait Tamlihat and B. Aitbenchikh and M. Akbiyik and T. P. A. Åkesson and A. V. Akimov and D. Akiyama and N. N. Akolkar and S. Aktas and K. Al Khoury and G. L. Alberghi and J. Albert and P. Albicocco and G. L. Albouy and S. Alderweireldt and Z. L. Alegria and M. Aleksa and I. N. Aleksandrov and C. Alexa and T. Alexopoulos and F. Alfonsi and M. Algren and M. Alhroob and B. Ali and H. M. J. Ali and S. Ali and S. W. Alibocus and M. Aliev and G. Alimonti and W. Alkakhi and C. Allaire and B. M. M. Allbrooke and J. F. Allen and C. A. Allendes Flores and P. P. Allport and A. Aloisio and F. Alonso and C. Alpigiani and Z. M. K. Alsolami and M. Alvarez Estevez and A. Alvarez Fernandez and M. Alves Cardoso and M. G. Alviggi and M. Aly and Y. Amaral Coutinho and A. Ambler and C. Amelung and M. Amerl and C. G. Ames and D. Amidei and K. Amirie and S. P. Amor Dos Santos and K. R. Amos and S. An and V. Ananiev and C. Anastopoulos and T. Andeen and J. K. Anders and A. C. Anderson and S. Y. Andrean and A. Andreazza and S. Angelidakis and A. Angerami and A. V. Anisenkov and A. Annovi and C. Antel and E. Antipov and M. Antonelli and F. Anulli and M. Aoki and T. Aoki and M. A. Aparo and L. Aperio Bella and C. Appelt and A. Apyan and S. J. Arbiol Val and C. Arcangeletti and A. T. H. Arce and E. Arena and J-F. Arguin and S. Argyropoulos and J.-H. Arling and O. Arnaez and H. Arnold and G. Artoni and H. Asada and K. Asai and S. Asai and N. A. Asbah and R. A. Ashby Pickering and K. Assamagan and R. Astalos and K. S. V. Astrand and S. Atashi and R. J. Atkin and M. Atkinson and H. Atmani and P. A. Atmasiddha and K. Augsten and S. Auricchio and A. D. Auriol and V. A. Austrup and G. Avolio and K. Axiotis and G. Azuelos and D. Babal and H. Bachacou and K. Bachas and A. Bachiu and F. Backman and A. Badea and T. M. Baer and P. Bagnaia and M. Bahmani and D. Bahner and K. Bai and J. T. Baines and L. Baines and O. K. Baker and E. Bakos and D. Bakshi Gupta and L. E. Balabram Filho and V. Balakrishnan and R. Balasubramanian and E. M. Baldin and P. Balek and E. Ballabene and F. Balli and L. M. Baltes and W. K. Balunas and J. Balz and I. Bamwidhi and E. Banas and M. Bandieramonte and A. Bandyopadhyay and S. Bansal and L. Barak and M. Barakat and E. L. Barberio and D. Barberis and M. Barbero and M. Z. Barel and K. N. Barends and T. Barillari and M-S. Barisits and T. Barklow and P. Baron and D. A. Baron Moreno and A. Baroncelli and G. Barone and A. J. Barr and J. D. Barr and F. Barreiro and J. Barreiro Guimarães da Costa and U. Barron and M. G. Barros Teixeira and S. Barsov and F. Bartels and R. Bartoldus and A. E. Barton and P. Bartos and A. Basan and M. Baselga and A. Bassalat and M. J. Basso and S. Bataju and R. Bate and R. L. Bates and S. Batlamous and B. Batool and M. Battaglia and D. Battulga and M. Bauce and M. Bauer and P. Bauer and L. T. Bazzano Hurrell and J. B. Beacham and T. Beau and J. Y. Beaucamp and P. H. Beauchemin and P. Bechtle and H. P. Beck and K. Becker and A. J. Beddall and V. A. Bednyakov and C. P. Bee and L. J. Beemster and T. A. Beermann and M. Begalli and M. Begel and A. Behera and J. K. Behr and J. F. Beirer and F. Beisiegel and M. Belfkir and G. Bella and L. Bellagamba and A. Bellerive and P. Bellos and K. Beloborodov and D. Benchekroun and F. Bendebba and Y. Benhammou and K. C. Benkendorfer and L. Beresford and M. Beretta and E. Bergeaas Kuutmann and N. Berger and B. Bergmann and J. Beringer and G. Bernardi and C. Bernius and F. U. Bernlochner and F. Bernon and A. Berrocal Guardia and T. Berry and P. Berta and A. Berthold and S. Bethke and A. Betti and A. J. Bevan and N. K. Bhalla and S. Bhatta and D. S. Bhattacharya and P. Bhattarai and K. D. Bhide and V. S. Bhopatkar and R. M. Bianchi and G. Bianco and O. Biebel and R. Bielski and M. Biglietti and C. S. Billingsley and M. Bindi and A. Bingul and C. Bini and A. Biondini and G. A. Bird and M. Birman and M. Biros and S. Biryukov and T. Bisanz and E. Bisceglie and J. P. Biswal and D. Biswas and I. Bloch and A. Blue and U. Blumenschein and J. Blumenthal and V. S. Bobrovnikov and M. Boehler and B. Boehm and D. Bogavac and A. G. Bogdanchikov and C. Bohm and V. Boisvert and P. Bokan and T. Bold and M. Bomben and M. Bona and M. Boonekamp and C. D. Booth and A. G. Borbély and I. S. Bordulev and H. M. Borecka-Bielska and G. Borissov and D. Bortoletto and D. Boscherini and M. Bosman and J. D. Bossio Sola and K. Bouaouda and N. Bouchhar and L. Boudet and J. Boudreau and E. V. Bouhova-Thacker and D. Boumediene and R. Bouquet and A. Boveia and J. Boyd and D. Boye and I. R. Boyko and L. Bozianu and J. Bracinik and N. Brahimi and G. Brandt and O. Brandt and F. Braren and B. Brau and J. E. Brau and R. Brener and L. Brenner and R. Brenner and S. Bressler and G. Brianti and D. Britton and D. Britzger and I. Brock and R. Brock and G. Brooijmans and E. M. Brooks and E. Brost and L. M. Brown and L. E. Bruce and T. L. Bruckler and P. A. Bruckman de Renstrom and B. Brüers and A. Bruni and G. Bruni and M. Bruschi and N. Bruscino and T. Buanes and Q. Buat and D. Buchin and A. G. Buckley and O. Bulekov and B. A. Bullard and S. Burdin and C. D. Burgard and A. M. Burger and B. Burghgrave and O. Burlayenko and J. Burleson and J. T. P. Burr and J. C. Burzynski and E. L. Busch and V. Büscher and P. J. Bussey and J. M. Butler and C. M. Buttar and J. M. Butterworth and W. Buttinger and C. J. Buxo Vazquez and A. R. Buzykaev and S. Cabrera Urbán and L. Cadamuro and D. Caforio and H. Cai and Y. Cai and V. M. M. Cairo and O. Cakir and N. Calace and P. Calafiura and G. Calderini and P. Calfayan and G. Callea and L. P. Caloba and D. Calvet and S. Calvet and M. Calvetti and R. Camacho Toro and S. Camarda and D. Camarero Munoz and P. Camarri and M. T. Camerlingo and D. Cameron and C. Camincher and M. Campanelli and A. Camplani and V. Canale and A. C. Canbay and E. Canonero and J. Cantero and Y. Cao and F. Capocasa and M. Capua and A. Carbone and R. Cardarelli and J. C. J. Cardenas and G. Carducci and T. Carli and G. Carlino and J. I. Carlotto and B. T. Carlson and E. M. Carlson and J. Carmignani and L. Carminati and A. Carnelli and M. Carnesale and S. Caron and E. Carquin and S. Carrá and G. Carratta and A. M. Carroll and T. M. Carter and M. P. Casado and M. Caspar and F. L. Castillo and L. Castillo Garcia and V. Castillo Gimenez and N. F. Castro and A. Catinaccio and J. R. Catmore and T. Cavaliere and V. Cavaliere and N. Cavalli and L. J. Caviedes Betancourt and Y. C. Cekmecelioglu and E. Celebi and S. Cella and F. Celli and M. S. Centonze and V. Cepaitis and K. Cerny and A. S. Cerqueira and A. Cerri and L. Cerrito and F. Cerutti and B. Cervato and A. Cervelli and G. Cesarini and S. A. Cetin and D. Chakraborty and J. Chan and W. Y. Chan and J. D. Chapman and E. Chapon and B. Chargeishvili and D. G. Charlton and M. Chatterjee and C. Chauhan and Y. Che and S. Chekanov and S. V. Chekulaev and G. A. Chelkov and A. Chen and B. Chen and H. Chen and J. Chen and M. Chen and S. Chen and S. J. Chen and X. Chen and Y. Chen and C. L. Cheng and H. C. Cheng and S. Cheong and A. Cheplakov and E. Cheremushkina and E. Cherepanova and R. Cherkaoui El Moursli and E. Cheu and K. Cheung and L. Chevalier and V. Chiarella and G. Chiarelli and N. Chiedde and G. Chiodini and A. S. Chisholm and A. Chitan and M. Chitishvili and M. V. Chizhov and K. Choi and Y. Chou and E. Y. S. Chow and K. L. Chu and M. C. Chu and X. Chu and Z. Chubinidze and J. Chudoba and J. J. Chwastowski and D. Cieri and K. M. Ciesla and V. Cindro and A. Ciocio and F. Cirotto and Z. H. Citron and M. Citterio and D. A. Ciubotaru and A. Clark and P. J. Clark and N. Clarke Hall and C. Clarry and J. M. Clavijo Columbie and S. E. Clawson and C. Clement and Y. Coadou and M. Cobal and A. Coccaro and R. F. Coelho Barrue and R. Coelho Lopes De Sa and S. Coelli and B. Cole and J. Collot and P. Conde Muiño and M. P. Connell and S. H. Connell and E. I. Conroy and F. Conventi and H. G. Cooke and A. M. Cooper-Sarkar and F. A. Corchia and A. Cordeiro Oudot Choi and L. D. Corpe and M. Corradi and F. Corriveau and A. Cortes-Gonzalez and M. J. Costa and F. Costanza and D. Costanzo and B. M. Cote and J. Couthures and G. Cowan and K. Cranmer and D. Cremonini and S. Crépé-Renaudin and F. Crescioli and M. Cristinziani and M. Cristoforetti and V. Croft and J. E. Crosby and G. Crosetti and A. Cueto and H. Cui and Z. Cui and W. R. Cunningham and F. Curcio and J. R. Curran and P. Czodrowski and M. M. Czurylo and M. J. Da Cunha Sargedas De Sousa and J. V. Da Fonseca Pinto and C. Da Via and W. Dabrowski and T. Dado and S. Dahbi and T. Dai and D. Dal Santo and C. Dallapiccola and M. Dam and G. D’amen and V. D’Amico and J. Damp and J. R. Dandoy and D. Dannheim and M. Danninger and V. Dao and G. Darbo and S. J. Das and F. Dattola and S. D’Auria and A. D’Avanzo and C. David and T. Davidek and I. Dawson and H. A. Day-hall and K. De and R. De Asmundis and N. De Biase and S. De Castro and N. De Groot and P. de Jong and H. De la Torre and A. De Maria and A. De Salvo and U. De Sanctis and F. De Santis and A. De Santo and J. B. De Vivie De Regie and D. V. Dedovich and J. Degens and A. M. Deiana and F. Del Corso and J. Del Peso and F. Del Rio and L. Delagrange and F. Deliot and C. M. Delitzsch and M. Della Pietra and D. Della Volpe and A. Dell’Acqua and L. Dell’Asta and M. Delmastro and P. A. Delsart and S. Demers and M. Demichev and S. P. Denisov and L. D’Eramo and D. Derendarz and F. Derue and P. Dervan and K. Desch and C. Deutsch and F. A. Di Bello and A. Di Ciaccio and L. Di Ciaccio and A. Di Domenico and C. Di Donato and A. Di Girolamo and G. Di Gregorio and A. Di Luca and B. Di Micco and R. Di Nardo and K. F. Di Petrillo and M. Diamantopoulou and F. A. Dias and T. Dias Do Vale and M. A. Diaz and F. G. Diaz Capriles and A. R. Didenko and M. Didenko and E. B. Diehl and S. Díez Cornell and C. Diez Pardos and C. Dimitriadi and A. Dimitrievska and J. Dingfelder and T. Dingley and I-M. Dinu and S. J. Dittmeier and F. Dittus and M. Divisek and F. Djama and T. Djobava and C. Doglioni and A. Dohnalova and J. Dolejsi and Z. Dolezal and K. Domijan and K. M. Dona and M. Donadelli and B. Dong and J. Donini and A. D’Onofrio and M. D’Onofrio and J. Dopke and A. Doria and N. Dos Santos Fernandes and P. Dougan and M. T. Dova and A. T. Doyle and M. A. Draguet and E. Dreyer and I. Drivas-koulouris and M. Drnevich and M. Drozdova and D. Du and T. A. du Pree and F. Dubinin and M. Dubovsky and E. Duchovni and G. Duckeck and O. A. Ducu and D. Duda and A. Dudarev and E. R. Duden and M. D’uffizi and L. Duflot and M. Dührssen and I. Duminica and A. E. Dumitriu and M. Dunford and S. Dungs and K. Dunne and A. Duperrin and H. Duran Yildiz and M. Düren and A. Durglishvili and B. L. Dwyer and G. I. Dyckes and M. Dyndal and B. S. Dziedzic and Z. O. Earnshaw and G. H. Eberwein and B. Eckerova and S. Eggebrecht and E. Egidio Purcino De Souza and L. F. Ehrke and G. Eigen and K. Einsweiler and T. Ekelof and P. A. Ekman and S. El Farkh and Y. El Ghazali and H. El Jarrari and A. El Moussaouy and V. Ellajosyula and M. Ellert and F. Ellinghaus and N. Ellis and J. Elmsheuser and M. Elsawy and M. Elsing and D. Emeliyanov and Y. Enari and I. Ene and S. Epari and P. A. Erland and D. Ernani Martins Neto and M. Errenst and M. Escalier and C. Escobar and E. Etzion and G. Evans and H. Evans and L. S. Evans and A. Ezhilov and S. Ezzarqtouni and F. Fabbri and L. Fabbri and G. Facini and V. Fadeyev and R. M. Fakhrutdinov and D. Fakoudis and S. Falciano and L. F. Falda Ulhoa Coelho and F. Fallavollita and G. Falsetti and J. Faltova and C. Fan and Y. Fan and Y. Fang and M. Fanti and M. Faraj and Z. Farazpay and A. Farbin and A. Farilla and T. Farooque and S. M. Farrington and F. Fassi and D. Fassouliotis and M. Faucci Giannelli and W. J. Fawcett and L. Fayard and P. Federic and P. Federicova and O. L. Fedin and M. Feickert and L. Feligioni and D. E. Fellers and C. Feng and M. Feng and Z. Feng and M. J. Fenton and L. Ferencz and R. A. M. Ferguson and S. I. Fernandez Luengo and P. Fernandez Martinez and M. J. V. Fernoux and J. Ferrando and A. Ferrari and P. Ferrari and R. Ferrari and D. Ferrere and C. Ferretti and D. Fiacco and F. Fiedler and P. Fiedler and A. Filipčič and E. K. Filmer and F. Filthaut and M. C. N. Fiolhais and L. Fiorini and W. C. Fisher and T. Fitschen and P. M. Fitzhugh and I. Fleck and P. Fleischmann and T. Flick and M. Flores and L. R. Flores Castillo and L. Flores Sanz De Acedo and F. M. Follega and N. Fomin and J. H. Foo and A. Formica and A. C. Forti and E. Fortin and A. W. Fortman and M. G. Foti and L. Fountas and D. Fournier and H. Fox and P. Francavilla and S. Francescato and S. Franchellucci and M. Franchini and S. Franchino and D. Francis and L. Franco and V. Franco Lima and L. Franconi and M. Franklin and G. Frattari and Y. Y. Frid and J. Friend and N. Fritzsche and A. Froch and D. Froidevaux and J. A. Frost and Y. Fu and S. Fuenzalida Garrido and M. Fujimoto and K. Y. Fung and E. Furtado De Simas Filho and M. Furukawa and J. Fuster and A. Gaa and A. Gabrielli and P. Gadow and G. Gagliardi and L. G. Gagnon and S. Gaid and S. Galantzan and E. J. Gallas and B. J. Gallop and K. K. Gan and S. Ganguly and Y. Gao and F. M. Garay Walls and B. Garcia and C. García and A. Garcia Alonso and A. G. Garcia Caffaro and J. E. García Navarro and M. Garcia-Sciveres and G. L. Gardner and R. W. Gardner and N. Garelli and D. Garg and R. B. Garg and J. M. Gargan and C. A. Garner and C. M. Garvey and V. K. Gassmann and G. Gaudio and V. Gautam and P. Gauzzi and J. Gavranovic and I. L. Gavrilenko and A. Gavrilyuk and C. Gay and G. Gaycken and E. N. Gazis and A. A. Geanta and C. M. Gee and A. Gekow and C. Gemme and M. H. Genest and A. D. Gentry and S. George and W. F. George and T. Geralis and P. Gessinger-Befurt and M. E. Geyik and M. Ghani and K. Ghorbanian and A. Ghosal and A. Ghosh and B. Giacobbe and S. Giagu and T. Giani and A. Giannini and S. M. Gibson and M. Gignac and D. T. Gil and A. K. Gilbert and B. J. Gilbert and D. Gillberg and G. Gilles and L. Ginabat and D. M. Gingrich and M. P. Giordani and P. F. Giraud and G. Giugliarelli and D. Giugni and F. Giuli and I. Gkialas and L. K. Gladilin and C. Glasman and G. R. Gledhill and G. Glemža and M. Glisic and I. Gnesi and Y. Go and M. Goblirsch-Kolb and B. Gocke and D. Godin and B. Gokturk and S. Goldfarb and T. Golling and M. G. D. Gololo and D. Golubkov and J. P. Gombas and A. Gomes and G. Gomes Da Silva and A. J. Gomez Delegido and R. Gonçalo and L. Gonella and A. Gongadze and F. Gonnella and J. L. Gonski and R. Y. González Andana and S. González de la Hoz and R. Gonzalez Lopez and C. Gonzalez Renteria and M. V. Gonzalez Rodrigues and R. Gonzalez Suarez and S. Gonzalez-Sevilla and L. Goossens and B. Gorini and E. Gorini and A. Gorišek and T. C. Gosart and A. T. Goshaw and M. I. Gostkin and S. Goswami and C. A. Gottardo and S. A. Gotz and M. Gouighri and V. Goumarre and A. G. Goussiou and N. Govender and I. Grabowska-Bold and K. Graham and E. Gramstad and S. Grancagnolo and C. M. Grant and P. M. Gravila and F. G. Gravili and H. M. Gray and M. Greco and M. J. Green and C. Grefe and A. S. Grefsrud and I. M. Gregor and K. T. Greif and P. Grenier and S. G. Grewe and A. A. Grillo and K. Grimm and S. Grinstein and J.-F. Grivaz and E. Gross and J. Grosse-Knetter and J. C. Grundy and L. Guan and J. G. R. Guerrero Rojas and G. Guerrieri and R. Gugel and J. A. M. Guhit and A. Guida and E. Guilloton and S. Guindon and F. Guo and J. Guo and L. Guo and Y. Guo and R. Gupta and S. Gurbuz and S. S. Gurdasani and G. Gustavino and P. Gutierrez and L. F. Gutierrez Zagazeta and M. Gutsche and C. Gutschow and C. Gwenlan and C. B. Gwilliam and E. S. Haaland and A. Haas and M. Habedank and C. Haber and H. K. Hadavand and A. Hadef and S. Hadzic and A. I. Hagan and J. J. Hahn and E. H. Haines and M. Haleem and J. Haley and J. J. Hall and G. D. Hallewell and L. Halser and K. Hamano and M. Hamer and G. N. Hamity and E. J. Hampshire and J. Han and K. Han and L. Han and S. Han and Y. F. Han and K. Hanagaki and M. Hance and D. A. Hangal and H. Hanif and M. D. Hank and J. B. Hansen and P. H. Hansen and K. Hara and D. Harada and T. Harenberg and S. Harkusha and M. L. Harris and Y. T. Harris and J. Harrison and N. M. Harrison and P. F. Harrison and N. M. Hartman and N. M. Hartmann and R. Z. Hasan and Y. Hasegawa and S. Hassan and R. Hauser and C. M. Hawkes and R. J. Hawkings and Y. Hayashi and S. Hayashida and D. Hayden and C. Hayes and R. L. Hayes and C. P. Hays and J. M. Hays and H. S. Hayward and F. He and M. He and Y. He and N. B. Heatley and V. Hedberg and A. L. Heggelund and N. D. Hehir and C. Heidegger and K. K. Heidegger and J. Heilman and S. Heim and T. Heim and J. G. Heinlein and J. J. Heinrich and L. Heinrich and J. Hejbal and A. Held and S. Hellesund and C. M. Helling and S. Hellman and R. C. W. Henderson and L. Henkelmann and A. M. Henriques Correia and H. Herde and Y. Hernández Jiménez and L. M. Herrmann and T. Herrmann and G. Herten and R. Hertenberger and L. Hervas and M. E. Hesping and N. P. Hessey and M. Hidaoui and N. Hidic and E. Hill and S. J. Hillier and J. R. Hinds and F. Hinterkeuser and M. Hirose and S. Hirose and D. Hirschbuehl and T. G. Hitchings and B. Hiti and J. Hobbs and R. Hobincu and N. Hod and M. C. Hodgkinson and B. H. Hodkinson and A. Hoecker and D. D. Hofer and J. Hofer and T. Holm and M. Holzbock and L. B. A. H. Hommels and B. P. Honan and J. J. Hong and J. Hong and T. M. Hong and B. H. Hooberman and W. H. Hopkins and M. C. Hoppesch and Y. Horii and S. Hou and A. S. Howard and J. Howarth and J. Hoya and M. Hrabovsky and A. Hrynevich and T. Hryn’ova and P. J. Hsu and S.-C. Hsu and T. Hsu and M. Hu and Q. Hu and S. Huang and X. Huang and Y. Huang and Z. Huang and Z. Hubacek and M. Huebner and F. Huegging and T. B. Huffman and C. A. Hugli and M. Huhtinen and S. K. Huiberts and R. Hulsken and N. Huseynov and J. Huston and J. Huth and R. Hyneman and G. Iacobucci and G. Iakovidis and L. Iconomidou-Fayard and J. P. Iddon and P. Iengo and R. Iguchi and Y. Iiyama and T. Iizawa and Y. Ikegami and N. Ilic and H. Imam and M. Ince Lezki and T. Ingebretsen Carlson and J. M. Inglis and G. Introzzi and M. Iodice and V. Ippolito and R. K. Irwin and M. Ishino and W. Islam and C. Issever and S. Istin and H. Ito and R. Iuppa and A. Ivina and J. M. Izen and V. Izzo and P. Jacka and P. Jackson and C. S. Jagfeld and G. Jain and P. Jain and K. Jakobs and T. Jakoubek and J. Jamieson and W. Jang and M. Javurkova and P. Jawahar and L. Jeanty and J. Jejelava and P. Jenni and C. E. Jessiman and C. Jia and J. Jia and X. Jia and Z. Jia and C. Jiang and Q. Jiang and S. Jiggins and J. Jimenez Pena and S. Jin and A. Jinaru and O. Jinnouchi and P. Johansson and K. A. Johns and J. W. Johnson and D. M. Jones and E. Jones and P. Jones and R. W. L. Jones and T. J. Jones and H. L. Joos and R. Joshi and J. Jovicevic and X. Ju and J. J. Junggeburth and T. Junkermann and A. Juste Rozas and M. K. Juzek and S. Kabana and A. Kaczmarska and M. Kado and H. Kagan and M. Kagan and A. Kahn and C. Kahra and T. Kaji and E. Kajomovitz and N. Kakati and I. Kalaitzidou and C. W. Kalderon and N. J. Kang and D. Kar and K. Karava and M. J. Kareem and E. Karentzos and O. Karkout and S. N. Karpov and Z. M. Karpova and V. Kartvelishvili and A. N. Karyukhin and E. Kasimi and J. Katzy and S. Kaur and K. Kawade and M. P. Kawale and C. Kawamoto and T. Kawamoto and E. F. Kay and F. I. Kaya and S. Kazakos and V. F. Kazanin and Y. Ke and J. M. Keaveney and R. Keeler and G. V. Kehris and J. S. Keller and A. S. Kelly and J. J. Kempster and P. D. Kennedy and O. Kepka and B. P. Kerridge and S. Kersten and B. P. Kerševan and L. Keszeghova and S. Ketabchi Haghighat and R. A. Khan and A. Khanov and A. G. Kharlamov and T. Kharlamova and E. E. Khoda and M. Kholodenko and T. J. Khoo and G. Khoriauli and J. Khubua and Y. A. R. Khwaira and B. Kibirige and D. Kim and D. W. Kim and Y. K. Kim and N. Kimura and M. K. Kingston and A. Kirchhoff and C. Kirfel and F. Kirfel and J. Kirk and A. E. Kiryunin and C. Kitsaki and O. Kivernyk and M. Klassen and C. Klein and L. Klein and M. H. Klein and S. B. Klein and U. Klein and P. Klimek and A. Klimentov and T. Klioutchnikova and P. Kluit and S. Kluth and E. Kneringer and T. M. Knight and A. Knue and R. Kobayashi and M. Kobel and D. Kobylianskii and S. F. Koch and M. Kocian and P. Kodyš and D. M. Koeck and P. T. Koenig and T. Koffas and O. Kolay and I. Koletsou and T. Komarek and K. Köneke and A. X. Y. Kong and T. Kono and N. Konstantinidis and P. Kontaxakis and B. Konya and R. Kopeliansky and S. Koperny and K. Korcyl and K. Kordas and A. Korn and S. Korn and I. Korolkov and N. Korotkova and B. Kortman and O. Kortner and S. Kortner and W. H. Kostecka and V. V. Kostyukhin and A. Kotsokechagia and A. Kotwal and A. Koulouris and A. Kourkoumeli-Charalampidi and C. Kourkoumelis and E. Kourlitis and O. Kovanda and R. Kowalewski and W. Kozanecki and A. S. Kozhin and V. A. Kramarenko and G. Kramberger and P. Kramer and M. W. Krasny and A. Krasznahorkay and A. C. Kraus and J. W. Kraus and J. A. Kremer and T. Kresse and L. Kretschmann and J. Kretzschmar and K. Kreul and P. Krieger and S. Krishnamurthy and M. Krivos and K. Krizka and K. Kroeninger and H. Kroha and J. Kroll and K. S. Krowpman and U. Kruchonak and H. Krüger and N. Krumnack and M. C. Kruse and O. Kuchinskaia and S. Kuday and S. Kuehn and R. Kuesters and T. Kuhl and V. Kukhtin and Y. Kulchitsky and S. Kuleshov and M. Kumar and N. Kumari and P. Kumari and A. Kupco and T. Kupfer and A. Kupich and O. Kuprash and H. Kurashige and L. L. Kurchaninov and O. Kurdysh and Y. A. Kurochkin and A. Kurova and M. Kuze and A. K. Kvam and J. Kvita and T. Kwan and N. G. Kyriacou and L. A. O. Laatu and C. Lacasta and F. Lacava and H. Lacker and D. Lacour and N. N. Lad and E. Ladygin and A. Lafarge and B. Laforge and T. Lagouri and F. Z. Lahbabi and S. Lai and J. E. Lambert and S. Lammers and W. Lampl and C. Lampoudis and G. Lamprinoudis and A. N. Lancaster and E. Lançon and U. Landgraf and M. P. J. Landon and V. S. Lang and O. K. B. Langrekken and A. J. Lankford and F. Lanni and K. Lantzsch and A. Lanza and J. F. Laporte and T. Lari and F. Lasagni Manghi and M. Lassnig and V. Latonova and A. Laurier and S. D. Lawlor and Z. Lawrence and R. Lazaridou and M. Lazzaroni and B. Le and E. M. Le Boulicaut and L. T. Le Pottier and B. Leban and A. Lebedev and M. LeBlanc and F. Ledroit-Guillon and S. C. Lee and S. Lee and T. F. Lee and L. L. Leeuw and H. P. Lefebvre and M. Lefebvre and C. Leggett and G. Lehmann Miotto and M. Leigh and W. A. Leight and W. Leinonen and A. Leisos and M. A. L. Leite and C. E. Leitgeb and R. Leitner and K. J. C. Leney and T. Lenz and S. Leone and C. Leonidopoulos and A. Leopold and R. Les and C. G. Lester and M. Levchenko and J. Levêque and L. J. Levinson and G. Levrini and M. P. Lewicki and C. Lewis and D. J. Lewis and A. Li and B. Li and C. Li and C-Q. Li and H. Li and J. Li and K. Li and L. Li and M. Li and S. Li and T. Li and X. Li and Z. Li and S. Liang and Z. Liang and M. Liberatore and B. Liberti and K. Lie and J. Lieber Marin and H. Lien and H. Lin and K. Lin and R. E. Lindley and J. H. Lindon and J. Ling and E. Lipeles and A. Lipniacka and A. Lister and J. D. Little and B. Liu and B. X. Liu and D. Liu and E. H. L. Liu and J. B. Liu and J. K. K. Liu and K. Liu and M. Liu and M. Y. Liu and P. Liu and Q. Liu and X. Liu and Y. Liu and Y. L. Liu and Y. W. Liu and J. Llorente Merino and S. L. Lloyd and E. M. Lobodzinska and P. Loch and T. Lohse and K. Lohwasser and E. Loiacono and M. Lokajicek and J. D. Lomas and J. D. Long and I. Longarini and R. Longo and I. Lopez Paz and A. Lopez Solis and N. Lorenzo Martinez and A. M. Lory and M. Losada and G. Löschcke Centeno and O. Loseva and X. Lou and A. Lounis and P. A. Love and G. Lu and M. Lu and S. Lu and Y. J. Lu and H. J. Lubatti and C. Luci and F. L. Lucio Alves and F. Luehring and I. Luise and O. Lukianchuk and O. Lundberg and B. Lund-Jensen and N. A. Luongo and M. S. Lutz and A. B. Lux and D. Lynn and R. Lysak and E. Lytken and V. Lyubushkin and T. Lyubushkina and M. M. Lyukova and M. Firdaus M. Soberi and H. Ma and K. Ma and L. L. Ma and W. Ma and Y. Ma and J. C. MacDonald and P. C. Machado De Abreu Farias and R. Madar and T. Madula and J. Maeda and T. Maeno and H. Maguire and V. Maiboroda and A. Maio and K. Maj and O. Majersky and S. Majewski and N. Makovec and V. Maksimovic and B. Malaescu and Pa. Malecki and V. P. Maleev and F. Malek and M. Mali and D. Malito and U. Mallik and S. Maltezos and S. Malyukov and J. Mamuzic and G. Mancini and M. N. Mancini and G. Manco and J. P. Mandalia and S. S. Mandarry and I. Mandić and L. Manhaes de Andrade Filho and I. M. Maniatis and J. Manjarres Ramos and D. C. Mankad and A. Mann and S. Manzoni and L. Mao and X. Mapekula and A. Marantis and G. Marchiori and M. Marcisovsky and C. Marcon and M. Marinescu and S. Marium and M. Marjanovic and A. Markhoos and M. Markovitch and E. J. Marshall and Z. Marshall and S. Marti-Garcia and J. Martin and T. A. Martin and V. J. Martin and B. Martin dit Latour and L. Martinelli and M. Martinez and P. Martinez Agullo and V. I. Martinez Outschoorn and P. Martinez Suarez and S. Martin-Haugh and G. Martinovicova and V. S. Martoiu and A. C. Martyniuk and A. Marzin and D. Mascione and L. Masetti and T. Mashimo and J. Masik and A. L. Maslennikov and P. Massarotti and P. Mastrandrea and A. Mastroberardino and T. Masubuchi and T. Mathisen and J. Matousek and N. Matsuzawa and J. Maurer and A. J. Maury and B. Maček and D. A. Maximov and A. E. May and R. Mazini and I. Maznas and M. Mazza and S. M. Mazza and E. Mazzeo and C. Mc Ginn and J. P. Mc Gowan and S. P. Mc Kee and C. C. McCracken and E. F. McDonald and A. E. McDougall and J. A. Mcfayden and R. P. McGovern and R. P. Mckenzie and T. C. Mclachlan and D. J. Mclaughlin and S. J. McMahon and C. M. Mcpartland and R. A. McPherson and S. Mehlhase and A. Mehta and D. Melini and B. R. Mellado Garcia and A. H. Melo and F. Meloni and A. M. Mendes Jacques Da Costa and H. Y. Meng and L. Meng and S. Menke and M. Mentink and E. Meoni and G. Mercado and S. Merianos and C. Merlassino and L. Merola and C. Meroni and J. Metcalfe and A. S. Mete and E. Meuser and C. Meyer and J-P. Meyer and R. P. Middleton and L. Mijović and G. Mikenberg and M. Mikestikova and M. Mikuž and H. Mildner and A. Milic and D. W. Miller and E. H. Miller and L. S. Miller and A. Milov and D. A. Milstead and T. Min and A. A. Minaenko and I. A. Minashvili and L. Mince and A. I. Mincer and B. Mindur and M. Mineev and Y. Mino and L. M. Mir and M. Miralles Lopez and M. Mironova and A. Mishima and M. C. Missio and A. Mitra and V. A. Mitsou and Y. Mitsumori and O. Miu and P. S. Miyagawa and T. Mkrtchyan and M. Mlinarevic and T. Mlinarevic and M. Mlynarikova and S. Mobius and P. Mogg and M. H. Mohamed Farook and A. F. Mohammed and S. Mohapatra and G. Mokgatitswane and L. Moleri and B. Mondal and S. Mondal and K. Mönig and E. Monnier and L. Monsonis Romero and J. Montejo Berlingen and M. Montella and F. Montereali and F. Monticelli and S. Monzani and N. Morange and A. L. Moreira De Carvalho and M. Moreno Llácer and C. Moreno Martinez and P. Morettini and S. Morgenstern and M. Morii and M. Morinaga and F. Morodei and L. Morvaj and P. Moschovakos and B. Moser and M. Mosidze and T. Moskalets and P. Moskvitina and J. Moss and P. Moszkowicz and A. Moussa and E. J. W. Moyse and O. Mtintsilana and S. Muanza and J. Mueller and D. Muenstermann and R. Müller and G. A. Mullier and A. J. Mullin and J. J. Mullin and D. P. Mungo and D. Munoz Perez and F. J. Munoz Sanchez and M. Murin and W. J. Murray and M. Muškinja and C. Mwewa and A. G. Myagkov and A. J. Myers and G. Myers and M. Myska and B. P. Nachman and O. Nackenhorst and K. Nagai and K. Nagano and J. L. Nagle and E. Nagy and A. M. Nairz and Y. Nakahama and K. Nakamura and K. Nakkalil and H. Nanjo and E. A. Narayanan and I. Naryshkin and L. Nasella and M. Naseri and S. Nasri and C. Nass and G. Navarro and J. Navarro-Gonzalez and R. Nayak and A. Nayaz and P. Y. Nechaeva and S. Nechaeva and F. Nechansky and L. Nedic and T. J. Neep and A. Negri and M. Negrini and C. Nellist and C. Nelson and K. Nelson and S. Nemecek and M. Nessi and M. S. Neubauer and F. Neuhaus and J. Neundorf and P. R. Newman and C. W. Ng and Y. W. Y. Ng and B. Ngair and H. D. N. Nguyen and R. B. Nickerson and R. Nicolaidou and J. Nielsen and M. Niemeyer and J. Niermann and N. Nikiforou and V. Nikolaenko and I. Nikolic-Audit and K. Nikolopoulos and P. Nilsson and I. Ninca and G. Ninio and A. Nisati and N. Nishu and R. Nisius and J-E. Nitschke and E. K. Nkadimeng and T. Nobe and T. Nommensen and M. B. Norfolk and B. J. Norman and M. Noury and J. Novak and T. Novak and L. Novotny and R. Novotny and L. Nozka and K. Ntekas and N. M. J. Nunes De Moura Junior and J. Ocariz and A. Ochi and I. Ochoa and S. Oerdek and J. T. Offermann and A. Ogrodnik and A. Oh and C. C. Ohm and H. Oide and R. Oishi and M. L. Ojeda and Y. Okumura and L. F. Oleiro Seabra and I. Oleksiyuk and S. A. Olivares Pino and G. Oliveira Correa and D. Oliveira Damazio and D. Oliveira Goncalves and J. L. Oliver and Ö. O. Öncel and A. P. O’Neill and A. Onofre and P. U. E. Onyisi and M. J. Oreglia and G. E. Orellana and D. Orestano and N. Orlando and R. S. Orr and L. M. Osojnak and R. Ospanov and G. Otero y Garzon and H. Otono and P. S. Ott and G. J. Ottino and M. Ouchrif and F. Ould-Saada and T. Ovsiannikova and M. Owen and R. E. Owen and V. E. Ozcan and F. Ozturk and N. Ozturk and S. Ozturk and H. A. Pacey and A. Pacheco Pages and C. Padilla Aranda and G. Padovano and S. Pagan Griso and G. Palacino and A. Palazzo and J. Pampel and J. Pan and T. Pan and D. K. Panchal and C. E. Pandini and J. G. Panduro Vazquez and H. D. Pandya and H. Pang and P. Pani and G. Panizzo and L. Panwar and L. Paolozzi and S. Parajuli and A. Paramonov and C. Paraskevopoulos and D. Paredes Hernandez and A. Pareti and K. R. Park and T. H. Park and M. A. Parker and F. Parodi and E. W. Parrish and V. A. Parrish and J. A. Parsons and U. Parzefall and B. Pascual Dias and L. Pascual Dominguez and E. Pasqualucci and S. Passaggio and F. Pastore and P. Patel and U. M. Patel and J. R. Pater and T. Pauly and C. I. Pazos and J. Pearkes and M. Pedersen and R. Pedro and S. V. Peleganchuk and O. Penc and E. A. Pender and G. D. Penn and K. E. Penski and M. Penzin and B. S. Peralva and A. P. Pereira Peixoto and L. Pereira Sanchez and D. V. Perepelitsa and G. Perera and E. Perez Codina and M. Perganti and H. Pernegger and S. Perrella and O. Perrin and K. Peters and R. F. Y. Peters and B. A. Petersen and T. C. Petersen and E. Petit and V. Petousis and C. Petridou and T. Petru and A. Petrukhin and M. Pettee and A. Petukhov and K. Petukhova and R. Pezoa and L. Pezzotti and G. Pezzullo and T. M. Pham and T. Pham and P. W. Phillips and G. Piacquadio and E. Pianori and F. Piazza and R. Piegaia and D. Pietreanu and A. D. Pilkington and M. Pinamonti and J. L. Pinfold and B. C. Pinheiro Pereira and A. E. Pinto Pinoargote and L. Pintucci and K. M. Piper and A. Pirttikoski and D. A. Pizzi and L. Pizzimento and A. Pizzini and M.-A. Pleier and V. Pleskot and E. Plotnikova and G. Poddar and R. Poettgen and L. Poggioli and I. Pokharel and S. Polacek and G. Polesello and A. Poley and A. Polini and C. S. Pollard and Z. B. Pollock and E. Pompa Pacchi and N. I. Pond and D. Ponomarenko and L. Pontecorvo and S. Popa and G. A. Popeneciu and A. Poreba and D. M. Portillo Quintero and S. Pospisil and M. A. Postill and P. Postolache and K. Potamianos and P. A. Potepa and I. N. Potrap and C. J. Potter and H. Potti and J. Poveda and M. E. Pozo Astigarraga and A. Prades Ibanez and J. Pretel and D. Price and M. Primavera and M. A. Principe Martin and R. Privara and T. Procter and M. L. Proffitt and N. Proklova and K. Prokofiev and G. Proto and J. Proudfoot and M. Przybycien and W. W. Przygoda and A. Psallidas and J. E. Puddefoot and D. Pudzha and D. Pyatiizbyantseva and J. Qian and D. Qichen and Y. Qin and T. Qiu and A. Quadt and M. Queitsch-Maitland and G. Quetant and R. P. Quinn and G. Rabanal Bolanos and D. Rafanoharana and F. Raffaeli and F. Ragusa and J. L. Rainbolt and J. A. Raine and S. Rajagopalan and E. Ramakoti and I. A. Ramirez-Berend and K. Ran and N. P. Rapheeha and H. Rasheed and V. Raskina and D. F. Rassloff and A. Rastogi and S. Rave and S. Ravera and B. Ravina and I. Ravinovich and M. Raymond and A. L. Read and N. P. Readioff and D. M. Rebuzzi and G. Redlinger and A. S. Reed and K. Reeves and J. A. Reidelsturz and D. Reikher and A. Rej and C. Rembser and M. Renda and F. Renner and A. G. Rennie and A. L. Rescia and S. Resconi and M. Ressegotti and S. Rettie and J. G. Reyes Rivera and E. Reynolds and O. L. Rezanova and P. Reznicek and H. Riani and N. Ribaric and E. Ricci and R. Richter and S. Richter and E. Richter-Was and M. Ridel and S. Ridouani and P. Rieck and P. Riedler and E. M. Riefel and J. O. Rieger and M. Rijssenbeek and M. Rimoldi and L. Rinaldi and P. Rincke and T. T. Rinn and M. P. Rinnagel and G. Ripellino and I. Riu and J. C. Rivera Vergara and F. Rizatdinova and E. Rizvi and B. R. Roberts and S. H. Robertson and D. Robinson and C. M. Robles Gajardo and M. Robles Manzano and A. Robson and A. Rocchi and C. Roda and S. Rodriguez Bosca and Y. Rodriguez Garcia and A. Rodriguez Rodriguez and A. M. Rodríguez Vera and S. Roe and J. T. Roemer and A. R. Roepe-Gier and O. Røhne and R. A. Rojas and C. P. A. Roland and J. Roloff and A. Romaniouk and E. Romano and M. Romano and A. C. Romero Hernandez and N. Rompotis and L. Roos and S. Rosati and B. J. Rosser and E. Rossi and L. P. Rossi and L. Rossini and R. Rosten and M. Rotaru and B. Rottler and C. Rougier and D. Rousseau and D. Rousso and A. Roy and S. Roy-Garand and A. Rozanov and Z. M. A. Rozario and Y. Rozen and A. Rubio Jimenez and A. J. Ruby and V. H. Ruelas Rivera and T. A. Ruggeri and A. Ruggiero and A. Ruiz-Martinez and A. Rummler and Z. Rurikova and N. A. Rusakovich and H. L. Russell and G. Russo and J. P. Rutherfoord and S. Rutherford Colmenares and M. Rybar and E. B. Rye and A. Ryzhov and J. A. Sabater Iglesias and P. Sabatini and H. F-W. Sadrozinski and F. Safai Tehrani and B. Safarzadeh Samani and S. Saha and M. Sahinsoy and A. Saibel and M. Saimpert and M. Saito and T. Saito and A. Sala and D. Salamani and A. Salnikov and J. Salt and A. Salvador Salas and D. Salvatore and F. Salvatore and A. Salzburger and D. Sammel and E. Sampson and D. Sampsonidis and D. Sampsonidou and J. Sánchez and V. Sanchez Sebastian and H. Sandaker and C. O. Sander and J. A. Sandesara and M. Sandhoff and C. Sandoval and L. Sanfilippo and D. P. C. Sankey and T. Sano and A. Sansoni and L. Santi and C. Santoni and H. Santos and A. Santra and E. Sanzani and K. A. Saoucha and J. G. Saraiva and J. Sardain and O. Sasaki and K. Sato and C. Sauer and E. Sauvan and P. Savard and R. Sawada and C. Sawyer and L. Sawyer and C. Sbarra and A. Sbrizzi and T. Scanlon and J. Schaarschmidt and U. Schäfer and A. C. Schaffer and D. Schaile and R. D. Schamberger and C. Scharf and M. M. Schefer and V. A. Schegelsky and D. Scheirich and M. Schernau and C. Scheulen and C. Schiavi and M. Schioppa and B. Schlag and K. E. Schleicher and S. Schlenker and J. Schmeing and M. A. Schmidt and K. Schmieden and C. Schmitt and N. Schmitt and S. Schmitt and L. Schoeffel and A. Schoening and P. G. Scholer and E. Schopf and M. Schott and J. Schovancova and S. Schramm and T. Schroer and H-C. Schultz-Coulon and M. Schumacher and B. A. Schumm and Ph. Schune and A. J. Schuy and H. R. Schwartz and A. Schwartzman and T. A. Schwarz and Ph. Schwemling and R. Schwienhorst and F. G. Sciacca and A. Sciandra and G. Sciolla and F. Scuri and C. D. Sebastiani and K. Sedlaczek and S. C. Seidel and A. Seiden and B. D. Seidlitz and C. Seitz and J. M. Seixas and G. Sekhniaidze and L. Selem and N. Semprini-Cesari and D. Sengupta and V. Senthilkumar and L. Serin and M. Sessa and H. Severini and F. Sforza and A. Sfyrla and Q. Sha and E. Shabalina and A. H. Shah and R. Shaheen and J. D. Shahinian and D. Shaked Renous and L. Y. Shan and M. Shapiro and A. Sharma and A. S. Sharma and P. Sharma and P. B. Shatalov and K. Shaw and S. M. Shaw and Q. Shen and D. J. Sheppard and P. Sherwood and L. Shi and X. Shi and C. O. Shimmin and J. D. Shinner and I. P. J. Shipsey and S. Shirabe and M. Shiyakova and M. J. Shochet and J. Shojaii and D. R. Shope and B. Shrestha and S. Shrestha and M. J. Shroff and P. Sicho and A. M. Sickles and E. Sideras Haddad and A. C. Sidley and A. Sidoti and F. Siegert and Dj. Sijacki and F. Sili and J. M. Silva and I. Silva Ferreira and M. V. Silva Oliveira and S. B. Silverstein and S. Simion and R. Simoniello and E. L. Simpson and H. Simpson and L. R. Simpson and N. D. Simpson and S. Simsek and S. Sindhu and P. Sinervo and S. Singh and S. Sinha and M. Sioli and I. Siral and E. Sitnikova and J. Sjölin and A. Skaf and E. Skorda and P. Skubic and M. Slawinska and V. Smakhtin and B. H. Smart and S. Yu. Smirnov and Y. Smirnov and L. N. Smirnova and O. Smirnova and A. C. Smith and D. R. Smith and E. A. Smith and H. A. Smith and J. L. Smith and R. Smith and M. Smizanska and K. Smolek and A. A. Snesarev and S. R. Snider and H. L. Snoek and S. Snyder and R. Sobie and A. Soffer and C. A. Solans Sanchez and E. Yu. Soldatov and U. Soldevila and A. A. Solodkov and S. Solomon and A. Soloshenko and K. Solovieva and O. V. Solovyanov and P. Sommer and A. Sonay and W. Y. Song and A. Sopczak and A. L. Sopio and F. Sopkova and J. D. Sorenson and I. R. Sotarriva Alvarez and V. Sothilingam and O. J. Soto Sandoval and S. Sottocornola and R. Soualah and Z. Soumaimi and D. South and N. Soybelman and S. Spagnolo and M. Spalla and D. Sperlich and G. Spigo and S. Spinali and B. Spisso and D. P. Spiteri and M. Spousta and E. J. Staats and R. Stamen and A. Stampekis and M. Standke and E. Stanecka and W. Stanek-Maslouska and M. V. Stange and B. Stanislaus and M. M. Stanitzki and B. Stapf and E. A. Starchenko and G. H. Stark and J. Stark and P. Staroba and P. Starovoitov and S. Stärz and R. Staszewski and G. Stavropoulos and A. Stefl and P. Steinberg and B. Stelzer and H. J. Stelzer and O. Stelzer-Chilton and H. Stenzel and T. J. Stevenson and G. A. Stewart and J. R. Stewart and M. C. Stockton and G. Stoicea and M. Stolarski and S. Stonjek and A. Straessner and J. Strandberg and S. Strandberg and M. Stratmann and M. Strauss and T. Strebler and P. Strizenec and R. Ströhmer and D. M. Strom and R. Stroynowski and A. Strubig and S. A. Stucci and B. Stugu and J. Stupak and N. A. Styles and D. Su and S. Su and W. Su and X. Su and D. Suchy and K. Sugizaki and V. V. Sulin and M. J. Sullivan and D. M. S. Sultan and L. Sultanaliyeva and S. Sultansoy and T. Sumida and S. Sun and O. Sunneborn Gudnadottir and N. Sur and M. R. Sutton and H. Suzuki and M. Svatos and M. Swiatlowski and T. Swirski and I. Sykora and M. Sykora and T. Sykora and D. Ta and K. Tackmann and A. Taffard and R. Tafirout and J. S. Tafoya Vargas and Y. Takubo and M. Talby and A. A. Talyshev and K. C. Tam and N. M. Tamir and A. Tanaka and J. Tanaka and R. Tanaka and M. Tanasini and Z. Tao and S. Tapia Araya and S. Tapprogge and A. Tarek Abouelfadl Mohamed and S. Tarem and K. Tariq and G. Tarna and G. F. Tartarelli and M. J. Tartarin and P. Tas and M. Tasevsky and E. Tassi and A. C. Tate and G. Tateno and Y. Tayalati and G. N. Taylor and W. Taylor and R. Teixeira De Lima and P. Teixeira-Dias and J. J. Teoh and K. Terashi and J. Terron and S. Terzo and M. Testa and R. J. Teuscher and A. Thaler and O. Theiner and N. Themistokleous and T. Theveneaux-Pelzer and O. Thielmann and D. W. Thomas and J. P. Thomas and E. A. Thompson and P. D. Thompson and E. Thomson and R. E. Thornberry and C. Tian and Y. Tian and V. Tikhomirov and Yu. A. Tikhonov and S. Timoshenko and D. Timoshyn and E. X. L. Ting and P. Tipton and A. Tishelman-Charny and S. H. Tlou and K. Todome and S. Todorova-Nova and S. Todt and L. Toffolin and M. Togawa and J. Tojo and S. Tokár and K. Tokushuku and O. Toldaiev and R. Tombs and M. Tomoto and L. Tompkins and K. W. Topolnicki and E. Torrence and H. Torres and E. Torró Pastor and M. Toscani and C. Tosciri and M. Tost and D. R. Tovey and I. S. Trandafir and T. Trefzger and A. Tricoli and I. M. Trigger and S. Trincaz-Duvoid and D. A. Trischuk and B. Trocmé and A. Tropina and L. Truong and M. Trzebinski and A. Trzupek and F. Tsai and M. Tsai and A. Tsiamis and P. V. Tsiareshka and S. Tsigaridas and A. Tsirigotis and V. Tsiskaridze and E. G. Tskhadadze and M. Tsopoulou and Y. Tsujikawa and I. I. Tsukerman and V. Tsulaia and S. Tsuno and K. Tsuri and D. Tsybychev and Y. Tu and A. Tudorache and V. Tudorache and A. N. Tuna and S. Turchikhin and I. Turk Cakir and R. Turra and T. Turtuvshin and P. M. Tuts and S. Tzamarias and E. Tzovara and F. Ukegawa and P. A. Ulloa Poblete and E. N. Umaka and G. Unal and A. Undrus and G. Unel and J. Urban and P. Urrejola and G. Usai and R. Ushioda and M. Usman and Z. Uysal and V. Vacek and B. Vachon and T. Vafeiadis and A. Vaitkus and C. Valderanis and E. Valdes Santurio and M. Valente and S. Valentinetti and A. Valero and E. Valiente Moreno and A. Vallier and J. A. Valls Ferrer and D. R. Van Arneman and T. R. Van Daalen and A. Van Der Graaf and P. Van Gemmeren and M. Van Rijnbach and S. Van Stroud and I. Van Vulpen and P. Vana and M. Vanadia and W. Vandelli and E. R. Vandewall and D. Vannicola and L. Vannoli and R. Vari and E. W. Varnes and C. Varni and T. Varol and D. Varouchas and L. Varriale and K. E. Varvell and M. E. Vasile and L. Vaslin and G. A. Vasquez and A. Vasyukov and L. M. Vaughan and R. Vavricka and T. Vazquez Schroeder and J. Veatch and V. Vecchio and M. J. Veen and I. Veliscek and L. M. Veloce and F. Veloso and S. Veneziano and A. Ventura and S. Ventura Gonzalez and A. Verbytskyi and M. Verducci and C. Vergis and M. Verissimo De Araujo and W. Verkerke and J. C. Vermeulen and C. Vernieri and M. Vessella and M. C. Vetterli and A. Vgenopoulos and N. Viaux Maira and T. Vickey and O. E. Vickey Boeriu and G. H. A. Viehhauser and L. Vigani and M. Villa and M. Villaplana Perez and E. M. Villhauer and E. Vilucchi and M. G. Vincter and A. Visibile and C. Vittori and I. Vivarelli and E. Voevodina and F. Vogel and J. C. Voigt and P. Vokac and Yu. Volkotrub and J. Von Ahnen and E. Von Toerne and B. Vormwald and V. Vorobel and K. Vorobev and M. Vos and K. Voss and M. Vozak and L. Vozdecky and N. Vranjes and M. Vranjes Milosavljevic and M. Vreeswijk and N. K. Vu and R. Vuillermet and O. Vujinovic and I. Vukotic and S. Wada and C. Wagner and J. M. Wagner and W. Wagner and S. Wahdan and H. Wahlberg and M. Wakida and J. Walder and R. Walker and W. Walkowiak and A. Wall and E. J. Wallin and T. Wamorkar and A. Z. Wang and C. Wang and H. Wang and J. Wang and P. Wang and R. Wang and S. M. Wang and S. Wang and T. Wang and W. T. Wang and W. Wang and X. Wang and Y. Wang and Z. Wang and A. Warburton and R. J. Ward and N. Warrack and S. Waterhouse and A. T. Watson and H. Watson and M. F. Watson and E. Watton and G. Watts and B. M. Waugh and J. M. Webb and C. Weber and H. A. Weber and M. S. Weber and S. M. Weber and C. Wei and Y. Wei and A. R. Weidberg and E. J. Weik and J. Weingarten and C. Weiser and C. J. Wells and T. Wenaus and B. Wendland and T. Wengler and N. S. Wenke and N. Wermes and M. Wessels and A. M. Wharton and A. S. White and A. White and M. J. White and D. Whiteson and L. Wickremasinghe and W. Wiedenmann and M. Wielers and C. Wiglesworth and D. J. Wilbern and H. G. Wilkens and J. J. H. Wilkinson and D. M. Williams and H. H. Williams and S. Williams and S. Willocq and B. J. Wilson and P. J. Windischhofer and F. I. Winkel and F. Winklmeier and B. T. Winter and J. K. Winter and M. Wittgen and M. Wobisch and T. Wojtkowski and Z. Wolffs and J. Wollrath and M. W. Wolter and H. Wolters and M. C. Wong and E. L. Woodward and S. D. Worm and B. K. Wosiek and K. W. Woźniak and S. Wozniewski and K. Wraight and C. Wu and M. Wu and S. L. Wu and X. Wu and Y. Wu and Z. Wu and J. Wuerzinger and T. R. Wyatt and B. M. Wynne and S. Xella and L. Xia and M. Xia and M. Xie and S. Xin and A. Xiong and J. Xiong and D. Xu and H. Xu and L. Xu and R. Xu and T. Xu and Y. Xu and Z. Xu and B. Yabsley and S. Yacoob and Y. Yamaguchi and E. Yamashita and H. Yamauchi and T. Yamazaki and Y. Yamazaki and J. Yan and S. Yan and Z. Yan and H. J. Yang and H. T. Yang and S. Yang and T. Yang and X. Yang and Y. Yang and Z. Yang and W-M. Yao and H. Ye and J. Ye and S. Ye and X. Ye and Y. Yeh and I. Yeletskikh and B. Yeo and M. R. Yexley and T. P. Yildirim and P. Yin and K. Yorita and S. Younas and C. J. S. Young and C. Young and C. Yu and Y. Yu and J. Yuan and M. Yuan and R. Yuan and L. Yue and M. Zaazoua and B. Zabinski and E. Zaid and Z. K. Zak and T. Zakareishvili and S. Zambito and J. A. Zamora Saa and J. Zang and D. Zanzi and O. Zaplatilek and C. Zeitnitz and H. Zeng and J. C. Zeng and D. T. Zenger, Jr and O. Zenin and T. Ženiš and S. Zenz and S. Zerradi and D. Zerwas and M. Zhai and D. F. Zhang and J. Zhang and K. Zhang and L. Zhang and P. Zhang and R. Zhang and S. Zhang and T. Zhang and X. Zhang and Y. Zhang and Z. Zhang and H. Zhao and T. Zhao and Y. Zhao and Z. Zhao and A. Zhemchugov and J. Zheng and K. Zheng and X. Zheng and Z. Zheng and D. Zhong and B. Zhou and H. Zhou and N. Zhou and Y. Zhou and C. G. Zhu and J. Zhu and X. Zhu and Y. Zhu and X. Zhuang and K. Zhukov and N. I. Zimine and J. Zinsser and M. Ziolkowski and L. Živković and A. Zoccoli and K. Zoch and T. G. Zorbas and O. Zormpa and W. Zou and L. Zwalinski}, doi = {10.1103/PhysRevLett.134.121801}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for dark matter produced in association with a dark higgs boson in the bb¯ final state using pp collisions at s=13 TeV with the ATLAS detector}, volume = {134}, year = {2025}, }
• (2025). Conformal perturbation theory from open string field theory. PRL, 134(12), 121601. (www)

  @article{ , abstract = {Conformal boundary conditions in two-dimensional conformal field theories are still mostly an uncharted territory. Even less is known about the relevant boundary deformations that connect them. A natural approach to the problem is via conformal perturbation theory, which, however, becomes quickly intractable. Using the formalism of open string field theory, we construct the corresponding classical solution, from which we can easily extract the boundary theory data. As a simple illustration we calculate the boundary degeneracy g to next-to-leading order for a generic theory.}, archive = {J_PRL}, author = {Jaroslav Scheinpflug and Martin Schnabl}, doi = {10.1103/PhysRevLett.134.121601}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121601}, shortjournal = {Phys. Rev. Lett.}, title = {Conformal perturbation theory from open string field theory}, volume = {134}, year = {2025}, }
• (2025). Quantum mechanics of a spherically symmetric causal diamond in minkowski spacetime. PRL, 134(12), 121501. (www)

  @article{ , abstract = {We construct the phase space of a spherically symmetric causal diamond in ( )-dimensional Minkowski spacetime. Utilizing the covariant phase space formalism, we identify the relevant degrees of freedom that localize to the -dimensional bifurcate horizon and, upon canonical quantization, determine their commutators. On this phase space, we find two Iyer-Wald charges. The first of these charges, proportional to the area of the causal diamond, is responsible for shifting the null time along the horizon and has been well documented in the literature. The second charge is much less understood, being integrable for only if we allow for field-dependent diffeomorphisms and is responsible for changing the size of the causal diamond.}, archive = {J_PRL}, author = {Mathew W. Bub and Temple He and Prahar Mitra and Yiwen Zhang and Kathryn M. Zurek}, doi = {10.1103/PhysRevLett.134.121501}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121501}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum mechanics of a spherically symmetric causal diamond in minkowski spacetime}, volume = {134}, year = {2025}, }
• (2025). Which is which? identification of the two compact objects in gravitational-wave binaries. PRL, 134(12), 121402. (www)

  @article{ , abstract = {Compact objects observed in gravitational-wave astronomy so far always come in pairs and never individually. Identifying the two components of a binary system is a delicate operation that is often taken for granted. The labeling procedure (i.e., which is object “1” and which is object “2”) effectively acts as systematics, or, equivalently, an unspecified prior, in gravitational-wave data inference. The common approach is to label the objects solely by their masses, on a sample-by-sample basis. We show that object identification can instead be tackled using the posterior distribution as a whole. We frame the problem in terms of constrained clustering—a flavor of semisupervised machine learning—and find that unfolding the labeling systematics can significantly impact, and arguably improve, our interpretation of the data. In particular, the precision of black-hole spin measurements improves by up to 50%, multimodalities and tails tend to disappear, posteriors become closer to Gaussian distributions, and the identification of the nature of the object (i.e., black hole vs neutron star) is facilitated. We estimate that about 10% of the LIGO/Virgo posterior samples are affected by this relabeling, i.e., they might have been attributed to the other compact object in the observed binaries.}, archive = {J_PRL}, author = {Davide Gerosa and Viola De Renzis and Federica Tettoni and Matthew Mould and Alberto Vecchio and Costantino Pacilio}, doi = {10.1103/PhysRevLett.134.121402}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121402}, shortjournal = {Phys. Rev. Lett.}, title = {Which is which? identification of the two compact objects in gravitational-wave binaries}, volume = {134}, year = {2025}, }
• (2025). Masking the equation-of-state effects in binary neutron star mergers. PRL, 134(12), 121401. (www)

  @article{ , abstract = {Recent nonmagnetized studies of binary neutron star mergers have indicated the possibility of identifying equation-of-state features, such as a phase transition or a quark-hadron crossover, based on the frequency shift of the main peak in the postmerger gravitational wave spectrum. By performing a series of general relativistic, magnetohydrodynamic simulations we show that similar frequency shifts can be obtained due to the effect of the magnetic field. The existing degeneracy can either mask or nullify a shift due to a specific equation-of-state feature, and therefore the interpretation of observational data is more complicated than previously thought, requiring a more complete treatment that would necessarily include the neutron star’s magnetic field.}, archive = {J_PRL}, author = {Antonios Tsokaros and Jamie Bamber and Milton Ruiz and Stuart L. Shapiro}, doi = {10.1103/PhysRevLett.134.121401}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121401}, shortjournal = {Phys. Rev. Lett.}, title = {Masking the equation-of-state effects in binary neutron star mergers}, volume = {134}, year = {2025}, }
• (2025). Search for the anomalous events detected by ANITA using the pierre auger observatory. PRL, 134(12), 121003. (www)

  @article{ , abstract = {A dedicated search for upward-going air showers at zenith angles exceeding 110° and energies has been performed using the Fluorescence Detector of the Pierre Auger Observatory. The search is motivated by two “anomalous” radio pulses observed by the ANITA flights I and III that appear inconsistent with the standard model of particle physics. Using simulations of both regular cosmic-ray showers and upward-going events, a selection procedure has been defined to separate potential upward-going candidate events and the corresponding exposure has been calculated in the energy range [0.1–33] EeV. One event has been found in the search period between January 1, 2004, and December 31, 2018, consistent with an expected background of events from misreconstructed cosmic-ray showers. This translates to an upper bound on the integral flux of and for an and spectrum, respectively. An upward-going flux of showers normalized to the ANITA observations is shown to predict over 34 events for an spectrum and over 8.1 events for a conservative spectrum, in strong disagreement with the interpretation of the anomalous events as upward-going showers.}, archive = {J_PRL}, author = {Pierre Auger Collaboration and A. Abdul Halim and P. Abreu and M. Aglietta and I. Allekotte and K. Almeida Cheminant and A. Almela and R. Aloisio and J. Alvarez-Muñiz and J. Ammerman Yebra and G. A. Anastasi and L. Anchordoqui and B. Andrada and S. Andringa and L. Apollonio and C. Aramo and P. R. Araújo Ferreira and E. Arnone and J. C. Arteaga Velázquez and P. Assis and G. Avila and E. Avocone and A. Bakalova and F. Barbato and A. Bartz Mocellin and J. A. Bellido and C. Berat and M. E. Bertaina and G. Bhatta and M. Bianciotto and P. L. Biermann and V. Binet and K. Bismark and T. Bister and J. Biteau and J. Blazek and C. Bleve and J. Blümer and M. Boháčová and D. Boncioli and C. Bonifazi and L. Bonneau Arbeletche and N. Borodai and J. Brack and P. G. Brichetto Orchera and F. L. Briechle and A. Bueno and S. Buitink and M. Buscemi and M. Büsken and A. Bwembya and K. S. Caballero-Mora and S. Cabana-Freire and L. Caccianiga and F. Campuzano and I. Caracas and R. Caruso and A. Castellina and F. Catalani and G. Cataldi and L. Cazon and M. Cerda and A. Cermenati and J. A. Chinellato and J. Chudoba and L. Chytka and R. W. Clay and A. C. Cobos Cerutti and R. Colalillo and M. R. Coluccia and R. Conceição and A. Condorelli and G. Consolati and M. Conte and F. Convenga and D. Correia dos Santos and P. J. Costa and C. E. Covault and M. Cristinziani and C. S. Cruz Sanchez and S. Dasso and K. Daumiller and B. R. Dawson and R. M. de Almeida and J. de Jesús and S. J. de Jong and J. R. T. de Mello Neto and I. De Mitri and J. de Oliveira and D. de Oliveira Franco and F. de Palma and V. de Souza and B. P. de Souza de Errico and E. De Vito and A. Del Popolo and O. Deligny and N. Denner and L. Deval and A. di Matteo and M. Dobre and C. Dobrigkeit and J. C. D’Olivo and L. M. Domingues Mendes and Q. Dorosti and J. C. dos Anjos and R. C. dos Anjos and J. Ebr and F. Ellwanger and M. Emam and R. Engel and I. Epicoco and M. Erdmann and A. Etchegoyen and C. Evoli and H. Falcke and G. Farrar and A. C. Fauth and N. Fazzini and F. Feldbusch and F. Fenu and A. Fernandes and B. Fick and J. M. Figueira and A. Filipčič and T. Fitoussi and B. Flaggs and T. Fodran and T. Fujii and A. Fuster and C. Galea and C. Galelli and B. García and C. Gaudu and H. Gemmeke and F. Gesualdi and A. Gherghel-Lascu and P. L. Ghia and U. Giaccari and J. Glombitza and F. Gobbi and F. Gollan and G. Golup and M. Gómez Berisso and P. F. Gómez Vitale and J. P. Gongora and J. M. González and N. González and D. Góra and A. Gorgi and M. Gottowik and T. D. Grubb and F. Guarino and G. P. Guedes and E. Guido and L. Gülzow and S. Hahn and P. Hamal and M. R. Hampel and P. Hansen and D. Harari and V. M. Harvey and A. Haungs and T. Hebbeker and C. Hojvat and J. R. Hörandel and P. Horvath and M. Hrabovský and T. Huege and A. Insolia and P. G. Isar and P. Janecek and V. Jilek and J. A. Johnsen and J. Jurysek and K.-H. Kampert and B. Keilhauer and A. Khakurdikar and V. V. Kizakke Covilakam and H. O. Klages and M. Kleifges and F. Knapp and J. Köhler and N. Kunka and B. L. Lago and N. Langner and M. A. Leigui de Oliveira and Y. Lema-Capeans and A. Letessier-Selvon and I. Lhenry-Yvon and L. Lopes and L. Lu and Q. Luce and J. P. Lundquist and A. Machado Payeras and M. Majercakova and D. Mandat and B. C. Manning and P. Mantsch and F. M. Mariani and A. G. Mariazzi and I. C. Mariş and G. Marsella and D. Martello and S. Martinelli and O. Martínez Bravo and M. A. Martins and M. Mastrodicasa and H.-J. Mathes and J. Matthews and G. Matthiae and E. Mayotte and S. Mayotte and P. O. Mazur and G. Medina-Tanco and J. Meinert and D. Melo and A. Menshikov and C. Merx and S. Michal and M. I. Micheletti and L. Miramonti and S. Mollerach and F. Montanet and L. Morejon and C. Morello and K. Mulrey and R. Mussa and W. M. Namasaka and S. Negi and L. Nellen and K. Nguyen and G. Nicora and M. Niechciol and D. Nitz and D. Nosek and V. Novotny and L. Nožka and A. Nucita and L. A. Núñez and C. Oliveira and M. Palatka and J. Pallotta and S. Panja and G. Parente and T. Paulsen and J. Pawlowsky and M. Pech and J. Pȩkala and R. Pelayo and L. A. S. Pereira and E. E. Pereira Martins and J. Perez Armand and C. Pérez Bertolli and L. Perrone and S. Petrera and C. Petrucci and T. Pierog and M. Pimenta and M. Platino and B. Pont and M. Pothast and M. Pourmohammad Shahvar and P. Privitera and M. Prouza and S. Querchfeld and J. Rautenberg and D. Ravignani and J. V. Reginatto Akim and M. Reininghaus and J. Ridky and F. Riehn and M. Risse and V. Rizi and W. Rodrigues de Carvalho and E. Rodriguez and J. Rodriguez Rojo and M. J. Roncoroni and S. Rossoni and M. Roth and E. Roulet and A. C. Rovero and P. Ruehl and A. Saftoiu and M. Saharan and F. Salamida and H. Salazar and G. Salina and J. D. Sanabria Gomez and F. Sánchez and E. M. Santos and E. Santos and F. Sarazin and R. Sarmento and R. Sato and P. Savina and C. M. Schäfer and V. Scherini and H. Schieler and M. Schimassek and M. Schimp and D. Schmidt and O. Scholten and H. Schoorlemmer and P. Schovánek and F. G. Schröder and J. Schulte and T. Schulz and S. J. Sciutto and M. Scornavacche and A. Sedoski and A. Segreto and S. Sehgal and S. U. Shivashankara and G. Sigl and G. Silli and O. Sima and K. Simkova and F. Simon and R. Smau and R. Šmída and P. Sommers and J. F. Soriano and R. Squartini and M. Stadelmaier and S. Stanič and J. Stasielak and P. Stassi and S. Strähnz and M. Straub and T. Suomijärvi and A. D. Supanitsky and Z. Svozilikova and Z. Szadkowski and F. Tairli and A. Tapia and C. Taricco and C. Timmermans and O. Tkachenko and P. Tobiska and C. J. Todero Peixoto and B. Tomé and Z. Torrès and A. Travaini and P. Travnicek and C. Trimarelli and M. Tueros and M. Unger and L. Vaclavek and M. Vacula and J. F. Valdés Galicia and L. Valore and E. Varela and A. Vásquez-Ramírez and D. Veberič and C. Ventura and I. D. Vergara Quispe and V. Verzi and J. Vicha and J. Vink and S. Vorobiov and C. Watanabe and A. A. Watson and A. Weindl and L. Wiencke and H. Wilczyński and D. Wittkowski and B. Wundheiler and B. Yue and A. Yushkov and O. Zapparrata and E. Zas and D. Zavrtanik and M. Zavrtanik and R. Prechelt and A. Romero-Wolf and S. Wissel and A. Zeolla}, doi = {10.1103/PhysRevLett.134.121003}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121003}, shortjournal = {Phys. Rev. Lett.}, title = {Search for the anomalous events detected by ANITA using the pierre auger observatory}, volume = {134}, year = {2025}, }
• (2025). Dark matter direct detection experiments are sensitive to the millicharged background. PRL, 134(12), 121002. (www)

  @article{ , abstract = {We show that dark matter direct detection experiments are sensitive to the existence of particles with a small effective charge (for instance, via couplings to a kinetically mixed, low-mass dark photon). Our forecasts do not depend on these particles comprising a significant fraction of the dark matter. Rather, these experiments are sensitive to the irreducible abundance produced in the early Universe through the freeze-in mechanism. We find that ongoing and proposed direct detection experiments will have world-leading sensitivity to effective charges Q ∼ 10 − 12 across 9 orders of magnitude in mass, corresponding to a dark matter subfraction as low as ∼ 10 − 3 .}, archive = {J_PRL}, author = {Ella Iles and Saniya Heeba and Katelin Schutz}, doi = {10.1103/PhysRevLett.134.121002}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121002}, shortjournal = {Phys. Rev. Lett.}, title = {Dark matter direct detection experiments are sensitive to the millicharged background}, volume = {134}, year = {2025}, }
• (2025). New physics decaying into metastable particles: Impact on cosmic neutrinos. PRL, 134(12), 121001. (www)

  @article{ , abstract = {We investigate decays of hypothetical unstable new physics particles into metastable species such as muons, pions, or kaons in the early Universe, when temperatures are in the MeV range, and study how they affect cosmic neutrinos. We demonstrate that the nontrivial dynamics of metastables in the plasma alters the impact of the new physics particles on the neutrino population, including the effective number of neutrino degrees of freedom, N eff , modifies neutrino spectral distortions, and may induce asymmetries in neutrino and antineutrino energy distributions. These modifications have important implications for observables such as big bang nucleosynthesis and the cosmic microwave background, especially in light of upcoming cosmic microwave background observations aiming to reach percent-level precision on N eff . We illustrate our findings with a few examples of new physics particles and provide a computational tool available for further exploration.}, archive = {J_PRL}, author = {Kensuke Akita and Gideon Baur and Maksym Ovchynnikov and Thomas Schwetz and Vsevolod Syvolap}, doi = {10.1103/PhysRevLett.134.121001}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {121001}, shortjournal = {Phys. Rev. Lett.}, title = {New physics decaying into metastable particles: Impact on cosmic neutrinos}, volume = {134}, year = {2025}, }
• (2025). Toward heisenberg limit without critical slowing down via quantum reinforcement learning. PRL, 134(12), 120803. (www)

  @article{ , abstract = {Critical ground states of quantum many-body systems have emerged as vital resources for quantum-enhanced sensing. Traditional methods to prepare these states often rely on adiabatic evolution, which may diminish the quantum sensing advantage. In this Letter, we propose a quantum reinforcement learning (QRL) enhanced critical sensing protocol for quantum many-body systems with exotic phase diagrams. Starting from product states and utilizing QRL-discovered gate sequences, we explore sensing accuracy in the presence of unknown external magnetic fields, covering both local and global regimes. Our results demonstrate that QRL-learned sequences reach the finite quantum speed limit and generalize effectively across systems of arbitrary size, ensuring accuracy regardless of preparation time. This method can robustly achieve Heisenberg and super-Heisenberg limits, even in noisy environments with practical Pauli measurements. Our study highlights the efficacy of QRL in enabling precise quantum state preparation, thereby advancing scalable, high-accuracy quantum critical sensing.}, archive = {J_PRL}, author = {Hang Xu and Tailong Xiao and Jingzheng Huang and Ming He and Jianping Fan and Guihua Zeng}, doi = {10.1103/PhysRevLett.134.120803}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120803}, shortjournal = {Phys. Rev. Lett.}, title = {Toward heisenberg limit without critical slowing down via quantum reinforcement learning}, volume = {134}, year = {2025}, }
• (2025). Robust noise suppression and quantum sensing by continuous phased dynamical decoupling. PRL, 134(12), 120802. (www)

  @article{ , abstract = {We propose and demonstrate experimentally continuous phased dynamical decoupling (CPDD), where we apply a continuous field with discrete phase changes for quantum sensing and robust compensation of environmental and amplitude noise. CPDD does not use short pulses, making it particularly suitable for experiments with limited driving power or nuclear magnetic resonance at high magnetic fields. It requires control of the timing of the phase changes, offering much greater precision than the Rabi frequency control needed in standard continuous sensing schemes. We successfully apply our method to nanoscale nuclear magnetic resonance and combine it with quantum heterodyne detection, achieving microhertz uncertainty in the estimated signal frequency for a 120 s measurement. Our Letter expands significantly the applicability of dynamical decoupling and opens the door for a wide range of experiments, e.g., in nitrogen-vacancy centers, trapped ions, or trapped atoms.}, archive = {J_PRL}, author = {Daniel Louzon and Genko T. Genov and Nicolas Staudenmaier and Florian Frank and Johannes Lang and Matthew L. Markham and Alex Retzker and Fedor Jelezko}, doi = {10.1103/PhysRevLett.134.120802}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120802}, shortjournal = {Phys. Rev. Lett.}, title = {Robust noise suppression and quantum sensing by continuous phased dynamical decoupling}, volume = {134}, year = {2025}, }
• (2025). Site-selective cavity readout and classical error correction of a 5-bit atomic register. PRL, 134(12), 120801. (www)

  @article{ , abstract = {Optical cavities can provide fast and nondestructive readout of individual atomic qubits; however, scaling up to many qubits remains a challenge. Using locally addressed excited-state Stark shifts to tune atoms out of resonance, we realize site-selective hyperfine-state cavity readout across a ten-site array. The state discrimination fidelity is 0.994(1) for one atom and 0.989(2) averaged over the entire array at a survival probability of 0.975(1). To further speed up array readout, we demonstrate adaptive search strategies utilizing global or subset checks. Finally, we demonstrate repeated rounds of classical error correction, showing exponential suppression of logical error and extending logical memory fivefold beyond the single-bit idling lifetime.}, archive = {J_PRL}, author = {Beili Hu and Josiah Sinclair and Edita Bytyqi and Michelle Chong and Alyssa Rudelis and Joshua Ramette and Zachary Vendeiro and Vladan Vuletić}, doi = {10.1103/PhysRevLett.134.120801}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120801}, shortjournal = {Phys. Rev. Lett.}, title = {Site-selective cavity readout and classical error correction of a 5-bit atomic register}, volume = {134}, year = {2025}, }
• (2025). Fast flux-activated leakage reduction for superconducting quantum circuits. PRL, 134(12), 120601. (www)

  @article{ , abstract = {Quantum computers will require quantum error correction to reach the low error rates necessary for solving problems that surpass the capabilities of conventional computers. One of the dominant errors limiting the performance of quantum error correction codes across multiple technology platforms is leakage out of the computational subspace arising from the multilevel structure of qubit implementations. Here, we present a resource-efficient universal leakage reduction unit for superconducting qubits using parametric flux modulation. This operation removes leakage down to our measurement inaccuracy of in approximately 50 ns with a low error of on the computational subspace, thereby reaching durations and fidelities comparable to those of single-qubit gates. We demonstrate that using the leakage reduction unit in repeated weight-two stabilizer measurements reduces the total number of detected errors in a scalable fashion to close to what can be achieved using leakage-rejection methods that do not scale. Our approach does not require additional control electronics or on-chip components and is applicable to both auxiliary and data qubits. These benefits make our method particularly attractive for mitigating leakage in large-scale quantum error correction circuits, a crucial requirement for the practical implementation of fault-tolerant quantum computation.}, archive = {J_PRL}, author = {Nathan Lacroix and Luca Hofele and Ants Remm and Othmane Benhayoune-Khadraoui and Alexander McDonald and Ross Shillito and Stefania Lazar and Christoph Hellings and François Swiadek and Dante Colao-Zanuz and Alexander Flasby and Mohsen Bahrami Panah and Michael Kerschbaum and Graham J. Norris and Alexandre Blais and Andreas Wallraff and Sebastian Krinner}, doi = {10.1103/PhysRevLett.134.120601}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120601}, shortjournal = {Phys. Rev. Lett.}, title = {Fast flux-activated leakage reduction for superconducting quantum circuits}, volume = {134}, year = {2025}, }
• (2025). Experimental demonstration of scalable cross-entropy benchmarking to detect measurement-induced phase transitions on a superconducting quantum processor. PRL, 134(12), 120401. (www)

  @article{ , abstract = {Quantum systems subject to random unitary evolution and measurements at random points in spacetime exhibit entanglement phase transitions which depend on the frequency of these measurements. Past work has experimentally observed entanglement phase transitions on near-term quantum computers, but the characterization approach using entanglement entropy is not scalable due to exponential overhead of quantum state tomography and postselection. Recently, an alternative protocol to detect entanglement phase transitions using linear cross entropy was proposed, attempting to eliminate both bottlenecks. Here, we report demonstrations of this protocol in systems with one-dimensional and all-to-all connectivities on IBM’s quantum hardware on up to 22 qubits, a regime which is presently inaccessible if postselection is required. We demonstrate data collapses onto scaling functions with critical exponents in semiquantitative agreement with theory. Our demonstration of the cross entropy benchmark (XEB) protocol paves the way for studies of measurement-induced entanglement phase transitions and associated critical phenomena on larger near-term quantum systems.}, archive = {J_PRL}, author = {Hirsh Kamakari and Jiace Sun and Yaodong Li and Jonathan J. Thio and Tanvi P. Gujarati and Matthew P. A. Fisher and Mario Motta and Austin J. Minnich}, doi = {10.1103/PhysRevLett.134.120401}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120401}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental demonstration of scalable cross-entropy benchmarking to detect measurement-induced phase transitions on a superconducting quantum processor}, volume = {134}, year = {2025}, }
• (2025). Bound entangled states are useful in prepare-and-measure scenarios. PRL, 134(12), 120203. (www)

  @article{ , abstract = {We show that bipartite bound entangled states make possible violations of correlation inequalities in the prepare-and-measure scenario. These inequalities are satisfied by all classical models as well as by all quantum models that do not feature entanglement. In contrast to the known Bell inequality violations from bound entangled states, we find that the violations in the prepare-and-measure scenario are sizeable and significantly noise-tolerant. Furthermore, we show that significantly stronger quantum correlations are made possible by considering bound entanglement with a larger dimension.}, archive = {J_PRL}, author = {Carles Roch i Carceller and Armin Tavakoli}, doi = {10.1103/PhysRevLett.134.120203}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120203}, shortjournal = {Phys. Rev. Lett.}, title = {Bound entangled states are useful in prepare-and-measure scenarios}, volume = {134}, year = {2025}, }
• (2025). Dual-capability machine learning models for quantum hamiltonian parameter estimation and dynamics prediction. PRL, 134(12), 120202. (www)

  @article{ , abstract = {Recent advancements in quantum hardware and classical computing simulations have significantly enhanced the accessibility of quantum system data, leading to an increased demand for precise descriptions and predictions of these systems. Accurate prediction of quantum Hamiltonian dynamics and identification of Hamiltonian parameters are crucial for advancements in quantum simulations, error correction, and control protocols. This Letter introduces a machine learning model with dual capabilities: it can deduce time-dependent Hamiltonian parameters from observed changes in local observables within quantum many-body systems, and it can predict the evolution of these observables based on Hamiltonian parameters. Our model’s validity was confirmed through theoretical simulations across various scenarios and further validated by two experiments. Initially, the model was applied to a nuclear magnetic resonance quantum computer, where it accurately predicted the dynamics of local observables. The model was then tested on a superconducting quantum computer with initially unknown Hamiltonian parameters, successfully inferring them. Our approach aims to enhance various quantum computing tasks, including parameter estimation, noise characterization, feedback processes, and quantum control optimization.}, archive = {J_PRL}, author = {Zheng An and Jiahui Wu and Zidong Lin and Xiaobo Yang and Keren Li and Bei Zeng}, doi = {10.1103/PhysRevLett.134.120202}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120202}, shortjournal = {Phys. Rev. Lett.}, title = {Dual-capability machine learning models for quantum hamiltonian parameter estimation and dynamics prediction}, volume = {134}, year = {2025}, }
• (2025). Phase-space measurements, decoherence, and classicality. PRL, 134(12), 120201. (www)

  @article{ , abstract = {The emergence of classical behavior in quantum theory is often ascribed to the interaction of a quantum system with its environment, which can be interpreted as environmental monitoring of the system. As a result, off-diagonal elements of the density matrix of the system are damped in the basis of a preferred observable, often taken to be the position, leading to the phenomenon of decoherence. This effect can be modeled dynamically in terms of a Lindblad equation driven by the position operator. Here the question of decoherence resulting from a monitoring of position and momentum, i.e., a phase-space measurement, by the environment is addressed. There is no standard quantum observable corresponding to the detection of phase-space points, which is forbidden by Heisenberg’s uncertainty principle. This issue is addressed by use of a coherent-state-based positive operator-valued measure for modeling phase-space monitoring by the environment. In this scheme, decoherence in phase space implies the diagonalization of the density matrix in both position and momentum representations. This is shown to be linked to a Lindblad equation where position and momentum appear as two independent Lindblad operators.}, archive = {J_PRL}, author = {Dorje C. Brody and Eva-Maria Graefe and Rishindra Melanathuru}, doi = {10.1103/PhysRevLett.134.120201}, journal = {Physical Review Letters}, month = {3}, number = {12}, pages = {120201}, shortjournal = {Phys. Rev. Lett.}, title = {Phase-space measurements, decoherence, and classicality}, volume = {134}, year = {2025}, }
• (2025). Erratum: Self-consistent extraction of spectroscopic bounds on light new physics [Phys. rev. lett. 130, 121801 (2023)]. PRL, 134(11), 119901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 119901 (2025)}, archive = {J_PRL}, author = {Cédric Delaunay and Jean-Philippe Karr and Teppei Kitahara and Jeroen C. J. Koelemeij and Yotam Soreq and Jure Zupan}, doi = {10.1103/PhysRevLett.134.119901}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {119901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Self-consistent extraction of spectroscopic bounds on light new physics [Phys. rev. lett. 130, 121801 (2023)]}, volume = {134}, year = {2025}, }
• (2025). Unbuckling mechanics of epithelial monolayers under compression. PRL, 134(11), 118402. (www)

  @article{ , abstract = {When cell sheets fold during development, their apical or basal surfaces constrict and cell shapes approach the geometric singularity in which these surfaces vanish. Here, we reveal the mechanical consequences of this geometric singularity for tissue folding in a minimal vertex model of an epithelial monolayer. In simulations of the buckling of the epithelium under compression and numerical solutions of the corresponding continuum model, we discover an “unbuckling” bifurcation: at large compression, the buckling amplitude can decrease with increasing compression. By asymptotic solution of the continuum equations, we reveal that this bifurcation comes with a large stiffening of the epithelium. Our results thus provide the mechanical basis for absorption of compressive stresses by tissue folds such as the cephalic furrow during germband extension in Drosophila .}, archive = {J_PRL}, author = {Chandraniva Guha Ray and Pierre A. Haas}, doi = {10.1103/PhysRevLett.134.118402}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {118402}, shortjournal = {Phys. Rev. Lett.}, title = {Unbuckling mechanics of epithelial monolayers under compression}, volume = {134}, year = {2025}, }
• (2025). Evolutionary advantage of cell size control. PRL, 134(11), 118401. (www)

  @article{ , abstract = {We analyze the advantage of cell size control strategies in growing populations under mortality constraints and show that growth-dependent mortality can select for accurate size control. We determine how mortality, noise, and nongenetic heritability of cell size impact long-term population growth. We derive an analytical expression for the optimal cell size. We demonstrate that size heritability enables selection to act on the distribution of cell sizes in a population to avoid viability thresholds and adapt to size- and growth-dependent mortality landscapes.}, archive = {J_PRL}, author = {Spencer Hobson-Gutierrez and Edo Kussell}, doi = {10.1103/PhysRevLett.134.118401}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {118401}, shortjournal = {Phys. Rev. Lett.}, title = {Evolutionary advantage of cell size control}, volume = {134}, year = {2025}, }
• (2025). Process-directed self-assembly of the frank-kasper a15 structure in linear, conformationally symmetric block copolymers. PRL, 134(11), 118102. (www)

  @article{ , abstract = {Protracted equilibration times and a multitude of competing periodically modulated structures are common characteristics of complex, self-assembled phases in block copolymer materials. These characteristics highlight the importance of designing processes to reproducibly direct the structure evolution of complex, spatially modulated structures. Using general symmetry considerations, we design a process that deterministically transforms the common, double-gyroid (DG) phase of linear diblock copolymers into a metastable A15 structure by irreversibly switching a conformationally symmetric A B B ′ diblock copolymer into an A B A ′ triblock copolymer. Key to the fabrication of the Frank-Kasper A15 structure is the nonmonotonic time evolution of the segregation that allows us to partition the large unit cell of the DG phase into 8 equivalent A15 units. Comparison between dynamic self-consistent field theory and particle-based simulations demonstrates the robustness of the designed pathway against thermal fluctuations and memory effects due to the underlying Rouse dynamics. Metastable structures that can be accessed from the DG phase are systematically explored as a function of molecular asymmetry and incompatibility.}, archive = {J_PRL}, author = {Xiao-Jie Geng and Hao Li and Xiao Yang and Li-Jia An and Marcus Müller and De-Wen Sun}, doi = {10.1103/PhysRevLett.134.118102}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {118102}, shortjournal = {Phys. Rev. Lett.}, title = {Process-directed self-assembly of the frank-kasper a15 structure in linear, conformationally symmetric block copolymers}, volume = {134}, year = {2025}, }
• (2025). Unveiling crystalline order from glassy behavior of charged rods at very low salt concentrations. PRL, 134(11), 118101. (www)

  @article{ , abstract = {Charged colloids can form ordered structures like Wigner crystals or glasses at very low concentrations due to long-range electrostatic repulsions. Here, we combine small-angle x-ray scattering (SAXS) and optical experiments with simulations to investigate the phase behavior of charged rodlike colloids across a wide range of salt concentrations and packing fractions. At ultralow ionic strength and packing fractions, we reveal both experimentally and numerically a direct transition from a nematic to a crystalline smectic-B phase, previously identified as a glass state. This transition, bypassing the smectic-A intermediate phase, results from minimizing Coulomb repulsion and maximizing entropic gains due to fluctuations in the crystalline structure. This demonstrates how long-range electrostatic repulsion significantly alters the phase behavior of rod-shaped particles and highlights its key role in driving the self-organization of anisotropic particles.}, archive = {J_PRL}, author = {Hanna Anop and Laura Dal Compare and Frédéric Nallet and Achille Giacometti and Eric Grelet}, doi = {10.1103/PhysRevLett.134.118101}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {118101}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling crystalline order from glassy behavior of charged rods at very low salt concentrations}, volume = {134}, year = {2025}, }
• (2025). Nonreciprocal ising model. PRL, 134(11), 117103. (www)

  @article{ , abstract = {Systems with nonreciprocal interactions generically display time-dependent states. These are routinely observed in finite systems, from neuroscience to active matter, in which globally ordered oscillations exist. However, the stability of these uniform nonreciprocal phases in noisy spatially-extended systems, their fate in the thermodynamic limit, and the critical behavior of the corresponding phase transitions are not fully understood. Here, we address these questions by introducing a nonreciprocal generalization of the Ising model and study its phase transitions by means of numerical and analytical approaches. While the mean-field equations predict three stable homogeneous phases (disordered, ordered, and a time-dependent swap phase), our large scale numerical simulations reveal a more complex picture. Static order is destroyed in any finite dimension due to the growth of rare droplets unless the symmetry between the two spin types is broken, triggering a stabilizing droplet-capture mechanism. The swap phase is destroyed by fluctuations in two dimensions through the proliferation of spiral defects but stabilized in three dimensions, where nonreciprocity changes the critical exponents from Ising to XY, thus giving rise to a robust spatially-distributed clock.}, archive = {J_PRL}, author = {Yael Avni and Michel Fruchart and David Martin and Daniel Seara and Vincenzo Vitelli}, doi = {10.1103/PhysRevLett.134.117103}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {117103}, shortjournal = {Phys. Rev. Lett.}, title = {Nonreciprocal ising model}, volume = {134}, year = {2025}, }
• (2025). Locality approach to the bootstrap percolation paradox. PRL, 134(11), 117102. (www)

  @article{ , abstract = {We revisit the bootstrap percolation model, leveraging recent mathematical advances linking it with its local counterpart. This new perspective resolves, for the first time, historic discrepancies between Monte Carlo simulations and theoretical results: previously, those predictions disagreed even in the first-order asymptotics of the model. In contrast, our framework achieves excellent agreement between numerics and theory, which now match up to the third-order expansion, as the infection probability approaches zero. Our algorithm allows us to generate novel predictions for the model.}, archive = {J_PRL}, author = {Ivailo Hartarsky and Augusto Teixeira}, doi = {10.1103/PhysRevLett.134.117102}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {117102}, shortjournal = {Phys. Rev. Lett.}, title = {Locality approach to the bootstrap percolation paradox}, volume = {134}, year = {2025}, }
• (2025). Backbone exponent and annulus crossing probability for planar percolation. PRL, 134(11), 117101. (www)

  @article{ , abstract = {We report the recent derivation of the backbone exponent for 2D percolation. In contrast to previously known exactly solved percolation exponents, the backbone exponent is a transcendental number, which is a root of an elementary equation. We also report an exact formula for the probability that there are two disjoint paths of the same color crossing an annulus. The backbone exponent captures the leading asymptotic, while the other roots of the elementary equation capture the asymptotic of the remaining terms. This suggests that the backbone exponent is part of a conformal field theory (CFT) whose bulk spectrum contains this set of roots. Our approach is based on the coupling between Schramm-Loewner evolution curves and Liouville quantum gravity (LQG), and the integrability of Liouville CFT that governs the LQG surfaces.}, archive = {J_PRL}, author = {Pierre Nolin and Wei Qian and Xin Sun and Zijie Zhuang}, doi = {10.1103/PhysRevLett.134.117101}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {117101}, shortjournal = {Phys. Rev. Lett.}, title = {Backbone exponent and annulus crossing probability for planar percolation}, volume = {134}, year = {2025}, }
• (2025). Emergent ferromagnetic ladder excitations in heavy fermion superconductor CeSb2. PRL, 134(11), 116704. (www)

  @article{ , abstract = {Low-dimensional spin fluctuations play a crucial role in unconventional superconductors, with quasi-one-dimensional spin excitations potentially linked with spin-triplet superconductivity. The heavy fermion superconductor CeSb 2 exhibits an unusual large inverted S -shaped upper critical field that suggests a possible triplet pairing state within its pressure-induced superconducting dome. Using inelastic neutron scattering, we discover quasi-one-dimensional magnetic excitations in CeSb 2 emerging from nearly square Ce layers with minor orthorhombic deformation. We show that the data are well described by a ferromagnetic spin ladder model, where the “rungs” of the ladder straddle Ce bilayers. Moreover, we find that diffuse excitations akin to those in the ordered phase persist well above T N , suggesting that quasi-one-dimensional ferromagnetic paramagnons may significantly contribute to the unusual superconductivity that appears under pressure once magnetic order is suppressed.}, archive = {J_PRL}, author = {Zhaoyang Shan and Yangjie Jiao and Jiayu Guo and Yifan Wang and Jinyu Wu and Jiawen Zhang and Yanan Zhang and Dajun Su and Devashibhai T. Adroja and Christian Balz and Matthias Gutmann and Yu Liu and Huiqiu Yuan and Zhentao Wang and Yu Song and Michael Smidman}, doi = {10.1103/PhysRevLett.134.116704}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116704}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent ferromagnetic ladder excitations in heavy fermion superconductor CeSb2}, volume = {134}, year = {2025}, }
• (2025). Two-dimensional fully compensated ferrimagnetism. PRL, 134(11), 116703. (www)

  @article{ , abstract = {Antiferromagnetic spintronics has long been a subject of intense research interest, and the recent introduction of altermagnetism has further ignited enthusiasm in the field. However, fully compensated ferrimagnetism, which exhibits band spin splitting but zero net magnetization, has yet to receive enough attention. Since the experimental preparation of two-dimensional (2D) magnetic van der Waals (vdW) materials in 2017, 2D magnetic materials, thanks to their super tunability, have quickly become an important playground for spintronics. Here, we extend the concept of fully compensated ferrimagnetism (fFIM) to two dimensions and propose 2D filling-enforced fFIM, demonstrate its stability and ease of manipulation, and present three feasible realization schemes with respective exemplary candidate materials. A simple model for 2D fully compensated ferrimagnets (fFIMs) is developed. Further investigation of 2D fFIMs’ physical properties reveals that they not only exhibit significant magneto-optical response but also show fully spin-polarized currents and the anomalous Hall effect in the half-metallic states, displaying characteristics previously almost exclusive to ferromagnetic materials, greatly broadening the research and application prospects of spintronic materials.}, archive = {J_PRL}, author = {Yichen Liu and San-Dong Guo and Yongpan Li and Cheng-Cheng Liu}, doi = {10.1103/PhysRevLett.134.116703}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116703}, shortjournal = {Phys. Rev. Lett.}, title = {Two-dimensional fully compensated ferrimagnetism}, volume = {134}, year = {2025}, }
• (2025). Exotic temperature dependence of uniaxial magnetocrystalline anisotropy in a two-dimensional ferromagnet. PRL, 134(11), 116702. (www)

  @article{ , abstract = {Uniaxial magnetocrystalline anisotropy (UMA) is the foundation for data storage technology as well as for realizing topological and quantum phases. Combined with the confined electrons and distinct lattice dynamics of two-dimensional (2D) materials, exploring UMA, especially its temperature dependence in 2D ferromagnets, is significant. Here, we report an unprecedented exotic behavior of temperature dependence of UMA in the 2D van der Waals ferromagnet . Below 20 K, the temperature-dependent UMA constant exhibits a canonical Akulov-Zener-Callen-Callen-type with rapidly decreasing trend. Strikingly, above 20 K, it transitions to an anomalous Carr-type one with rapidly increasing trend. Temperature-dependent x-ray diffraction measurements combined with first-principles calculations reveal that the enhanced ferromagnetic exchange coupling caused by the lattice variation preserves the two-ion anisotropy at high temperature. Therein, both the itinerant nature and lattice thermal expansion are altered, thus triggering such exotic . Our findings not only deepen the basic understanding of the temperature dependence of UMA but also favor optimizing the ultra-high-density heat-assisted magnetic recording technology by considering the cooperation between lattice and ferromagnetic exchange coupling.}, archive = {J_PRL}, author = {Jiawei Liu and Jiawei Jiang and Liming Wang and Liang Zhou and Rui Liang and Shuilin Li and Ziying Li and Kai Chang and Hongxin Yang and Nujiang Tang}, doi = {10.1103/PhysRevLett.134.116702}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116702}, shortjournal = {Phys. Rev. Lett.}, title = {Exotic temperature dependence of uniaxial magnetocrystalline anisotropy in a two-dimensional ferromagnet}, volume = {134}, year = {2025}, }
• (2025). Curvature-induced magnetization of altermagnetic films. PRL, 134(11), 116701. (www)

  @article{ , abstract = {The altermagnetic nature of a large class of magnetically ordered materials is the source of a wide range of new effects. Here, we show that the merging of two areas, namely the altermagnetism and the physics of curvilinear low-dimensional magnets gives rise to a distinct novel physical effect: a curvature-induced magnetization in bend altermagnetic films. This effect opens a promising possibility for imaging of the domain structure in the magnetically compensated structures. We consider a thin film of a -wave altermagnet bent in a stretching-free manner and demonstrate that gradients of the film curvature induce a local magnetization that is approximately tangential to the film. The magnetization amplitude directly reflects the altermagnetic symmetry and depends on the direction of bending. It is maximal for the bending along directions of the maximal altermagnetic splitting of the magnon bands. A periodically bent film of sinusoidal shape possesses a total magnetic moment per period , where and are the bending amplitude and wave vector, respectively. The total magnetic moment is perpendicular to the plane of the unbent film and its direction (up or down) is determined by the bending direction. A film roll-up to a nanotube possesses a toroidal moment directed along the tube per one coil, where and are the coil radius and the pitch between coils. All these analytical predictions agree with numerical spin-lattice simulations.}, archive = {J_PRL}, author = {Kostiantyn V. Yershov and Olena Gomonay and Jairo Sinova and Jeroen van den Brink and Volodymyr P. Kravchuk}, doi = {10.1103/PhysRevLett.134.116701}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116701}, shortjournal = {Phys. Rev. Lett.}, title = {Curvature-induced magnetization of altermagnetic films}, volume = {134}, year = {2025}, }
• (2025). Symmetry-related large-area corner mode with a tunable mode area and stable frequency. PRL, 134(11), 116607. (www)

  @article{ , abstract = {Emergent collective modes in lattices give birth to many intriguing physical phenomena in condensed matter physics. Among these collective modes, large-area modes typically feature small-level spacings, while a mode with stable frequency tends to be spatially tightly confined. In this Letter, we theoretically propose and experimentally demonstrate a symmetry-related large-area topological corner mode with a tunable mode area and stable frequency. This mode emerges from the hybridization of the homogeneous Dirac point mode and in-gap topological corner modes. Remarkably, this hybridized mode possesses unique chirality related to the chiral symmetry. We experimentally observe such hybridized mode in a two-dimensional (2D) photonic system and demonstrate its robustness by introducing disorders in the structure. Our findings advance the frontier of higher-order topology research, transitioning it from single-lattice systems to hybridized multilattice systems. These results may support promising potential applications, particularly in vertical-cavity surface-emitting lasers.}, archive = {J_PRL}, author = {Zhongfu Li and Shiqi Li and Bei Yan and Hsun-Chi Chan and Jing Li and Jun Guan and Wengang Bi and Yuanjiang Xiang and Zhen Gao and Shuang Zhang and Peng Zhan and Zhenlin Wang and Biye Xie}, doi = {10.1103/PhysRevLett.134.116607}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116607}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry-related large-area corner mode with a tunable mode area and stable frequency}, volume = {134}, year = {2025}, }
• (2025). Acoustic exceptional line semimetal. PRL, 134(11), 116606. (www)

  @article{ , abstract = {Non-Hermitian topological phases, which exhibit unique features such as skin effect and exceptional points originated from nontrivial band topologies in complex plane, have attracted enormous attention in condensed-matter physics and metamaterials. Here, we report the realization of an exceptional line semimetal in a three-dimensional non-Hermitian phononic crystal. A pair of exceptional rings with opposite topologies are connected by the drumhead bulk states in the first Brillouin zone. The exceptional rings not only possess wave-function topology and thus result in the drumhead surface states, but also host spectral topology and thereby give rise to the geometry-dependent skin effect in three dimensions. Our experimental results evidence the complete non-Hermitian bulk-boundary correspondence of the three-dimensional exceptional line semimetal and may pave the way for designing non-Hermitian acoustic devices.}, archive = {J_PRL}, author = {Yejian Hu and Jien Wu and Peidong Ye and Weiyin Deng and Jiuyang Lu and Xueqin Huang and Ziyu Wang and Manzhu Ke and Zhengyou Liu}, doi = {10.1103/PhysRevLett.134.116606}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116606}, shortjournal = {Phys. Rev. Lett.}, title = {Acoustic exceptional line semimetal}, volume = {134}, year = {2025}, }
• (2025). Topological zero modes and correlation pumping in an engineered kondo lattice. PRL, 134(11), 116605. (www)

  @article{ , abstract = {Topological phases of matter provide a flexible platform to engineer unconventional quantum excitations in quantum materials. Beyond single particle topological matter, in systems with strong quantum many-body correlations, many-body effects can be the driving force for non-trivial topology. Here, we propose a one-dimensional engineered Kondo lattice where the emergence of topological excitations is driven by collective many-body Kondo physics. We first show the existence of topological zero modes in this system by solving the interacting model with tensor networks, and demonstrate their robustness against disorder. To unveil the origin of the topological zero modes, we analyze the associated periodic Anderson model showing that it can be mapped to a topological non-Hermitian model, enabling rationalizing the origin of the topological zero modes. We finally show that the topological invariant of the many-body Kondo lattice can be computed with a correlation matrix pumping method directly with the exact quantum many-body wave function. Our results provide a strategy to engineer topological Kondo insulators, highlighting quantum magnetism as a driving force in engineering topological matter.}, archive = {J_PRL}, author = {Zina Lippo and Elizabeth Louis Pereira and Jose L. Lado and Guangze Chen}, doi = {10.1103/PhysRevLett.134.116605}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116605}, shortjournal = {Phys. Rev. Lett.}, title = {Topological zero modes and correlation pumping in an engineered kondo lattice}, volume = {134}, year = {2025}, }
• (2025). Observation of oriented landau levels and helical zero modes in berry dipole acoustic crystals. PRL, 134(11), 116604. (www)

  @article{ , abstract = {Landau levels play a fundamental role in condensed matter physics, as they offer critical insights into charged particles’ behavior in magnetic fields. These unique characteristics have significant implications for understanding various quantum phenomena and materials’ electronic properties, such as the renowned quantum Hall effect. Over the past two decades, substantial advancements have been achieved in Landau levels in systems with linear band crossing points, like Weyl points, which exhibit fascinating features like chiral zero modes. The Landau levels observed thus far are independent of the magnetic field’s orientation. In this Letter, we experimentally demonstrate unconventional oriented Landau levels in acoustic Berry dipole systems, wherein by reversing the orientation of the pseudomagnetic field, the system exhibits distinct Landau spectra. Remarkably, we observe a new type of helical zero mode, whose existence critically depends on the magnetic field’s orientation. This is in sharp contrast to the well-studied chiral zero modes in Weyl systems, whose propagation direction, but not existence, depends on the applied magnetic field’s orientation. Our Letter opens up avenues for understanding the interaction of gauge fields with band singularities that go beyond Chern class, including Berry multipoles and even-dimensional monopoles, and offers new insights for exploring topological devices.}, archive = {J_PRL}, author = {Qingyang Mo and Riyi Zheng and Cuicui Lu and Xueqin Huang and Zhengyou Liu and Shuang Zhang}, doi = {10.1103/PhysRevLett.134.116604}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116604}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of oriented landau levels and helical zero modes in berry dipole acoustic crystals}, volume = {134}, year = {2025}, }
• (2025). Chern number tunable quantum anomalous hall effect in compensated antiferromagnets. PRL, 134(11), 116603. (www)

  @article{ , abstract = {We propose to realize the quantum anomalous Hall effect (QAHE) in two-dimensional compensated antiferromagnets without net spin magnetization. We consider antiferromagnetic as a concrete example. By breaking the parity-time ( ) symmetry of even-layer , we find that the system can host the QAHE with a nonzero Chern number. We show that by controlling the antiferromagnetic spin configuration—for example, down/up/up/down that breaks symmetry—tetralayer can host a Chern number . Such spin configuration can be stabilized by pinning the spin orientations of the surfaces. Furthermore, via tuning the on-site orbital energy and vertical electric fields, we find rich QAHE phases with tunable Chern number of . In addition, we reveal that the edge states are layer selective and primarily located at the boundaries of the bottom and top layers. Our Letter not only proposes a scheme to realize Chern number tunable QAHE in antiferromagnets without net spin magnetization but also provides a platform for layer-selective dissipationless transport devices.}, archive = {J_PRL}, author = {Wenhao Liang and Zeyu Li and Jiaqi An and Yafei Ren and Zhenhua Qiao and Qian Niu}, doi = {10.1103/PhysRevLett.134.116603}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116603}, shortjournal = {Phys. Rev. Lett.}, title = {Chern number tunable quantum anomalous hall effect in compensated antiferromagnets}, volume = {134}, year = {2025}, }
• (2025). Topological quantum criticality from multiplicative topological phases. PRL, 134(11), 116602. (www)

  @article{ , abstract = {Symmetry-protected topological phases (SPTs) characterized by short-range entanglement include many states essential to the understanding of topological condensed matter physics, and the extension to gapless SPTs provides essential understanding of their consequences. In this work, we identify a fundamental connection between gapless SPTs and recently introduced multiplicative topological phases, demonstrating that multiplicative topological phases are an intuitive and general approach to realizing concrete models for gapless SPTs. In particular, they are naturally well suited to realizing higher-dimensional, stable, and intrinsically gapless SPTs through the combination of canonical topological insulator and semimetal models with critical gapless models in symmetry-protected tensor product constructions, opening avenues to far broader and deeper investigation of topology via short-range entanglement.}, archive = {J_PRL}, author = {R. Flores-Calderón and Elio J. König and Ashley M. Cook}, doi = {10.1103/PhysRevLett.134.116602}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116602}, shortjournal = {Phys. Rev. Lett.}, title = {Topological quantum criticality from multiplicative topological phases}, volume = {134}, year = {2025}, }
• (2025). Ideal flat and resolved SU(3) landau levels in three dimensions. PRL, 134(11), 116601. (www)

  @article{ , abstract = {Landau levels (LLs) are of great importance for understanding the quantum Hall effect and associated many-body physics. Recently, their three-dimensional (3D) counterparts, i.e., dispersionless 3D LLs with well-defined quantum numbers, have attracted significant attention but have not yet been reported. Here we theoretically propose and experimentally observe 3D LLs with a sharply quantized spectrum in a diamond acoustic lattice, where the eigenstates are characterized by SU(3) quantum numbers. The engineered inhomogeneous hopping strengths not only introduce pseudomagnetic fields that quantize the nodal lines into LLs but also provide three bosonic degrees of freedom, embedding a generic SU(3) symmetry into the LLs. Using a phased array of acoustic sources, we selectively excite distinct eigenstates within the degenerate LL multiplets and visualize their 3D eigenmodes. Importantly, our approach enables the precise reconstruction of SU(3) quantum numbers directly from eigenmode correlations. Our results establish SU(3) LLs as a tractable model in artificial platforms, and pave the way for synthesizing LLs with zero dispersion and countable quantum numbers in arbitrary dimensions.}, archive = {J_PRL}, author = {Mian Peng and Qiang Wei and Jiale Yuan and Da-Wei Wang and Mou Yan and Han Cai and Gang Chen}, doi = {10.1103/PhysRevLett.134.116601}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116601}, shortjournal = {Phys. Rev. Lett.}, title = {Ideal flat and resolved SU(3) landau levels in three dimensions}, volume = {134}, year = {2025}, }
• (2025). Spin waves in dirac semimetal Ca0.6Sr0.4MnSb2 investigated with neutrons by the diffraction method. PRL, 134(11), 116504. (www)

  @article{ , abstract = {The tunability of Dirac semimetals with antiferromagnetic Mn layers is of great interest. The observed sign change of interlayer magnetic coupling between CaMnBi 2 and SrMnBi 2 suggests ionic substitution as a potential tuning mechanism. If so, novel behavior near the compensation point could be expected. To explore this, we study a mixed-cation analog, Ca 0.6 Sr 0.4 MnSb 2 , where Bi is replaced by Sb. Conventional inelastic neutron scattering is impractical due to the small crystal size ( m ≈ 0.28 g ) available for compositional studies; however, we find that using a neutron diffractometer with a wide-angle area detector we can obtain a good quality spin-wave signal, which is shaped by energy-momentum conservation and retains spectroscopic information even without direct energy analysis. Spin-wave modeling reveals an interlayer coupling quantitatively similar to SrMnSb 2 , indicating it is not directly tuned by ionic size and that the sign change in Bi-based compounds likely arises from the observed change in lattice symmetry. Beyond this key insight, our results present an efficient method for parametric and compositional studies of spin dynamics in small crystals.}, archive = {J_PRL}, author = {Xiao Hu and Yan Wu and Matthias D. Frontzek and Zhixiang Hu and Cedomir Petrovic and John M. Tranquada and Igor A. Zaliznyak}, doi = {10.1103/PhysRevLett.134.116504}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116504}, shortjournal = {Phys. Rev. Lett.}, title = {Spin waves in dirac semimetal Ca0.6Sr0.4MnSb2 investigated with neutrons by the diffraction method}, volume = {134}, year = {2025}, }
• (2025). Quantum thermalization via travelling waves. PRL, 134(11), 116503. (www)

  @article{ , abstract = {Isolated quantum many-body systems which thermalize under their own dynamics are expected to act as their own thermal baths, thereby losing memory of initial conditions and bringing their local subsystems to thermal equilibrium. Here we show that the infinite-dimensional limit of a quantum lattice model, as described by dynamical mean-field theory (DMFT), provides a natural framework to understand this self-consistent thermalization process. Using the Fermi-Hubbard model as a working example, we demonstrate that the emergence of a self-consistent bath occurs via a sharp thermalization front, moving ballistically and separating the initial condition from the long time thermal fixed point. We characterize the full DMFT dynamics through an effective temperature for which we derive a traveling wave equation of the Fisher-Kolmogorov-Petrovsky-Piskunov type. This equation allows for predicting the asymptotic shape of the front and its velocity, which match perfectly the full DMFT numerics. Our results provide a new angle to understand the onset of quantum thermalization in closed isolated systems.}, archive = {J_PRL}, author = {Antonio Picano and Giulio Biroli and Marco Schirò}, doi = {10.1103/PhysRevLett.134.116503}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116503}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum thermalization via travelling waves}, volume = {134}, year = {2025}, }
• (2025). Frustration-induced superconductivity in the t−t′ hubbard model. PRL, 134(11), 116502. (www)

  @article{ , abstract = {The two-dimensional Hubbard model is widely believed to capture key ingredients of high- T c superconductivity in cuprate materials. However, compelling evidence remains elusive. In particular, various magnetic orders may emerge as strong competitors of superconducting orders. Here, we study the ground state properties of the doped two-dimensional t − t ′ Hubbard model on a square lattice via the infinite projected entangled-pair state method with U(1) or SU(2) spin symmetry. The former is compatible with antiferromagnetic orders, while the latter forbids them. Therefore, we obtain by comparison a detailed understanding of the magnetic impact on superconductivity. Moreover, an additional t ′ term accommodates the particle-hole asymmetry, which facilitates studies on the discrepancies between electron- and hole-doped systems. We demonstrate that (i) a positive t ′ / t significantly amplifies the strength of superconducting orders; (ii) at sufficiently large doping levels, the t − t ′ Hubbard model favors a uniform state with superconducting orders instead of stripe states with charge and spin modulations; and (iii) the enhancement of magnetic frustration, by increasing either the strength of next-nearest neighbor interactions or the charge doping, impairs stripe orders and helps stabilize superconductivity.}, archive = {J_PRL}, author = {Changkai Zhang (张昌凯 and Jheng-Wei Li and Dimitra Nikolaidou and Jan von Delft}, doi = {10.1103/PhysRevLett.134.116502}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116502}, shortjournal = {Phys. Rev. Lett.}, title = {Frustration-induced superconductivity in the t−t′ hubbard model}, volume = {134}, year = {2025}, }
• (2025). Intraband collective excitations and spatial correlations in fractional chern insulators. PRL, 134(11), 116501. (www)

  @article{ , abstract = {The low-energy collective excitations of semiconductors and insulators often couple strongly to light, allowing them to be probed optically. We argue here that in fractional Chern insulators intraband collective excitations are dark in the sense that they couple anomalously weakly to light. Using this property, we establish a general relationship between flat-band Chern numbers, quantum geometry, and spatial correlations in fractional-Chern-insulator states.}, archive = {J_PRL}, author = {Tobias Wolf and Yung-Chun Chao and Allan H. MacDonald and Jung-Jung Su}, doi = {10.1103/PhysRevLett.134.116501}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116501}, shortjournal = {Phys. Rev. Lett.}, title = {Intraband collective excitations and spatial correlations in fractional chern insulators}, volume = {134}, year = {2025}, }
• (2025). Intrinsic gyrotropic magnetic current from zeeman quantum geometry. PRL, 134(11), 116301. (www)

  @article{ , abstract = {Quantum geometric tensor (QGT), which is usually obtained by evaluating the quantum distance between Bloch states parametrized by momentum, plays a key role in exploring the exotic responses of quantum materials. Herein, we revisit the concept of QGT by further taking into account the spin degree of freedom. Besides the conventional QGT relating to momentum translation, we uncover a new QGT (termed Zeeman QGT) relating to momentum translation as well as spin rotation, whose imaginary (real) part gives the Zeeman Berry curvature (quantum metric). Notably, we show that these novel quantum geometric quantities can drive an intrinsic gyrotropic magnetic current (IGMC) in spin-orbit coupled materials when the electron spin is steered by an oscillating magnetic field. With symmetry analysis, we show that a wide range of materials can support the IGMC, as illustrated by model calculations. Finally, we discuss the experimental aspects of detecting the IGMC driven by Zeeman QGT.}, archive = {J_PRL}, author = {Longjun Xiang and Jinxiong Jia and Fuming Xu and Zhenhua Qiao and Jian Wang}, doi = {10.1103/PhysRevLett.134.116301}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116301}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic gyrotropic magnetic current from zeeman quantum geometry}, volume = {134}, year = {2025}, }
• (2025). Atomic manipulation on a highly corrugated topological insulator. PRL, 134(11), 116201. (www)

  @article{ , abstract = {We report a mechanism of lateral manipulation of single Fe adatoms on the surface of the topological insulator Bi 2 Se 3 with atomic force microscopy. The Fe atoms are embedded within the sparsely packed surface layer, rendering them inaccessible to classical manipulation methods. Nevertheless, we find a manipulation mechanism in which the Fe atom is plucked from its adsorption site and can be pulled along the surface. We demonstrate the controllability of this pluck-pull manipulation by the construction of a small nanostructure.}, archive = {J_PRL}, author = {Emma Grasser and Adrian Weindl and Alfred J. Weymouth and Franz J. Giessibl}, doi = {10.1103/PhysRevLett.134.116201}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116201}, shortjournal = {Phys. Rev. Lett.}, title = {Atomic manipulation on a highly corrugated topological insulator}, volume = {134}, year = {2025}, }
• (2025). Two characteristic contributions to the superconducting state of 2H−NbSe2. PRL, 134(11), 116001. (www)

  @article{ , abstract = {Multiband superconductivity arises when multiple electronic bands contribute to the formation of the superconducting state, allowing distinct pairing interactions and gap structures. Here, we present field- and temperature-dependent data on the vortex lattice structure in as a contribution to the ongoing debate as to whether the defining feature of the superconductivity is the anisotropy or the multiband nature. The field-dependent data clearly show that there are two distinct superconducting bands, and the contribution of one of them to the vortex lattice signal is completely suppressed for magnetic fields above , well below . By combining the temperature and field scans, we can deduce that there is a moderate degree of interband coupling. From the observed temperature dependences, we find that at low field and zero temperature, the two gaps in temperature units are and ( and 0.94 ); the band with the larger gap gives just under two-thirds of the superfluid density. The penetration depth extrapolated to zero field and zero temperature is .}, archive = {J_PRL}, author = {A. Alshemi and E. M. Forgan and A. Hiess and R. Cubitt and J. S. White and K. Schmalzl and E. Blackburn}, doi = {10.1103/PhysRevLett.134.116001}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {116001}, shortjournal = {Phys. Rev. Lett.}, title = {Two characteristic contributions to the superconducting state of 2H−NbSe2}, volume = {134}, year = {2025}, }
• (2025). Detection of large guide field electron-only reconnection in a filamentary current sheet immersed in a large-scale magnetopause reconnection exhaust. PRL, 134(11), 115201. (www)

  @article{ , abstract = {We present the Magnetospheric Multiscale (MMS) mission’s observations of large-scale reconnection with a laminar ion exhaust containing many electron-scale filamentary current sheets, one of which exhibited a super-ion-Alfvénic electron jet flowing opposite to the ion exhaust jet, identified as electron-only reconnection. Despite the close proximity (a few electron inertial lengths) of the four MMS spacecraft, they recorded different electron-only reconnection signatures, including differences in the magnitude and profile of the electron jet, parallel electric fields, and dissipation , indicating extremely short-scale spatial and temporal variability. Furthermore, the leading spacecraft did not detect reconnection signatures, suggesting that MMS may have witnessed the onset of electron-only reconnection. Hall magnetic field perturbations associated with an electron-scale current sheet were detected after the onset. The dissipation in the electron-only current sheet was dominated by the component perpendicular to the magnetic field, contrasting with the dominance of the parallel component in previous large guide field reconnection events.}, archive = {J_PRL}, author = {P. S. Pyakurel and T. D. Phan and M. Øieroset and J. F. Drake and M. A. Shay and A. Mallet and J. Stawarz and S. Wang and M. Oka and K. J. Genestreti and N. Ahmadi and J. L. Burch and R. B. Torbert and R. E. Ergun and D. J. Gershman and B. L. Giles and R. J. Strangeway}, doi = {10.1103/PhysRevLett.134.115201}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {115201}, shortjournal = {Phys. Rev. Lett.}, title = {Detection of large guide field electron-only reconnection in a filamentary current sheet immersed in a large-scale magnetopause reconnection exhaust}, volume = {134}, year = {2025}, }
• (2025). Spectrotemporal shaping of attosecond X-ray pulses with a fresh-slice free-electron laser. PRL, 134(11), 115001. (www)

  @article{ , abstract = {We propose a scheme allowing coherent shaping, i.e., controlling both the amplitude and phase, of attosecond x-ray pulses at free-electron lasers. We show that by seeding a free-electron laser with a short coherent seed that overfills the amplification bandwidth, one can shape the Wigner function of the pulse by controlling the undulator taper profile. The examples of controllable pulse pairs and trains, as well as isolated spectrotemporally shaped pulses with very broad bandwidths are examined in detail. Existing attosecond x-ray free-electron lasers can achieve these experimental conditions in a two-stage cascade, in which the seed is generated by a short current spike in an electron bunch and shaped in an unspoiled region within the same bunch. We experimentally demonstrate the production and control of phase-stable pulse trains using this method at the Linac Coherent Light Source II.}, archive = {J_PRL}, author = {River R. Robles and Kirk A. Larsen and David Cesar and Taran Driver and Joseph Duris and Paris Franz and Douglas Garratt and Veronica Guo and Gabriel Just and Randy Lemons and Ming-Fu Lin and Razib Obaid and Nicholas Sudar and Jun Wang and Zhen Zhang and James Cryan and Agostino Marinelli}, doi = {10.1103/PhysRevLett.134.115001}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {115001}, shortjournal = {Phys. Rev. Lett.}, title = {Spectrotemporal shaping of attosecond X-ray pulses with a fresh-slice free-electron laser}, volume = {134}, year = {2025}, }
• (2025). Photonic spin hall effect by electro-optically induced pancharatnam-berry phases. PRL, 134(11), 113805. (www)

  @article{ , abstract = {Here, a novel photonic spin Hall effect is demonstrated based on the spatially varying Pancharatnam-Berry (PB) phases, aroused naturally in an -cut crystal via the Pockels effect. Applied with an electric field, the principal axes of crystal will rotate around the -axis with the rotation angle varying linearly with the component of the applied field. By depositing an asymmetric electrode pair on the crystal to induce inhomogeneously distributed electric fields, spatially varying rotations of the principal axes of crystal are generated, resulting in spatially varying PB phases. These spatially varying PB phases are redistributable by the applied voltage, different from those unchangeable PB phases aroused by the spatially varying orientations of anisotropic structure units such as patterned liquid crystals and metasurfaces. The redistributable PB phases can cause tunable separations of spin photons in the momentum space. The separation speed is measured as . These findings deepen the understanding of the geometric phase and pave the way for high-speed control of spin photons.}, archive = {J_PRL}, author = {Xingliang Xie and Hongdao Cheng and Huifeng Chen and Huadan Zheng and Yongchun Zhong and Jieyuan Tang and Jianhui Yu and Zhe Chen and Wenguo Zhu}, doi = {10.1103/PhysRevLett.134.113805}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113805}, shortjournal = {Phys. Rev. Lett.}, title = {Photonic spin hall effect by electro-optically induced pancharatnam-berry phases}, volume = {134}, year = {2025}, }
• (2025). Inverse spin thermal hall effect in nonreciprocal photonic systems. PRL, 134(11), 113804. (www)

  @article{ , abstract = {A transverse radiative heat flux induced by the gradient of spin angular momentum of photons in nonreciprocal systems is predicted. This thermal analog of the inverse spin Hall effect is analyzed in magneto-optical networks exhibiting C 4 symmetry, under the action of spatially variable external magnetic fields. This finding opens new avenues for thermal management and energy conversion with nonreciprocal systems through a localized and dynamic control of the spin angular momentum of light.}, archive = {J_PRL}, author = {P. Ben-Abdallah}, doi = {10.1103/PhysRevLett.134.113804}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113804}, shortjournal = {Phys. Rev. Lett.}, title = {Inverse spin thermal hall effect in nonreciprocal photonic systems}, volume = {134}, year = {2025}, }
• (2025). Observation of light localization at the edges of quasicrystal waveguide arrays. PRL, 134(11), 113803. (www)

  @article{ , abstract = {Quasicrystals are unique systems that, unlike periodic structures, lack translational symmetry but exhibit long-range order dramatically enriching the system properties. While evolution of light in the bulk of photonic quasicrystals is well studied, experimental evidences of light localization near the edge of truncated photonic quasicrystal structures are practically absent. In this Letter, we observe both linear and nonlinear localization of light at the edges of radially cropped quasicrystal waveguide arrays, forming an aperiodic Penrose tiling. Our theoretical analysis reveals that for certain truncation radii, the system exhibits linear eigenstates localized at the edge of the truncated array, whereas for other radii, this localization does not occur, highlighting the significant influence of truncation on edge light localization. Using single-waveguide excitations, we experimentally confirm the presence of localized states in Penrose arrays inscribed by a femtosecond laser and investigate the effects of nonlinearity on these states. Our theoretical findings identify a family of edge solitons, and experimentally, we observe a transition from linear localized states to edge solitons as the power of the input pulse increases. Our results represent the first experimental demonstration of localization phenomena induced by the selective truncation of quasiperiodic photonic systems.}, archive = {J_PRL}, author = {S. K. Ivanov and S. A. Zhuravitskii and N. S. Kostyuchenko and N. N. Skryabin and I. V. Dyakonov and A. A. Kalinkin and S. P. Kulik and V. O. Kompanets and S. V. Chekalin and S. Alyatkin and A. Ferrando and Y. V. Kartashov and V. N. Zadkov}, doi = {10.1103/PhysRevLett.134.113803}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113803}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of light localization at the edges of quasicrystal waveguide arrays}, volume = {134}, year = {2025}, }
• (2025). Chiral resonant modes induced by intrinsic birefringence in lithium niobate metasurfaces. PRL, 134(11), 113802. (www)

  @article{ , abstract = {The intrinsic chirality of natural materials is known to be weak, prompting extensive efforts to enhance chiral light-matter interactions on the metasurface platform. Chiral metasurfaces are typically created by manipulating the geometry of nanostructures, such as three-dimensional helical structures and slanted structures. However, these approaches are generally challenging to implement experimentally in optical frequency ranges. Here, we present the achievement of significant chirality on planar lithium niobate metasurfaces. We theoretically demonstrate that the birefringence of lithium niobate enables a strong coupling between two nearly degenerate resonant modes when rotating the optical axis. Despite the achiral geometric morphology of the lithium niobate structure, we show that these mixed modes exhibit chirality and can produce nearly full circular dichroism signals. Moreover, we experimentally validate our theoretical proposal using our advanced process technique for lithium niobate nanostructures and the measured circular dichroism signal reaches . These findings offer new possibilities for chiral metaphotonics.}, archive = {J_PRL}, author = {Bo Wang and Tingyue Zhu and Yunan Liu and Haifang Yang and Ruhao Pan and Junjie Li}, doi = {10.1103/PhysRevLett.134.113802}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113802}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral resonant modes induced by intrinsic birefringence in lithium niobate metasurfaces}, volume = {134}, year = {2025}, }
• (2025). Temperature sensitivity of a thorium-229 solid-state nuclear clock. PRL, 134(11), 113801. (www)

  @article{ , abstract = {Quantum state-resolved spectroscopy of the low energy thorium-229 nuclear transition was recently achieved. The five allowed transitions within the electric quadrupole structure were measured to the kilohertz level in a calcium fluoride host crystal, opening many new areas of research using nuclear clocks. Central to the performance of solid-state clock operation is an understanding of systematic shifts such as the temperature dependence of the clock transitions. In this work, we measure the four strongest transitions of thorium-229 in the same crystal at three temperature values: 150 K, 229 K, and 293 K. We find shifts of the unsplit frequency and the electric quadrupole splittings, corresponding to decreases in the electron density, electric field gradient, and field gradient asymmetry at the nucleus as temperature increases. The line shifts only 62(6) kHz over the temperature range, i.e., approximately , representing a promising candidate for a future solid-state optical clock. Achieving precision requires crystal temperature stability of .}, archive = {J_PRL}, author = {Jacob S. Higgins and Tian Ooi and Jack F. Doyle and Chuankun Zhang and Jun Ye and Kjeld Beeks and Tomas Sikorsky and Thorsten Schumm}, doi = {10.1103/PhysRevLett.134.113801}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113801}, shortjournal = {Phys. Rev. Lett.}, title = {Temperature sensitivity of a thorium-229 solid-state nuclear clock}, volume = {134}, year = {2025}, }
• (2025). Thermal radiation force and torque on moving nanostructures with anisotropic optical response. PRL, 134(11), 113604. (www)

  @article{ , abstract = {Nanoscale objects moving relative to a thermal radiation bath experience a drag force due to the imbalance in their interaction with the blue- and redshifted components of the electromagnetic field. Here, we show that, in addition to this drag force, moving nanostructures with an anisotropic optical response experience a lateral force and a torque that substantially modify their trajectory. These phenomena emerge from the additional coupling between the electromagnetic field components polarized parallel and perpendicular to the trajectory, enabled by the anisotropic response of the nanostructure. This work unveils the intricate dynamics of anisotropic nanostructures moving in a thermal radiation bath.}, archive = {J_PRL}, author = {Juan R. Deop-Ruano and Alejandro Manjavacas}, doi = {10.1103/PhysRevLett.134.113604}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113604}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal radiation force and torque on moving nanostructures with anisotropic optical response}, volume = {134}, year = {2025}, }
• (2025). Nonchiral non-bloch invariants and topological phase diagram in nonunitary quantum dynamics without chiral symmetry. PRL, 134(11), 113603. (www)

  @article{ , abstract = {The non-Bloch topology leads to the emergence of various counterintuitive phenomena in non-Hermitian systems under the open boundary condition, which can not find a counterpart in Hermitian systems. However, in the non-Hermitian system without chiral symmetry, being ubiquitous in nature, exploring its non-Bloch topology has so far eluded experimental effort. Here, by introducing the concept of nonchiral non-Bloch invariants, we theoretically predict and experimentally identify the non-Bloch topological phase diagram of a one-dimensional (1D) non-Hermitian system without chiral symmetry in discrete-time nonunitary quantum walks of single photons. Interestingly, we find that such topological invariants not only can distinguish topologically distinct gapped phases, but they also faithfully capture the corresponding gap closing in open-boundary spectrum at the phase boundary. Different topological regions are experimentally identified by measuring the featured discontinuities of the higher moments of the walker’s displacement, which amazingly match excellently with our defined non-Bloch invariants. Our work provides a useful platform to study the interplay among topology, symmetries, and the non-Hermiticity.}, archive = {J_PRL}, author = {Yue Zhang and Shuai Li and Yingchao Xu and Rui Tian and Miao Zhang and Hongrong Li and Hong Gao and M. Suhail Zubairy and Fuli Li and Bo Liu}, doi = {10.1103/PhysRevLett.134.113603}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113603}, shortjournal = {Phys. Rev. Lett.}, title = {Nonchiral non-bloch invariants and topological phase diagram in nonunitary quantum dynamics without chiral symmetry}, volume = {134}, year = {2025}, }
• (2025). Engineering dipole-dipole couplings for enhanced cooperative light-matter interactions. PRL, 134(11), 113602. (www)

  @article{ , abstract = {Cooperative optical effects are enabled and controlled by interactions between molecular dipoles, meaning that their mutual orientation is of paramount importance to, for example, superabsorbing light-harvesting antennas. Here we show how to move beyond the possibilities of simple geometric tailoring, demonstrating how a metallic sphere placed within a ring of parallel dipoles engineers an effective Hamiltonian that generates “guide-sliding” states within the ring system. This allows steady-state superabsorption in noisy room temperature environments, outperforming previous designs while being significantly simpler to implement. As exemplified by this showcase, our approach represents a powerful design paradigm for tailoring cooperative light-matter effects in molecular structures that extends beyond superabsorbing systems to a huge array of quantum energy transport systems.}, archive = {J_PRL}, author = {Adam Burgess and Madeline C. Waller and Erik M. Gauger and Robert Bennett}, doi = {10.1103/PhysRevLett.134.113602}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113602}, shortjournal = {Phys. Rev. Lett.}, title = {Engineering dipole-dipole couplings for enhanced cooperative light-matter interactions}, volume = {134}, year = {2025}, }
• (2025). Cross-polarized stimulated brillouin scattering in lithium niobate waveguides. PRL, 134(11), 113601. (www)

  @article{ , abstract = {We report on the experimental demonstration of cross-polarization backward stimulated Brillouin scattering (BSBS) in lithium niobate on insulator (LNOI) waveguides. Performing polarization-sensitive pump and probe measurements, we captured both intra- and intermodal scattering between counterpropagating fundamental optical modes. Remarkably, cross-polarization scattering achieved SBS gains that exceeded . This substantial gain not only broadens the utility of polarization in SBS but also paves the way for high-performance devices, including ultranarrowband lasers, robust broadband nonreciprocal devices, RF filters, and microwave-to-optical converters.}, archive = {J_PRL}, author = {Caique C. Rodrigues and Nick J. Schilder and Roberto O. Zurita and Letícia S. Magalhães and Amirhassan Shams-Ansari and Felipe J. L. dos Santos and Otávio M. Paiano and Thiago P. M. Alegre and Marko Lončar and Gustavo S. Wiederhecker}, doi = {10.1103/PhysRevLett.134.113601}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113601}, shortjournal = {Phys. Rev. Lett.}, title = {Cross-polarized stimulated brillouin scattering in lithium niobate waveguides}, volume = {134}, year = {2025}, }
• (2025). Self-trapping phenomenon, multistability and chaos in open anisotropic dicke dimer. PRL, 134(11), 113404. (www)

  @article{ , abstract = {We investigate semiclassical dynamics of a coupled atom-photon interacting system described by a dimer of anisotropic Dicke model in the presence of photon loss, exhibiting a rich variety of nonlinear dynamics. Based on symmetries and dynamical classification, we characterize and chart out various dynamical phases in a phase diagram. A key feature of this system is the multistability of different dynamical states, particularly the coexistence of various superradiant phases as well as limit cycles. Remarkably, this dimer system manifests self-trapping phenomena, resulting in a photon population imbalance between the cavities. Such a self-trapped state arises from a saddle-node bifurcation, which can be understood from an equivalent Landau-Ginzburg description. Additionally, we identify a unique class of oscillatory dynamics, “ self-trapped limit cycle, ” hosting self-trapping of photons. The absence of stable dynamical phases leads to the onset of chaos, which is diagnosed using the saturation value of the decorrelator dynamics. Moreover, the self-trapped states can coexist with chaotic attractor, which may have intriguing consequences in quantum dynamics. Finally, we discuss the experimental relevance of our findings, which can be tested in cavity and circuit quantum electrodynamics setups.}, archive = {J_PRL}, author = {G. Vivek and Debabrata Mondal and Subhadeep Chakraborty and S. Sinha}, doi = {10.1103/PhysRevLett.134.113404}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113404}, shortjournal = {Phys. Rev. Lett.}, title = {Self-trapping phenomenon, multistability and chaos in open anisotropic dicke dimer}, volume = {134}, year = {2025}, }
• (2025). Many-body gap protection against motional dephasing of an optical clock transition. PRL, 134(11), 113403. (www)

  @article{ , abstract = {Quantum simulation and metrology with atoms, ions, and molecules often rely on using light fields to manipulate their internal states. The absorbed momentum from the light fields can induce spin-orbit coupling and associated motional-induced (Doppler) dephasing, which may limit the coherence time available for metrology and simulation. We experimentally demonstrate the suppression of Doppler dephasing on a strontium optical clock transition by enabling atomic interactions through a shared mode in a high-finesse optical ring cavity. The interactions create a many-body energy gap that increases with atom number, suppressing motional dephasing when it surpasses the dephasing energy scale. This collective approach offers an alternative to traditional methods, like Lamb-Dicke confinement or Mössbauer spectroscopy, for advancing optical quantum sensors and simulations.}, archive = {J_PRL}, author = {Zhijing Niu and Vera M. Schäfer and Haoqing Zhang and Cameron Wagner and Nathan R. Taylor and Dylan J. Young and Eric Yilun Song and Anjun Chu and Ana Maria Rey and James K. Thompson}, doi = {10.1103/PhysRevLett.134.113403}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113403}, shortjournal = {Phys. Rev. Lett.}, title = {Many-body gap protection against motional dephasing of an optical clock transition}, volume = {134}, year = {2025}, }
• (2025). Coherence of symmetry-protected rotational qubits in cold polyatomic molecules. PRL, 134(11), 113402. (www)

  @article{ , abstract = {Polar polyatomic molecules provide an ideal but largely unexplored platform to encode qubits in rotational states. Here, we trap cold (100–600 mK) formaldehyde ( ) inside an electric box and perform a Ramsey-type experiment to observe long-lived ( ) coherences between symmetry-protected molecular states with opposite rotation but identical orientation, representing a quasi-hidden molecular degree of freedom. As a result, the observed qubit is insensitive to the magnitude of an external electric field and depends only weakly on magnetic fields. Our findings provide a basis for future quantum and precision experiments with trapped cold molecules.}, archive = {J_PRL}, author = {Maximilian Löw and Martin Ibrügger and Gerhard Rempe and Martin Zeppenfeld}, doi = {10.1103/PhysRevLett.134.113402}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113402}, shortjournal = {Phys. Rev. Lett.}, title = {Coherence of symmetry-protected rotational qubits in cold polyatomic molecules}, volume = {134}, year = {2025}, }
• (2025). Observation of ergodicity breaking and quantum many-body scars in spinor gases. PRL, 134(11), 113401. (www)

  @article{ , abstract = {We experimentally and theoretically demonstrate that spinor gases driven by spin-flopping fields are excellent platforms for investigating ergodicity breaking and quantum scarring. We observe that specific initial states remain nonthermal at weak driving despite the majority of states thermalizing, which constitutes clear evidence of quantum many-body scars (QMBSs). As the driving strength increases, the experimental system undergoes a smooth transition from integrable to weakly ergodicity breaking, which supports QMBSs, and then to fully thermal. This is in agreement with the theoretical spectra, which predict towers of states dissolving with increasing driving strength. This Letter advances the study of QMBSs and quantum scars with applications to, e.g., quantum information storage.}, archive = {J_PRL}, author = {J. O. Austin-Harris and I. Rana and S. E. Begg and C. Binegar and T. Bilitewski and Y. Liu}, doi = {10.1103/PhysRevLett.134.113401}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113401}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of ergodicity breaking and quantum many-body scars in spinor gases}, volume = {134}, year = {2025}, }
• (2025). Quantum logic control of a transition metal ion. PRL, 134(11), 113201. (www)

  @article{ , abstract = {Extending quantum control to increasingly complex systems is crucial for both advancing quantum technologies and fundamental physics. In trapped ion systems, quantum logic techniques that combine a well-controlled logic species with a more complex spectroscopy species have proven to be a powerful tool for extending the range of accessible species. Here, we demonstrate that a quantum system as complex as Ti + 48 with its many metastable states can be controlled employing a combination of intrinsic thermalization due to collisions with background gas and quantum-logic techniques using a far-detuned Raman laser. The preparation of pure quantum states allows coherent manipulation and high resolution measurements of the Zeeman structure in Ti + 48 . The presented techniques are applicable to a wide range of ionic species giving access to a larger variety of systems for fundamental physics and constitute the first step for quantum-controlled spectroscopy of transition metals, relevant, e.g., for the interpretation of astrophysical spectra.}, archive = {J_PRL}, author = {Till Rehmert and Maximilian J. Zawierucha and Kai Dietze and Piet O. Schmidt and Fabian Wolf}, doi = {10.1103/PhysRevLett.134.113201}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {113201}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum logic control of a transition metal ion}, volume = {134}, year = {2025}, }
• (2025). Discovery of the origin of the enormous zr88 neutron-capture cross section and quantifying its impact on applications. PRL, 134(11), 112702. (www)

  @article{ , abstract = {The probability per unit area for a radioactive nucleus (83.4 d half life) to absorb neutrons across resonance energies—its neutron-capture resonance integral—is the largest ever reported [Shusterman et al. , Phys. Rev. C 103 , 024614 (2021) .] and implies that the neutron-capture cross section is orders of magnitude larger than previously thought at energies relevant to nuclear test diagnostics and nucleosynthesis applications such as the process [Xiong et al. , Phys. Rev. Lett. 132 , 192701 (2024) .]. However, these applications require the shape of this cross section across a range of energies, not just this integral quantity. We measured the neutron total cross section from 0.0253 to 500 eV. Because the same resonances or other nuclear structure responsible for the neutron-capture cross section are reflected in the total cross section, we used these data to extract the former from the latter as a function of energy. Our data reveal a resonance at 0.171 eV and result in a thermal neutron-capture cross section of , in good agreement with the recently published value. In contrast, the neutron-capture resonance integral extracted from our data is and is roughly a factor of 200 smaller than the recently reported value. We discuss the impact of this difference on applications.}, archive = {J_PRL}, author = {Athanasios Stamatopoulos and Paul E. Koehler and Brad DiGiovine and Veronika Mocko and Artem Matyskin and Christiaan Vermeulen and Aaron Couture and Andrew Cooper and Jonathan Morrell and Ellen O’Brien}, doi = {10.1103/PhysRevLett.134.112702}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {112702}, shortjournal = {Phys. Rev. Lett.}, title = {Discovery of the origin of the enormous zr88 neutron-capture cross section and quantifying its impact on applications}, volume = {134}, year = {2025}, }
• (2025). First measurement of a weak r-process reaction on a radioactive nucleus. PRL, 134(11), 112701. (www)

  @article{ , abstract = {This Letter reports on the first cross-section measurements for the Sr 94 ( α , n ) Zr 97 and Kr 86 ( α , n ) Sr 89 reactions. In particular, our measurement of Sr 94 ( α , n ) Zr 97 is the first weak r -process reaction cross section obtained using a radioactive ion beam. This experiment was enabled by the use of novel solid helium targets, comprised of silicon thin films with high helium incorporation obtained via a sputtering technique. Yield measurements were performed at center-of-mass energies of 10.4 and 9.0 MeV for the Kr 86 ( α , n ) Sr 89 reaction, and 9.9 MeV for Sr 94 ( α , n ) Zr 97 , extending into the respective Gamow energy windows for a temperature of 5 GK. Reactions were uniquely identified by prompt γ rays detected in coincidence with heavy ions selected by a recoil mass spectrometer. The obtained cross sections are smaller than predicted for both reactions. In the case of Sr 94 ( α , n ) Zr 97 , the reaction rate found here is lowered by an order of magnitude at temperatures below 5 GK, which is expected to impact the predicted abundance of ruthenium, a signature weak r -process element.}, archive = {J_PRL}, author = {M. Williams and C. Angus and A. M. Laird and B. Davids and C. Aa. Diget and A. Fernandez and E. J. Williams and A. N. Andreyev and H. Asch and A. A. Avaa and G. Bartram and S. Chakraborty and I. Dillmann and K. Directo and D. T. Doherty and E. Geerlof and C. J. Griffin and A. Grimes and G. Hackman and J. Henderson and K. Hudson and D. Hufschmidt and J. Jeong and M. C. Jiménez de Haro and V. Karayonchev and A. Katrusiak and A. Lennarz and G. Lotay and B. Marlow and M. S. Martin and S. Molló and F. Montes and J. R. Murias and J. O’Neill and K. Pak and C. Paxman and L. Pedro-Botet and A. Psaltis and E. Raleigh-Smith and D. Rhodes and J. S. Rojo and M. Satrazani and T. Sauvage and C. Shenton and C. E. Svensson and D. Tam and L. Wagner and D. Yates}, doi = {10.1103/PhysRevLett.134.112701}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {112701}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of a weak r-process reaction on a radioactive nucleus}, volume = {134}, year = {2025}, }
• (2025). Extreme softening of QCD phase transition under weak acceleration: First-principles monte carlo results for gluon plasma. PRL, 134(11), 111904. (www)

  @article{ , abstract = {We study the properties of gluon plasma subjected to a weak acceleration using first-principles numerical Monte Carlo simulations. We use the Luttinger (Tolman-Ehrenfest) correspondence between temperature gradient and gravitational field to impose acceleration in imaginary time formalism. Under acceleration, the system resides in global thermal equilibrium. Our results indicate that even the weakest acceleration up to drastically softens the deconfinement phase transition, converting the first-order phase transition of a static system to a soft crossover for accelerating gluons. The accelerating environment can be relevant to the first moments of the early Universe and the initial glasma regime of relativistic heavy ion collisions. In particular, our results imply that the acceleration, if present, may also inhibit the detection of the thermodynamic phase transition from quark-gluon plasma to the hadronic phase.}, archive = {J_PRL}, author = {M. N. Chernodub and V. A. Goy and A. V. Molochkov and D. V. Stepanov and A. S. Pochinok}, doi = {10.1103/PhysRevLett.134.111904}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111904}, shortjournal = {Phys. Rev. Lett.}, title = {Extreme softening of QCD phase transition under weak acceleration: First-principles monte carlo results for gluon plasma}, volume = {134}, year = {2025}, }
• (2025). Search for nuclear modifications of b+ meson production in p-pb collisions at sNN=8.16 TeV. PRL, 134(11), 111903. (www)

  @article{ , abstract = {Nuclear medium effects on B + meson production are studied using the binary-collision scaled cross section ratio between events of different charged-particle multiplicities from proton-lead collisions. Data, collected by the CMS experiment in 2016 at a nucleon-nucleon center-of-mass energy of s NN = 8.16 TeV , corresponding to an integrated luminosity of 175 nb − 1 , were used. The scaling factors in the ratio are determined using a novel approach based on the Z → μ − μ + cross sections measured in the same events. The scaled ratio for B + is consistent with unity for all event multiplicities, putting stringent constraints on nuclear modification for heavy flavor.}, archive = {J_PRL}, author = {CMS Collaboration and A. Hayrapetyan and A. Tumasyan and W. Adam and J. W. Andrejkovic and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and S. Templ and W. Waltenberger and C.-E. Wulz and M. R. Darwish and T. Janssen and P. Van Mechelen and N. Breugelmans and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and F. Heyen and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Clerbaux and A. K. Das and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and D. Hohov and J. Jaramillo and A. Khalilzadeh and F. A. Khan and K. Lee and M. Mahdavikhorrami and A. Malara and S. Paredes and M. A. Shahzad and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and G. Gokbulut and Y. Hong and J. Knolle and L. Lambrecht and D. Marckx and G. Mestdach and K. Mota Amarilo and A. Samalan and K. Skovpen and N. Van Den Bossche and J. van der Linden and L. Wezenbeek and A. Benecke and A. Bethani and G. Bruno and C. Caputo and J. De Favereau De Jeneret and C. Delaere and I. S. Donertas and A. Giammanco and A. O. Guzel and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and S. Wertz and G. A. Alves and M. Alves Gallo Pereira and E. Coelho and G. Correia Silva and C. Hensel and T. Menezes De Oliveira and A. Moraes and P. Rebello Teles and M. Soeiro and A. Vilela Pereira and W. L. Aldá Júnior and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and M. Macedo and J. Martins and C. Mora Herrera and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and I. Maietto Silverio and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and Z. Liang and J. Liu and K. Yi and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and J. Zhao and A. Agapitos and Y. Ban and S. Deng and B. Guo and C. Jiang and A. Levin and C. Li and Q. Li and Y. Mao and S. Qian and S. J. Qian and X. Qin and X. Sun and D. Wang and H. Yang and L. Zhang and Y. Zhao and C. Zhou and S. Yang and Z. You and K. Jaffel and N. Lu and G. Bauer and B. Li and J. Zhang and X. Gao and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and F. Ramirez and C. Rendón and M. Rodriguez and A. A. Ruales Barbosa and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and A. Petkovic and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and S. Mishra and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and C. Leonidou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Carrera Jarrin and Y. Assran and B. El-mahdy and S. Elgammal and A. Lotfy and M. A. Mahmoud and K. Ehataht and M. Kadastik and T. Lange and S. Nandan and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and H. Kirschenmann and K. Osterberg and M. Voutilainen and S. Bharthuar and N. Bin Norjoharuddeen and E. Brücken and F. Garcia and P. Inkaew and K. T. S. Kallonen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and L. Martikainen and M. Myllymäki and M. m. Rantanen and H. Siikonen and J. Tuominiemi and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and P. Busson and A. Cappati and C. Charlot and M. Chiusi and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and M. Nguyen and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and L. Urda Gómez and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and R. Haeberle and A.-C. Le Bihan and M. Meena and O. Poncet and G. Saha and M. A. Sessini and P. Van Hove and P. Vaucelle and A. Di Florio and D. Amram and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and E. Jourd‘huy and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and I. Bagaturia and I. Lomidze and Z. Tsamalaidze and V. Botta and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and D. Pérez Adán and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and D. Noll and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and V. Sarkisovi and A. Schmidt and A. Sharma and J. L. Spah and A. Stein and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and J. Bach and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and S. Bhattacharya and F. Blekman and K. Borras and A. Campbell and A. Cardini and C. Cheng and F. Colombina and S. Consuegra Rodríguez and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and O. Filatov and E. Gallo and A. Geiser and V. Guglielmi and M. Guthoff and A. Hinzmann and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and K. Moral Figueroa and A. Mussgiller and L. P. Nair and J. Niedziela and A. Nürnberg and Y. Otarid and J. Park and E. Ranken and A. Raspereza and D. Rastorguev and J. Rübenach and L. Rygaard and A. Saggio and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and Y. Wen and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bein and L. Benato and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and C. c. Kuo and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and M. Wolf and S. Brommer and M. Burkart and E. Butz and T. Chwalek and A. Dierlamm and A. Droll and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and R. Koppenhöfer and J. M. Lawhorn and M. Link and A. Lintuluoto and B. Maier and S. Maier and S. Mitra and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and N. Shadskiy and I. Shvetsov and H. J. Simonis and L. Sowa and L. Stockmeier and K. Tauqeer and M. Toms and N. Trevisani and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and P. Kontaxakis and G. Melachroinos and Z. Painesis and I. Papavergou and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and K. Adamidis and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and A. Fehérkuti and M. M. A. Gadallah and Á. Kadlecsik and P. Major and G. Pásztor and G. I. Veres and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and J. Babbar and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and K. Sandeep and T. Sheokand and J. B. Singh and A. Singla and A. Ahmed and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and M. K. Saini and S. Saumya and S. Baradia and S. Barman and S. Das Gupta and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and G. Dash and P. Jana and P. Kalbhor and S. Kamble and J. R. Komaragiri and D. Kumar and P. R. Pujahari and N. R. Saha and A. K. Sikdar and R. K. Singh and P. Verma and S. Verma and A. Vijay and S. Dugad and M. Kumar and G. B. Mohanty and B. Parida and M. Shelake and P. Suryadevara and A. Bala and S. Banerjee and R. M. Chatterjee and M. Guchait and Sh. Jain and A. Jaiswal and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and T. Mishra and V. K. Muraleedharan Nair Bindhu and K. Naskar and A. Nayak and S. Nayak and K. Pal and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and A. Jafari and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and Y. Hosseini and M. Khakzad and E. Khazaie and M. Mohammadi Najafabadi and S. Tizchang and M. Felcini and M. Grunewald and M. Abbrescia and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and W. Elmetenawee and L. Fiore and G. Iaselli and L. Longo and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and D. Troiano and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and L. Borgonovi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and M. Lorusso and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and G. Paggi and A. Perrotta and F. Primavera and A. M. Rossi and S. Rossi Tisbeni and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and A. Lapertosa and R. Potenza and A. Tricomi and C. Tuve and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and P. Chatagnon and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and G. Boldrini and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and A. Perego and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and R. Ardino and P. Azzi and N. Bacchetta and P. Bortignon and G. Bortolato and A. Bragagnolo and A. C. M. Bulla and R. Carlin and T. Dorigo and F. Gasparini and U. Gasparini and E. Lusiani and M. Margoni and A. T. Meneguzzo and M. Migliorini and M. Passaseo and J. Pazzini and P. Ronchese and R. Rossin and M. Sgaravatto and F. Simonetto and G. Strong and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and C. Aimè and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and M. E. Ascioti and G. M. Bilei and C. Carrivale and D. Ciangottini and L. Fanò and M. Magherini and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and C. A. Alexe and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and D. Matos Figueiredo and A. Messineo and M. Musich and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and C. Baldenegro Barrera and P. Barria and C. Basile and M. Campana and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and E. Longo and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and L. Menzio and P. Meridiani and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and R. White and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and C. Huh and B. Kim and J. Kim and D. Lee and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and B. Tae and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and Y. Ryou and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and J. Yoo and J. Goh and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and S. Ko and H. Kwon and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and Y. Gharbia and K. Dreimanis and A. Gaile and G. Pikurs and A. Potrebko and M. Seidel and D. Sidiropoulos Kontos and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and J. Mejia Guisao and C. A. Mondragon Herrera and R. Reyes-Almanza and A. Sánchez Hernández and C. Oropeza Barrera and D. L. Ramirez Guadarrama and M. Ramírez García and I. Bautista and I. Pedraza and H. A. Salazar Ibarguen and C. Torres and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and L. Grzanka and M. Malawski and H. Bialkowska and M. Bluj and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and G. B. Marozzo and T. Niknejad and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and M. Dordevic and J. Milosevic and L. Nadderd and V. Rekovic and J. Alcaraz Maestre and Cristina F. Bedoya and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and E. Martin Viscasillas and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and S. Sánchez Navas and J. Sastre and J. Vazquez Escobar and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and J. R. González Fernández and P. Leguina and E. Palencia Cortezon and C. Ramón Álvarez and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Bhowmik and S. Blanco Fernández and J. A. Brochero Cifuentes and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and B. Kailasapathy and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and B. Bilin and A. A. Bin Anuar and A. Bocci and C. Botta and E. Brondolin and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and J. Hegeman and J. K. Heikkilä and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and L. Malgeri and M. Mannelli and A. C. Marini and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and H. Qu and D. Rabady and B. Ribeiro Lopes and M. Rovere and H. Sakulin and S. Sanchez Cruz and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and D. Walter and J. Wanczyk and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and T. K. Aarrestad and K. Androsov and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and P. De Bryas Dexmiers D‘archiac and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and C. Martin Perez and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and C. Reissel and T. Reitenspiess and B. Ristic and F. Riti and R. Seidita and J. Steggemann and A. Tarabini and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and F. Meng and U. Molinatti and J. Motta and A. Reimers and P. Robmann and M. Senger and E. Shokr and F. Stäger and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and S. S. Yu and L. Ceard and K. F. Chen and P. s. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and D. Agyel and F. Boran and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and U. Kiminsu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and S. Turkcapar and E. Uslan and I. S. Zorbakir and G. Sokmen and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and G. G. Dincer and Y. Komurcu and S. Sen and O. Aydilek and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and S. Cerci and B. Isildak and D. Sunar Cerci and T. Yetkin and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and S. Seif El Nasr-Storey and V. J. Smith and N. Stylianou and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and A. Elliot and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and K. C. Whalen and T. Williams and I. Andreou and R. Bainbridge and P. Bloch and C. E. Brown and O. Buchmuller and V. Cacchio and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and J. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and M. H. Hassanshahi and A. Howard and G. Iles and M. Knight and J. Langford and J. León Holgado and L. Lyons and A.-M. Magnan and S. Mallios and M. Mieskolainen and J. Nash and M. Pesaresi and P. B. Pradeep and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and L. H. Vage and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and K. Coldham and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and B. Caraway and E. Collins and J. Dittmann and K. Hatakeyama and J. Hiltbrand and B. McMaster and J. Samudio and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and C. Huerta Escamilla and A. E. Simsek and R. Uniyal and A. M. Vargas Hernandez and B. Bam and A. Buchot Perraguin and R. Chudasama and S. I. Cooper and C. Crovella and S. V. Gleyzer and E. Pearson and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and C. Cosby and G. De Castro and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and J. O‘cain and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and A. G. Zecchinelli and G. Benelli and X. Coubez and D. Cutts and L. Gouskos and M. Hadley and U. Heintz and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and D. Li and J. Luo and S. Mondal and M. Narain and N. Pervan and T. Russell and S. Sagir and F. Simpson and M. Stamenkovic and N. Venkatasubramanian and X. Yan and W. Zhang and S. Abbott and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and S. Ostrom and W. Wei and Y. Yao and S. Yoo and F. Zhang and M. Bachtis and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and M. Gordon and G. Hanson and W. Si and S. Wimpenny and A. Aportela and A. Arora and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and Y. Gu and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and M. Quinnan and B. V. Sathia Narayanan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and K. Downham and C. Grieco and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and S. N. Santpur and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and S. Wang and D. Zhang and A. Bornheim and O. Cerri and A. Latorre and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and M. B. Andrews and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and T. A. Gómez Espinosa and A. Harilal and A. Kallil Tharayil and C. Liu and T. Mudholkar and S. Murthy and P. Palit and K. Park and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and G. Karathanasis and N. Manganelli and A. Perloff and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and S. Bright-Thonney and X. Chen and D. J. Cranshaw and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and J. Dickinson and I. Dutta and V. D. Elvira and Y. Feng and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and R. Heller and T. C. Herwig and J. Hirschauer and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and D. Lincoln and R. Lipton and T. Liu and C. Madrid and K. Maeshima and C. Mantilla and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and S. Norberg and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and M. Safdari and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and P. Chang and V. Cherepanov and R. D. Field and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and S. Rosenzweig and Y. Takahashi and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Habibullah and V. Hagopian and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and B. Alsufyani and M. M. Baarmand and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and M. Rahmani and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and A. H. Merrit and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and T. Roy and S. Rudrabhatla and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and S. Arteaga Escatel and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and N. Minafra and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and R. Salvatico and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and A. Baden and A. Belloni and J. Bistany-riebman and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and B. Kronheim and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and L. Wang and J. Bendavid and I. A. Cali and P. c. Chou and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and C. Mcginn and A. Novak and C. Paus and D. Rankin and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and B. M. Joshi and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and M. Revering and R. Rusack and R. Saradhy and N. Strobbe and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and H. w. Hsia and I. Iashvili and A. Kalogeropoulos and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and P. Young and G. Alverson and E. Barberis and J. Bonilla and J. Dervan and Y. Haddad and Y. Han and A. Krishna and J. Li and M. Lu and G. Madigan and R. Mccarthy and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and D. Wood and J. Bueghly and S. Dittmer and K. A. Hahn and Y. Liu and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. W. Ho and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and B. Bylsma and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and B. L. Winer and B. R. Yates and H. Bouchamaoui and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and K. Kennedy and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and A. Shevelev and D. Stickland and C. Tully and S. Malik and A. S. Bakshi and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and V. Scheurer and J. F. Schulte and M. Stojanovic and J. Thieman and A. K. Virdi and F. Wang and W. Xie and J. Dolen and N. Parashar and A. Pathak and D. Acosta and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and W. Li and J. Lin and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and E. Popova and R. Taus and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and O. Karacheban and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and J. Reichert and H. Routray and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and H. Wang and H. Acharya and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and T. Akhter and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and D. Rathjens and A. Safonov and N. Akchurin and J. Damgov and N. Gogate and V. Hegde and A. Hussain and Y. Kazhykarim and K. Lamichhane and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Neu and P. E. Karchin and A. Aravind and K. Black and T. Bose and S. Dasu and I. De Bruyn and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Alexakhin and D. Budkouski and I. Golutvin and I. Gorbunov and V. Karjavine and V. Korenkov and A. Lanev and A. Malakhov and V. Matveev and V. Palichik and V. Perelygin and M. Savina and V. Shalaev and S. Shmatov and S. Shulha and V. Smirnov and O. Teryaev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and G. Gavrilov and V. Golovtcov and Y. Ivanov and V. Kim and P. Levchenko and V. Murzin and V. Oreshkin and D. Sosnov and V. Sulimov and L. Uvarov and A. Vorobyev and Yu. Andreev and A. Dermenev and S. Gninenko and N. Golubev and A. Karneyeu and D. Kirpichnikov and M. Kirsanov and N. Krasnikov and I. Tlisova and A. Toropin and T. Aushev and V. Gavrilov and N. Lychkovskaya and A. Nikitenko and V. Popov and A. Zhokin and R. Chistov and M. Danilov and S. Polikarpov and V. Andreev and M. Azarkin and M. Kirakosyan and A. Terkulov and E. Boos and A. Ershov and A. Gribushin and A. Kaminskiy and L. Khein and O. Kodolova and V. Korotkikh and S. Obraztsov and S. Petrushanko and V. Savrin and A. Snigirev and I. Vardanyan and V. Blinov and T. Dimova and A. Kozyrev and O. Radchenko and Y. Skovpen and V. Kachanov and D. Konstantinov and S. Slabospitskii and A. Uzunian and A. Babaev and V. Borshch and D. Druzhkin and E. Tcherniaev and V. Chekhovsky and V. Makarenko}, doi = {10.1103/PhysRevLett.134.111903}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111903}, shortjournal = {Phys. Rev. Lett.}, title = {Search for nuclear modifications of b+ meson production in p-pb collisions at sNN=8.16 TeV}, volume = {134}, year = {2025}, }
• (2025). Entanglement as a probe of hadronization. PRL, 134(11), 111902. (www)

  @article{ , abstract = {Recently, it was discovered that the proton structure at high energies exhibits maximal entanglement. This leads to a simple relation between the proton’s parton distributions and the entropy of hadrons produced in high-energy inelastic interactions, which has been experimentally confirmed. In this Letter, we extend this approach to the production of jets. Here, the maximal entanglement predicts a relation between the jet fragmentation function and the entropy of hadrons produced in jet fragmentation. We test this relation using the ATLAS Collaboration data on jet production at the Large Hadron Collider, and find a good agreement between the prediction based on maximal entanglement within the jet and the data. This study represents the first use of a quantum entanglement framework in an experimental study of the hadronization process, offering a new perspective on the transition from perturbative to nonperturbative QCD. Our results open the door to a more comprehensive understanding of the quantum nature of hadronization.}, archive = {J_PRL}, author = {Jaydeep Datta and Abhay Deshpande and Dmitri E. Kharzeev and Charles Joseph Naïm and Zhoudunming Tu}, doi = {10.1103/PhysRevLett.134.111902}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111902}, shortjournal = {Phys. Rev. Lett.}, title = {Entanglement as a probe of hadronization}, volume = {134}, year = {2025}, }
• (2025). Light and strange vector resonances from lattice QCD at physical quark masses. PRL, 134(11), 111901. (www)

  @article{ , abstract = {We present the first ab initio calculation at physical quark masses of scattering amplitudes describing the lightest pseudoscalar mesons interacting via the strong force in the vector channel. Using lattice quantum chromodynamics, we postdict the defining parameters for two short-lived resonances, the and , which manifest as complex energy poles in and scattering amplitudes, respectively. The calculation proceeds by first computing the finite-volume energy spectrum of the two-hadron systems and then determining the amplitudes from the energies using the Lüscher formalism. The error budget includes a data-driven systematic error, obtained by scanning possible fit ranges and fit models to extract the spectrum from Euclidean correlators, as well as the scattering amplitudes from the latter. The final results, obtained by analytically continuing multiple parametrizations into the complex energy plane, are , and , where the subscript indicates the resonance and and stand for the mass and width, respectively, and where the first bracket indicates the statistical and the second bracket the systematic uncertainty.}, archive = {J_PRL}, author = {Peter Boyle and Felix Erben and Vera Gülpers and Maxwell T. Hansen and Fabian Joswig and Michael Marshall and Nelson Pitanga Lachini and Antonin Portelli}, doi = {10.1103/PhysRevLett.134.111901}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111901}, shortjournal = {Phys. Rev. Lett.}, title = {Light and strange vector resonances from lattice QCD at physical quark masses}, volume = {134}, year = {2025}, }
• (2025). Topological portal to the dark sector. PRL, 134(11), 111804. (www)

  @article{ , abstract = {We propose a unique topological portal between quantum chromodynamics (QCD) and a dark sector characterized by a global symmetry breaking, which connects three QCD to two dark pions. When gauged, it serves as the leading portal between the two sectors, providing an elegant, self-consistent scenario of light thermal inelastic dark matter. The inherent antisymmetrization leads to diminished annihilations at later times and suppressed direct detection. However, novel collider signatures offer tremendous prospects for discovery at Belle II.}, archive = {J_PRL}, author = {Joe Davighi and Admir Greljo and Nudžeim Selimović}, doi = {10.1103/PhysRevLett.134.111804}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111804}, shortjournal = {Phys. Rev. Lett.}, title = {Topological portal to the dark sector}, volume = {134}, year = {2025}, }
• (2025). Hybrid SO(10) axion model without quality problem. PRL, 134(11), 111803. (www)

  @article{ , abstract = {Invisible axion models that solve the strong problem via the Peccei-Quinn (PQ) mechanism typically have a quality problem that arises from quantum gravity effects which violate all global symmetries. These models therefore require extreme fine-tuning of parameters for consistency. We present a new solution to the quality problem in a unified gauge model, where is an anomaly free axial gauge symmetry. PQ symmetry emerges as an accidental symmetry in this setup, which admits a PQ breaking scale as large as , allowing for the axion to be the cosmological dark matter. We call this a hybrid axion model due to its unique feature that it interpolates between the popular KSVZ and DFSZ axion models. Its predictions for the experimentally measurable axion couplings to the nucleon and electron are distinct from those of the usual models, a feature that can be used to test it. Furthermore, the model has no domain wall problem and it provides a realistic and predictive framework for fermion masses and mixings.}, archive = {J_PRL}, author = {K. S. Babu and Bhaskar Dutta and Rabindra N. Mohapatra}, doi = {10.1103/PhysRevLett.134.111803}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111803}, shortjournal = {Phys. Rev. Lett.}, title = {Hybrid SO(10) axion model without quality problem}, volume = {134}, year = {2025}, }
• (2025). First search for light dark matter in the neutrino fog with XENONnT. PRL, 134(11), 111802. (www)

  @article{ , abstract = {We search for dark matter (DM) with a mass using an exposure of with the XENONnT experiment. We consider spin-independent DM-nucleon interactions mediated by a heavy or light mediator, spin-dependent DM-neutron interactions, momentum-dependent DM scattering, and mirror DM. Using a lowered energy threshold compared to the previous weakly interacting massive particle search, a blind analysis of [0.5, 5.0] keV nuclear recoil events reveals no significant signal excess over the background. XENONnT excludes spin-independent DM-nucleon cross sections at 90% confidence level for DM. In the considered mass range, the DM sensitivity approaches the “neutrino fog,” the limitation where neutrinos produce a signal that is indistinguishable from that of light DM-xenon nucleus scattering.}, archive = {J_PRL}, author = {XENON Collaboration and E. Aprile and J. Aalbers and K. Abe and S. Ahmed Maouloud and L. Althueser and B. Andrieu and E. Angelino and D. Antón Martin and F. Arneodo and L. Baudis and M. Bazyk and L. Bellagamba and R. Biondi and A. Bismark and K. Boese and A. Brown and G. Bruno and R. Budnik and C. Cai and C. Capelli and J. M. R. Cardoso and A. P. Cimental Chávez and A. P. Colijn and J. Conrad and J. J. Cuenca-García and V. D’Andrea and L. C. Daniel Garcia and M. P. Decowski and A. Deisting and C. Di Donato and P. Di Gangi and S. Diglio and K. Eitel and S. el Morabit and A. Elykov and A. D. Ferella and C. Ferrari and H. Fischer and T. Flehmke and M. Flierman and W. Fulgione and C. Fuselli and P. Gaemers and R. Gaior and M. Galloway and F. Gao and S. Ghosh and R. Giacomobono and R. Glade-Beucke and L. Grandi and J. Grigat and H. Guan and M. Guida and P. Gyorgy and R. Hammann and A. Higuera and C. Hils and L. Hoetzsch and N. F. Hood and M. Iacovacci and Y. Itow and J. Jakob and F. Joerg and Y. Kaminaga and M. Kara and P. Kavrigin and S. Kazama and M. Kobayashi and D. Koke and A. Kopec and H. Landsman and R. F. Lang and L. Levinson and I. Li and S. Li and S. Liang and Y.-T. Lin and S. Lindemann and M. Lindner and K. Liu and M. Liu and J. Loizeau and F. Lombardi and J. Long and J. A. M. Lopes and T. Luce and Y. Ma and C. Macolino and J. Mahlstedt and A. Mancuso and L. Manenti and F. Marignetti and T. Marrodán Undagoitia and K. Martens and J. Masbou and E. Masson and S. Mastroianni and A. Melchiorre and J. Merz and M. Messina and A. Michael and K. Miuchi and A. Molinario and S. Moriyama and K. Morå and Y. Mosbacher and M. Murra and J. Müller and K. Ni and U. Oberlack and B. Paetsch and Y. Pan and Q. Pellegrini and R. Peres and C. Peters and J. Pienaar and M. Pierre and G. Plante and T. R. Pollmann and L. Principe and J. Qi and J. Qin and D. Ramírez García and M. Rajado and R. Singh and L. Sanchez and J. M. F. dos Santos and I. Sarnoff and G. Sartorelli and J. Schreiner and P. Schulte and H. Schulze Eißing and M. Schumann and L. Scotto Lavina and M. Selvi and F. Semeria and P. Shagin and S. Shi and J. Shi and M. Silva and H. Simgen and C. Szyszka and A. Takeda and P.-L. Tan and D. Thers and F. Toschi and G. Trinchero and C. D. Tunnell and F. Tönnies and K. Valerius and S. Vecchi and S. Vetter and F. I. Villazon Solar and G. Volta and C. Weinheimer and M. Weiss and D. Wenz and C. Wittweg and V. H. S. Wu and Y. Xing and D. Xu and Z. Xu and M. Yamashita and L. Yang and J. Ye and L. Yuan and G. Zavattini and M. Zhong}, doi = {10.1103/PhysRevLett.134.111802}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111802}, shortjournal = {Phys. Rev. Lett.}, title = {First search for light dark matter in the neutrino fog with XENONnT}, volume = {134}, year = {2025}, }
• (2025). Observation of d+→η′μ+νμ and first experimental study of d+→η′ℓ+νℓ decay dynamics. PRL, 134(11), 111801. (www)

  @article{ , abstract = {Using of collision data collected at the center-of-mass energy 3.773 GeV with the BESIII detector, we report the first observation of the semileptonic decay with significance of including systematic uncertainties, and an improved measurement of . The branching fractions of and are determined to be and , respectively. The ratio of the two branching fractions is determined to be , which agrees with the theoretical expectation of lepton flavor universality within the standard model. From an analysis of the decay dynamics, the product of the hadronic form factor and the Cabibbo-Kobayashi-Maskawa matrix element is measured for the first time, giving . The mixing angle in the quark flavor basis is determined to be .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and J. F. Chang and G. R. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and J. J. Lane and L. Lavezzi and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and L. R. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. Ma and Y. M. Ma and F. E. Maas and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and H. C. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and S. S. Su and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. Xu and Y. C. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. X. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Junhao Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and M. C. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. D. Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and Z. Z. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and Z. C. Zhou and A. N. Zhu and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and T. J. Zhu and W. D. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.111801}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111801}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of d+→η′μ+νμ and first experimental study of d+→η′ℓ+νℓ decay dynamics}, volume = {134}, year = {2025}, }
• (2025). One-loop N-point correlators in pure gravity. PRL, 134(11), 111602. (www)

  @article{ , abstract = {In this Letter we propose a simple algebraic recursion for the complete one-loop integrands of -graviton correlators. This formula automatically yields the correct symmetry factors of individual diagrams, taking into account both the graviton and the ghost loop, and seamlessly controlling the related combinatorics.}, archive = {J_PRL}, author = {Humberto Gomez and Renann Lipinski Jusinskas and Cristhiam Lopez-Arcos and Alexander Quintero Vélez}, doi = {10.1103/PhysRevLett.134.111602}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111602}, shortjournal = {Phys. Rev. Lett.}, title = {One-loop N-point correlators in pure gravity}, volume = {134}, year = {2025}, }
• (2025). Higher fermions in supergravity. PRL, 134(11), 111601. (www)

  @article{ , abstract = {We show that the generalized geometry formalism provides a new approach to the description of higher-fermion terms in 𝒩 = 1 supergravity in ten dimensions, which does not appeal to supercovariantization or superspace. We find expressions containing only five higher-fermion terms across the action and supersymmetry transformations, working in the second-order formalism.}, archive = {J_PRL}, author = {Julian Kupka and Charles Strickland-Constable and Fridrich Valach}, doi = {10.1103/PhysRevLett.134.111601}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111601}, shortjournal = {Phys. Rev. Lett.}, title = {Higher fermions in supergravity}, volume = {134}, year = {2025}, }
• (2025). New method for the astrometric direct detection of ultralight dark matter. PRL, 134(11), 111003. (www)

  @article{ , abstract = {Ultralight dark matter induces time-dependent perturbations in the spacetime metric, enabling its gravitational direct detection . In this Letter, we propose using astrometry to detect dark matter. After reviewing the calculation of the metric in the presence of scalar dark matter, we study the influence of the perturbations on the apparent motion of astrophysical bodies. We apply our results to angular position measurements of quasars, whose vast distances from Earth present an opportunity to discover subcomponent dark matter with a mass as low as . We explore the prospects of very long baseline interferometry and optical astrometric survey measurements for detecting ultralight relics, finding that for the smallest masses, current astrometric surveys can detect dark matter moving locally with a velocity of with energy density as low as .}, archive = {J_PRL}, author = {Jeff A. Dror and Sarunas Verner}, doi = {10.1103/PhysRevLett.134.111003}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111003}, shortjournal = {Phys. Rev. Lett.}, title = {New method for the astrometric direct detection of ultralight dark matter}, volume = {134}, year = {2025}, }
• (2025). ADMX axion dark matter bounds around 3.3 μeV with dine-fischler-srednicki-zhitnitsky discovery ability. PRL, 134(11), 111002. (www)

  @article{ , abstract = {We report the results of a QCD axion dark matter search with discovery ability for Dine-Fischler-Srednicki-Zhitnitsky (DFSZ) axions using an axion haloscope. Sub-Kelvin noise temperatures are reached with an ultralow noise Josephson parametric amplifier cooled by a dilution refrigerator. This work excludes (with a 90% confidence level) DFSZ axions with masses between 3.27 to 3.34 μ eV , assuming a standard halo model with a local energy density of 0.45 G e V / cm 3 made up 100% of axions.}, archive = {J_PRL}, author = {C. Goodman and M. Guzzetti and C. Hanretty and L. J. Rosenberg and G. Rybka and J. Sinnis and D. Zhang and John Clarke and I. Siddiqi and A. S. Chou and M. Hollister and S. Knirck and A. Sonnenschein and T. J. Caligiure and J. R. Gleason and A. T. Hipp and P. Sikivie and M. E. Solano and N. S. Sullivan and D. B. Tanner and R. Khatiwada and G. Carosi and C. Cisneros and N. Du and N. Robertson and N. Woollett and L. D. Duffy and C. Boutan and T. Braine and E. Lentz and N. S. Oblath and M. S. Taubman and E. J. Daw and C. Mostyn and M. G. Perry and C. Bartram and T. A. Dyson and S. Ruppert and M. O. Withers and C. L. Kuo and B. T. McAllister and J. H. Buckley and C. Gaikwad and J. Hoffman and K. Murch and M. Goryachev and E. Hartman and A. Quiskamp and M. E. Tobar and ADMX Collaboration}, doi = {10.1103/PhysRevLett.134.111002}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111002}, shortjournal = {Phys. Rev. Lett.}, title = {ADMX axion dark matter bounds around 3.3 μeV with dine-fischler-srednicki-zhitnitsky discovery ability}, volume = {134}, year = {2025}, }
• (2025). Constraints on velocity and spin dependent exotic interaction at the millimeter scale with a diamagnetic-levitated force sensor. PRL, 134(11), 111001. (www)

  @article{ , abstract = {Light bosons, beyond the standard model and as prominent candidates for dark matter, can mediate velocity and spin dependent exotic interaction between electron spins and nucleons. At short ranges, it remains an open challenge to test this exotic interaction with high precision. Here, we present a method based on a diamagnetic-levitated force sensor to detect the exotic interaction at the millimeter scale. Improved constraints for the coupling g A e g V N are established, within the force range spanning from 0.15 to 1.5 mm. The constraint | g A e g V N | ≤ 4.39 × 10 − 26 at λ = 0.5 mm at the 95% confidence level significantly surpasses previous results by more than 3 orders of magnitude. The diamagnetic levitation force measurement system developed here can also be repurposed to probe other exotic spin dependent interactions, such as the exotic spin-spin interaction. This system provides a platform for the exploration of dark matter.}, archive = {J_PRL}, author = {Kenan Tian and Yuanji Sheng and Rui Li and Lei Wang and Peiran Yin and Shaochun Lin and Dingjiang Long and Chang-Kui Duan and Xi Kong and Pu Huang and Jiangfeng Du}, doi = {10.1103/PhysRevLett.134.111001}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {111001}, shortjournal = {Phys. Rev. Lett.}, title = {Constraints on velocity and spin dependent exotic interaction at the millimeter scale with a diamagnetic-levitated force sensor}, volume = {134}, year = {2025}, }
• (2025). Krylov shadow tomography: Efficient estimation of quantum fisher information. PRL, 134(11), 110802. (www)

  @article{ , abstract = {Efficiently estimating the quantum Fisher information (QFI) is pivotal in quantum information science but remains an outstanding challenge for large systems due to its high nonlinearity. In this Letter, we tackle this long-standing challenge by integrating the Krylov subspace method–a celebrated tool from applied mathematics–into the framework of shadow tomography. The integrated technique, dubbed Krylov shadow tomography, enables us to formulate a strict hierarchy of nonpolynomial lower bounds on the QFI, among which the highest one matches the QFI exactly. We show that all the bounds can be expressed as expected values of the inverses of Hankel matrices, which are accessible via shadow tomography. Our Krylov shadow tomography therefore opens up a resource-efficient and experimentally feasible avenue to estimate not only nonpolynomial lower bounds but also the QFI itself.}, archive = {J_PRL}, author = {Da-Jian Zhang and D. M. Tong}, doi = {10.1103/PhysRevLett.134.110802}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {110802}, shortjournal = {Phys. Rev. Lett.}, title = {Krylov shadow tomography: Efficient estimation of quantum fisher information}, volume = {134}, year = {2025}, }
• (2025). Levitated ferromagnetic magnetometer with energy resolution well below ℏ. PRL, 134(11), 110801. (www)

  @article{ , abstract = {A quantum limit on the measurement of magnetic fields has been recently pointed out, stating that the so-called energy resolution E R is bounded to E R ≳ ℏ . This limit indeed holds true for the vast majority of existing quantum magnetometers, including superconducting quantum interference devices and solid state spin and optically pumped atomic magnetometers. However, it can be surpassed by highly correlated spin systems, as recently demonstrated with a single-domain spinor BEC. Here, we show that similar and potentially much better resolution can be achieved with a hard ferromagnet levitated above a superconductor at cryogenic temperature. We demonstrate E R = ( 0.064 ± 0.010 ) ℏ and anticipate that E R < 10 − 3 ℏ is within reach with near-future improvements. This finding opens the way to new applications in condensed matter, biophysics, and fundamental science. In particular, we propose an experiment to search for axionlike dark matter and project a sensitivity that is orders of magnitude better than in previous searches.}, archive = {J_PRL}, author = {Felix Ahrens and Wei Ji and Dmitry Budker and Chris Timberlake and Hendrik Ulbricht and Andrea Vinante}, doi = {10.1103/PhysRevLett.134.110801}, journal = {Physical Review Letters}, month = {3}, number = {11}, pages = {110801}, shortjournal = {Phys. Rev. Lett.}, title = {Levitated ferromagnetic magnetometer with energy resolution well below ℏ}, volume = {134}, year = {2025}, }
• (2025). Erratum: Non-hermitian random matrices and the calogero-sutherland model [Phys. rev. lett. 87, 194102 (2001)]. PRL, 134(10), 109901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 109901 (2025)}, archive = {J_PRL}, author = {Pragya Shukla}, doi = {10.1103/PhysRevLett.134.109901}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {109901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Non-hermitian random matrices and the calogero-sutherland model [Phys. rev. lett. 87, 194102 (2001)]}, volume = {134}, year = {2025}, }
• (2025). Biased lévy walk enables light gradient sensing in euglena gracilis. PRL, 134(10), 108301. (www)

  @article{ , abstract = {We examine the navigation behavior of the photosensitive alga Euglena gracilis in confined environments. Under uniform lighting conditions, E. gracilis exhibits stochastic movements with nearly straight runs interrupted by abrupt directional changes. The lengths of these runs follow a long-tailed distribution typical of a Lévy walk, with scaling exponents that vary with light intensity. In gradient lighting conditions, the cells modulate their run durations—extending them upon detecting an increase in light intensity and shortening them when a decrease is detected. This adjustment effectively biases the Lévy walk, enabling the cells to ascend the spatial light gradient. This behavior mirrors well-known prokaryotic stochastic navigation strategies, such as bacterial chemotaxis, offering a eukaryotic parallel. The experimental observations under varied lighting conditions are consistently replicated through an agent-based model.}, archive = {J_PRL}, author = {Yu’an Li and Yongfeng Zhao and Siyuan Yang and Min Tang and H. P. Zhang}, doi = {10.1103/PhysRevLett.134.108301}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {108301}, shortjournal = {Phys. Rev. Lett.}, title = {Biased lévy walk enables light gradient sensing in euglena gracilis}, volume = {134}, year = {2025}, }
• (2025). Defects enhance stability in 12-fold symmetric soft-matter quasicrystals. PRL, 134(10), 108201. (www)

  @article{ , abstract = {Quasicrystals are materials that exhibit long-range order without translational periodicity. In soft matter, the most commonly observed quasicrystal has 12-fold symmetry and consists of tilings made out of squares and triangles. Intriguingly, both in experiments and simulations, these tilings nearly always appear with many point defects. These defects can be decomposed into squares, triangles, and an additional tile: a rhombus. In this Letter, we explore how rhombus tiles change the entropy of square-triangle 12-fold quasicrystals. We introduce a novel lattice-based Monte Carlo simulation method that uses open boundaries to allow the concentration of different tile types to fluctuate. Our simulations show that rhombus tiles significantly increase the configurational entropy of the quasicrystal phase, enhancing its stability. These findings highlight the critical role of defects in stabilizing soft-matter quasicrystals.}, archive = {J_PRL}, author = {Alptuğ Ulugöl and Robert J. Hardeman and Frank Smallenburg and Laura Filion}, doi = {10.1103/PhysRevLett.134.108201}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {108201}, shortjournal = {Phys. Rev. Lett.}, title = {Defects enhance stability in 12-fold symmetric soft-matter quasicrystals}, volume = {134}, year = {2025}, }
• (2025). Metadensity functional theory for classical fluids: Extracting the pair potential. PRL, 134(10), 107301. (www)

  @article{ , abstract = {The excess free energy functional of classical density functional theory depends upon the type of fluid model, specifically on the choice of (pair) potential. This functional is unknown in general and is approximated reliably only in special cases. We present a machine learning scheme for training a neural network that acts as a generic metadensity functional for truncated but otherwise arbitrary pair potentials. Automatic differentiation and neural functional calculus then yield, for one-dimensional fluids, accurate predictions for inhomogeneous states and immediate access to the pair distribution function. The approach provides a means of addressing a fundamental problem in the physics of liquids and for soft matter design: “How do we best invert structural data to obtain the pair potential?”}, archive = {J_PRL}, author = {Stefanie M. Kampa and Florian Sammüller and Matthias Schmidt and Robert Evans}, doi = {10.1103/PhysRevLett.134.107301}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {107301}, shortjournal = {Phys. Rev. Lett.}, title = {Metadensity functional theory for classical fluids: Extracting the pair potential}, volume = {134}, year = {2025}, }
• (2025). Self-injection locked and phase offset-free micromechanical frequency combs. PRL, 134(10), 107201. (www)

  @article{ , abstract = {Pure mechanical frequency combs attracted a lot of attention recently due to the intriguing nonlinear dynamics and potential of miniatured precision timekeeping but are currently limited by narrow spectra and missing frequency locking physics. In this Letter, we report the design and experiment of a self-injection locked micromechanical frequency comb that is further intrinsically immune to phase offset. We show that by tuning the pump frequency of a pair of nonlinearly coupled flexural and torsional oscillations, self-injection locking could be achieved via aligning the comb teeth from neighboring harmonic clusters, leading to decade-wide cascading of hundreds of equidistant teeth. Inside the injection locking region, the stability of the comb spacing and the phase noise are significantly improved. Moreover, the phase offset in the temporal signal also disappears because all comb lines are locked as integer multiples of the comb spacing and the first tooth is locked to the d.c. frequency due to the comb origination from harmonics. The observation of self-injection locking and zero phase offset in mechanical frequency combs greatly promotes their value for precision applications.}, archive = {J_PRL}, author = {Jiahao Wu and Penghui Song and Shuke Zang and Zian Mao and Wenming Zhang and Lei Shao}, doi = {10.1103/PhysRevLett.134.107201}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {107201}, shortjournal = {Phys. Rev. Lett.}, title = {Self-injection locked and phase offset-free micromechanical frequency combs}, volume = {134}, year = {2025}, }
• (2025). Phase locking and fractional shapiro steps in collective dynamics of microparticles. PRL, 134(10), 107102. (www)

  @article{ , abstract = {In driven nonlinear systems, phase locking is an intriguing effect leading to robust stationary states that are stable over extended ranges of control parameters. Recent experiments allow for exploring microscopic mechanisms underlying such phenomena in collective dynamics of micro- and nanoparticles. Here, we show that phase-locked dynamics of hardcore-interacting microparticles in a densely populated periodic potential under time-periodic driving arises from running solitary cluster waves. We explain how values of phase-locked currents are related to soliton velocities and why collective particle dynamics synchronize with the driving for certain particle diameters only. Our analysis is based on an effective potential for the solitary wave propagation and a unit displacement law, which states that the total average shift of all particle positions per soliton period equals one wavelength of the periodic potential.}, archive = {J_PRL}, author = {Seemant Mishra and Artem Ryabov and Philipp Maass}, doi = {10.1103/PhysRevLett.134.107102}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {107102}, shortjournal = {Phys. Rev. Lett.}, title = {Phase locking and fractional shapiro steps in collective dynamics of microparticles}, volume = {134}, year = {2025}, }
• (2025). Thermomajorization mpemba effect. PRL, 134(10), 107101. (www)

  @article{ , abstract = {The Mpemba effect is a counterintuitive physical phenomenon where a hot system cools faster than a warm one. In recent years, theoretical analyses of the Mpemba effect have been developed for microscopic systems and experimentally verified. However, the conventional theory relies on a specific choice of distance measure to quantify relaxation speed, leading to several theoretical ambiguities. In this Letter, we derive a rigorous quantification of the Mpemba effect based on thermomajorization theory, referred to as the thermomajorization Mpemba effect. This approach resolves all existing ambiguities and provides a unification of the conventional Mpemba effect across all monotone measures. Furthermore, we demonstrate the generality of the thermomajorization Mpemba effect for Markovian dynamics, rigorously proving that it can occur in any temperature regime with fixed energy levels.}, archive = {J_PRL}, author = {Tan Van Vu and Hisao Hayakawa}, doi = {10.1103/PhysRevLett.134.107101}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {107101}, shortjournal = {Phys. Rev. Lett.}, title = {Thermomajorization mpemba effect}, volume = {134}, year = {2025}, }
• (2025). Using light to polarize and detect electron spins in silicon. PRL, 134(10), 106902. (www)

  @article{ , abstract = {Despite decades of research, demonstration of all-optical detection and control of free electron spins in silicon remains elusive. Here, we directly probe the electron spin properties in bulk silicon by measuring the polarization of luminescence following circularly polarized light excitation. The all-optical experiments performed for both direct and indirect gap excitation allow not only an experimental determination of the optical selection rules in silicon for the different phonon-assisted transitions but they also lead to the measurement of the spin relaxation of electrons in conditions that are not accessible using transport techniques. We also measure the spin properties of free excitons in bulk silicon, a very little explored field.}, archive = {J_PRL}, author = {Xavier Marie and Delphine Lagarde and Andrea Balocchi and Cédric Robert and Laurent Lombez and Pierre Renucci and Thierry Amand and Fabian Cadiz}, doi = {10.1103/PhysRevLett.134.106902}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106902}, shortjournal = {Phys. Rev. Lett.}, title = {Using light to polarize and detect electron spins in silicon}, volume = {134}, year = {2025}, }
• (2025). Loss-enabled chirality inversion in terahertz metasurfaces. PRL, 134(10), 106901. (www)

  @article{ , abstract = {Exceptional points (EPs), known as non-Hermitian degeneracies featuring missing eigenspace dimensions, have led to a variety of intriguing wave phenomena in various physical platforms. Chiral EPs collapsing in two orthogonal eigenstates can lead to unique effects and applications, such as loss-induced transparency, EP-enhanced sensing, and chirality-reversal electronics, etc. However, in previous experiments, chiral EPs were typically induced in fixed structures with inherent active gains or nearby nanotips, which are unfavorable for on-chip integrations with low-power elements. Here, we demonstrate the active control of EPs chirality in situ with exceptional-line metasurface. Selective chirality inversion can be well achieved by only light-induced loss without altering the metasurface size. We also perform an ultrafast chirality switch in the picosecond level within transient disturbance. In a broader view, our results provide a platform for the investigation of metasurface-based non-Hermitian physics and active EP modulation, which can stimulate exciting works along this line in near future.}, archive = {J_PRL}, author = {Weibao He and Shun Wan and Yunlan Zuo and Siyang Hu and Ziheng Ren and Zhongyi Yu and Dongsheng Yang and Xiang’ai Cheng and Keyu Xia and Yuze Hu and Hui Jing and Tian Jiang}, doi = {10.1103/PhysRevLett.134.106901}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106901}, shortjournal = {Phys. Rev. Lett.}, title = {Loss-enabled chirality inversion in terahertz metasurfaces}, volume = {134}, year = {2025}, }
• (2025). Ferroelectric switchable altermagnetism. PRL, 134(10), 106802. (www)

  @article{ , abstract = {We propose a novel ferroelectric switchable altermagnetism effect: the reversal of ferroelectric polarization is coupled to the switching of altermagnetic spin splitting. We demonstrate the design principles for the ferroelectric altermagnets and the additional symmetry constraints necessary for switching the spin splitting through flipping the electric polarization based on the state-of-the-art spin-group symmetry techniques. We find 22 ferroelectric altermagnets by screening through the 2001 experimental reported magnetic structures in the MAGNDATA database and identify two of them as ferroelectric switchable altermagnets. Using the hybrid improper ferroelectric material as an example, we show how the altermagnetic spin splitting is tightly coupled to the ferroelectric polarization, providing an ideal platform for designing electric-field-controllable multiferroic devices. Finally, we find that such manipulation of altermagnetism can be detected by monitoring the physical quantities that are related to the nonvanishing Berry curvature dipole, such as the linearly polarized photogalvanic spin current.}, archive = {J_PRL}, author = {Mingqiang Gu and Yuntian Liu and Haiyuan Zhu and Kunihiro Yananose and Xiaobing Chen and Yongkang Hu and Alessandro Stroppa and Qihang Liu}, doi = {10.1103/PhysRevLett.134.106802}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106802}, shortjournal = {Phys. Rev. Lett.}, title = {Ferroelectric switchable altermagnetism}, volume = {134}, year = {2025}, }
• (2025). Antiferroelectric altermagnets: Antiferroelectricity alters magnets. PRL, 134(10), 106801. (www)

  @article{ , abstract = {Magnetoelectric coupling is crucial for uncovering fundamental phenomena and advancing technologies in high-density data storage and energy-efficient devices. The emergence of altermagnets, which unify the advantages of ferromagnets and antiferromagnets, offers unprecedented opportunities for magnetoelectric coupling. However, electrically tuning altermagnets remains an outstanding challenge. Here, we demonstrate how this challenge can be overcome by using antiferroelectricity and ferroelectricity to modulate the spin splitting in altermagnets, employing a universal, symmetry-based design principle supported by an effective model. We introduce an unexplored class of multiferroics: antiferroelectric altermagnets (AFEAM), where antiferroelectricity and altermagnetism coexist in a single material. From first-principles calculations, we validate the feasibility of AFEAM in well-established van der Waals metal thio(seleno)phosphates and perovskite oxides. We reveal the design of AFEAM ranging from two-dimensional monolayers to three-dimensional bulk structures. Remarkably, even a weak electric field can effectively toggle spin polarization in the AFEAM by switching between antiferroelectric and ferroelectric states. Our findings not only enrich the understanding of magnetoelectric coupling but also pave the way for electrically controlled spintronic and multiferroic devices.}, archive = {J_PRL}, author = {Xunkai Duan and Jiayong Zhang and Ziye Zhu and Yuntian Liu and Zhenyu Zhang and Igor Žutić and Tong Zhou}, doi = {10.1103/PhysRevLett.134.106801}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106801}, shortjournal = {Phys. Rev. Lett.}, title = {Antiferroelectric altermagnets: Antiferroelectricity alters magnets}, volume = {134}, year = {2025}, }
• (2025). Revealing quadrupolar excitations with nonlinear spectroscopy. PRL, 134(10), 106703. (www)

  @article{ , abstract = {Local moments with a spin S > 1 / 2 can exhibit a rich variety of elementary quasiparticle excitations, such as quadrupolar excitations, that go beyond the dipolar magnons of conventional spin- 1 / 2 systems. However, the experimental observation of such quadrupolar excitations is often challenging due to the dipolar selection rules of many linear response probes, rendering them invisible. Here we show that nonlinear spectroscopy, in the form of two-dimensional coherent spectroscopy (2DCS), can be used to reveal quadrupolar excitations. Considering a family of spin-1 Heisenberg ferromagnets with single-ion easy-axis anisotropy as an example, we explicitly calculate their 2DCS signature by combining exact diagonalization and generalized spin wave theory. We further demonstrate that 2DCS can provide access to the quadrupolar weight of an excitation, analogous to how linear response provides access to the dipolar weight. Our work highlights the potential of nonlinear spectroscopy as a powerful tool to diagnose multipolar excitations in quantum magnets.}, archive = {J_PRL}, author = {Yoshito Watanabe and Simon Trebst and Ciarán Hickey}, doi = {10.1103/PhysRevLett.134.106703}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106703}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing quadrupolar excitations with nonlinear spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Fluctuations in spin dynamics excited by pulsed light. PRL, 134(10), 106702. (www)

  @article{ , abstract = {We theoretically investigate nonequilibrium spin fluctuations in a ferromagnet induced by a light pulse. Using a Lindblad equation consistent with the Landau-Lifshitz-Gilbert equation, we compute the autocorrelation function of magnetization. Our analysis reveals that this function comprises both thermal and nonequilibrium components. To examine the latter in detail, we introduce a Fano factor similar to nonequilibrium current noise in electronic circuits. We demonstrate that this factor encapsulates insights into the transfer of spin units to the environment. Our findings lay the groundwork for nonequilibrium spin noise spectroscopy, offering valuable insights into spin relaxation dynamics.}, archive = {J_PRL}, author = {Tetsuya Sato and Shinichi Watanabe and Mamoru Matsuo and Takeo Kato}, doi = {10.1103/PhysRevLett.134.106702}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106702}, shortjournal = {Phys. Rev. Lett.}, title = {Fluctuations in spin dynamics excited by pulsed light}, volume = {134}, year = {2025}, }
• (2025). Field-angle-resolved specific heat in Na2Co2TeO6: Evidence against kitaev quantum spin liquid. PRL, 134(10), 106701. (www)

  @article{ , abstract = {Kitaev quantum spin liquids (KSLs) in layered honeycomb magnets are known to host Majorana quasiparticles, whose excitations depend strongly on the direction of the applied magnetic field. In the high-field phase of , specific heat measurements have revealed characteristic field-angle dependence of low-energy excitations consistent with the Kitaev model, providing bulk evidence for the KSL state. Here we present low-temperature measurements of specific heat for another KSL candidate (NCTO) under field rotation within the honeycomb plane. Above the critical field of antiferromagnetic order, the field-angle dependence of exhibits minima along the bond directions, contrasting with the maxima observed in the KSL state of . Our analysis indicates nodeless, fully gapped excitations, which are inconsistent with the angle-dependent Majorana excitations with gapless nodes predicted by the Kitaev model. These findings suggest that low-energy excitations in NCTO are governed by gapped magnon excitations rather than Majorana quasiparticles, providing thermodynamic evidence against a KSL state.}, archive = {J_PRL}, author = {Shengjie Fang and Kumpei Imamura and Yuta Mizukami and Ryuichi Namba and Kota Ishihara and Kenichiro Hashimoto and Takasada Shibauchi}, doi = {10.1103/PhysRevLett.134.106701}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106701}, shortjournal = {Phys. Rev. Lett.}, title = {Field-angle-resolved specific heat in Na2Co2TeO6: Evidence against kitaev quantum spin liquid}, volume = {134}, year = {2025}, }
• (2025). Topological degeneracy induced by twisting. PRL, 134(10), 106601. (www)

  @article{ , abstract = {In recent years, twisting has emerged as a new degree of freedom that plays an increasingly important role in Bloch bands of various physical systems. However, there is currently a lack of reports on the nontrivial physics of topological degeneracy in twisted systems. In this Letter, we investigated the intrinsic physical correlation between twisting and topological degeneracy. We found that twisting not only breaks the symmetry of the system but also introduces topological degeneracy that does not exist under the original symmetric system without twisting. Furthermore, the topological degeneracy can be easily tuned through twisting. This new twist-induced topological degeneracy gives rise to a unique polarization-degenerate birefringent medium, wherein the twist angle acts as a novel degree of freedom for dispersion and polarization management of interface states. Exhibiting fascinating properties and experimental feasibilities, our Letter points to new possibilities in the research of various topological physics in twisted photonics.}, archive = {J_PRL}, author = {Han Peng and Qiang Wang and Meng Xiao and Xiayi Wang and Shining Zhu and Hui Liu}, doi = {10.1103/PhysRevLett.134.106601}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106601}, shortjournal = {Phys. Rev. Lett.}, title = {Topological degeneracy induced by twisting}, volume = {134}, year = {2025}, }
• (2025). Exploring a new regime of molecular orbital physics in 4d cluster magnets with resonant inelastic X-ray scattering. PRL, 134(10), 106504. (www)

  @article{ , abstract = {Molecular orbital systems with clusters of heavy transition metal (TM) ions are one of the most important classes of model materials for studying the interplay between local physics and effects of itinerancy. Despite a large number of candidates identified in the family of materials, an understanding of their physics from competing microscopic energy scales is still missing. We bridge this gap by reporting the first resonant inelastic x-ray scattering (RIXS) measurement on a well-known series of Ru cluster magnets with a -perovskite structure ( ) comprised of Ru dimers. In addition to providing a microscopic explanation for their anomalous magnetic properties, our RIXS measurements combined with theoretical modeling uncover a new regime of molecular orbital physics where the combined effect of large hopping and small spin-orbit coupling results in highly fragile electronic states in the Ru-dimer compounds directly manifested as an abrupt change in the RIXS spectrum accompanying a tiny change in the local structure tuned by the -site ion. This unique combination of energy scales found only in the but not the cluster magnets highlights the value of these materials as a new platform for studying quantum phase transition involving molecular orbitals.}, archive = {J_PRL}, author = {Bo Yuan and Beom Hyun Kim and Qiang Chen and Daniel Dobrowolski and Monika Azmanska and G. M. Luke and Shiyu Fan and Valentina Bisogni and Jonathan Pelliciari and J. P. Clancy}, doi = {10.1103/PhysRevLett.134.106504}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106504}, shortjournal = {Phys. Rev. Lett.}, title = {Exploring a new regime of molecular orbital physics in 4d cluster magnets with resonant inelastic X-ray scattering}, volume = {134}, year = {2025}, }
• (2025). Emergent chiral metal near a kondo breakdown quantum phase transition. PRL, 134(10), 106503. (www)

  @article{ , abstract = {The destruction of the Kondo effect in a local-moment metal can lead to a topological non-Fermi-liquid phase, dubbed fractionalized Fermi liquid, with spinon-type excitations and an emergent gauge field. We demonstrate that, if the latter displays an internal -flux structure, a chiral heavy-fermion metal emerges near the Kondo-breakdown transition. Utilizing a parton mean-field theory describing the transition between a conventional heavy Fermi liquid and a U(1) fractionalized Fermi liquid, we find a novel intermediate phase near the transition whose emergent flux pattern spontaneously breaks both translation and time-reversal symmetries. This phase is an orbital antiferromagnet, and we derive a Landau-type theory which shows that such a phase generically emerges from a -flux spin liquid. We discuss the relevance to pertinent experiments.}, archive = {J_PRL}, author = {Tom Drechsler and Matthias Vojta}, doi = {10.1103/PhysRevLett.134.106503}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106503}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent chiral metal near a kondo breakdown quantum phase transition}, volume = {134}, year = {2025}, }
• (2025). Higher vortexability: Zero-field realization of higher landau levels. PRL, 134(10), 106502. (www)

  @article{ , abstract = {The rise of moiré materials has led to experimental realizations of integer and fractional Chern insulators in small or vanishing magnetic fields. At the same time, a set of minimal conditions sufficient to guarantee an Abelian fractional state in a flat band were identified, namely, “ideal” or “vortexable” quantum geometry. Such vortexable bands share essential features with the lowest Landau level (LL), while excluding the need for more fine-tuned aspects such as flat Berry curvature. A natural and important generalization is to ask if such conditions can be extended to capture the quantum geometry of higher Landau levels, particularly the first LL (1LL), where non-Abelian states at ν = 1 / 2 , 2 / 5 are known to be competitive. The possibility of realizing these states at zero magnetic field, and perhaps even more exotic ones, could become a reality if we could identify the essential structure of the 1LL in Chern bands. In this work, we introduce a precise definition of 1LL quantum geometry, along with a figure of merit that measures how closely a given band approaches the 1LL. Periodically strained Bernal graphene is shown to realize such a 1LL structure even in zero magnetic field.}, archive = {J_PRL}, author = {Manato Fujimoto and Daniel E. Parker and Junkai Dong and Eslam Khalaf and Ashvin Vishwanath and Patrick Ledwith}, doi = {10.1103/PhysRevLett.134.106502}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106502}, shortjournal = {Phys. Rev. Lett.}, title = {Higher vortexability: Zero-field realization of higher landau levels}, volume = {134}, year = {2025}, }
• (2025). Dynamical scaling and planckian dissipation due to heavy-fermion quantum criticality. PRL, 134(10), 106501. (www)

  @article{ , abstract = {We study dynamical scaling associated with a Kondo-breakdown quantum-critical point (KB QCP) of the periodic Anderson model, treated by two-site cellular dynamical mean-field theory (2CDMFT). In the quantum-critical region, the dynamical staggered-spin susceptibility exhibits ω / T scaling. We propose a scaling ansatz that describes this behavior and reveals Planckian dissipation for the longest-lived excitations. The current susceptibility follows the same scaling, leading to strange-metal behavior for the optical conductivity and resistivity. Importantly, this behavior is driven by strong short-ranged vertex contributions, not single-particle decay. This suggests that the KB QCP described by 2CDMFT is a novel intrinsic (i.e., disorder-free) strange-metal fixed point. Our results for the optical conductivity match experimental observations on YbRh 2 Si 2 and CeCoIn 5 .}, archive = {J_PRL}, author = {Andreas Gleis and Seung-Sup B. Lee and Gabriel Kotliar and Jan von Delft}, doi = {10.1103/PhysRevLett.134.106501}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106501}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical scaling and planckian dissipation due to heavy-fermion quantum criticality}, volume = {134}, year = {2025}, }
• (2025). Framework to measure quantum metric from step response. PRL, 134(10), 106403. (www)

  @article{ , abstract = {The quantum metric is known to influence several observables, such as the dielectric constant, superfluid stiffness, and optical mass. However, a direct measurement of the metric has remained elusive. In linear response functions such as electric conductivity, only the matrix elements of the metric appear convoluted with energy prefactors, but to this date no direct observable has been identified that is directly proportional to the integrated metric over the Brillouin zone. In this Letter, we propose relaxation from constrained equilibrium to directly measure the symmetric part of the quantum geometric tensor. This response implements the integral over frequencies appearing in the Souza-Wilkens-Martin sum rule by choosing the electric field appropriately. Our work shines light on other geometric properties of insulators that are absent in the frequency expansions of conductivity in insulators but can, in principle, be revealed in step response.}, archive = {J_PRL}, author = {Nishchhal Verma and Raquel Queiroz}, doi = {10.1103/PhysRevLett.134.106403}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106403}, shortjournal = {Phys. Rev. Lett.}, title = {Framework to measure quantum metric from step response}, volume = {134}, year = {2025}, }
• (2025). Meta-generalized gradient approximation made magnetic. PRL, 134(10), 106402. (www)

  @article{ , abstract = {The Jacob’s ladder of density functional theory (DFT) proposes the compelling view that by extending the form of successful approximations—being guided by exact conditions and selected (least empirical) norms—upper rungs will do better than the lower, thus allowing to balance accuracy and computational effort. Meta-generalized gradient approximations (MGGAs) belong to the last rung of the semilocal approximations before hybridization with nonlocal wave function theories. Among the MGGAs, the strongly constrained and appropriately normed approximation (SCAN) greatly improves upon GGAs from the lower rung. But the over magnetized solutions of SCAN make GGAs more reliable for magnetism. Here, we provide a solution that satisfies the most pressing desiderata for a density functional approximations for ferromagnetic, antiferromagnetic and noncollinear states. The approach is available in an implementation in the crystal electronic structure package.}, archive = {J_PRL}, author = {Jacques K. Desmarais and Alessandro Erba and Giovanni Vignale and Stefano Pittalis}, doi = {10.1103/PhysRevLett.134.106402}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106402}, shortjournal = {Phys. Rev. Lett.}, title = {Meta-generalized gradient approximation made magnetic}, volume = {134}, year = {2025}, }
• (2025). Diverse manifestations of electron-phonon coupling in a kagome superconductor. PRL, 134(10), 106401. (www)

  @article{ , abstract = {Recent angle-resolved photoemission spectroscopy (ARPES) experiments on the kagome metal revealed distinct multimodal dispersion kinks and nodeless superconducting gaps across multiple electron bands. The prominent photoemission kinks suggest a definitive coupling between electrons and certain collective modes, yet the precise nature of this interaction and its connection to superconductivity remain to be established. Here, employing the state-of-the-art ab initio many-body perturbation theory computation, we present direct evidence that electron-phonon ( -ph) coupling induces the multimodal photoemission kinks in , and profoundly, drives the nodeless -wave superconductivity, showcasing the diverse manifestations of the -ph coupling. Our calculations well capture the experimentally measured kinks and their fine structures, and reveal that vibrations from different atomic species dictate the multimodal behavior. Results from anisotropic -Eliashberg equations predict a phonon-mediated superconductivity with nodeless -wave gaps, in excellent agreement with various ARPES and scanning tunneling spectroscopy measurements. Despite the universal origin of the -ph coupling, the contributions of several characteristic phonon vibrations vary in different phenomena, highlighting a versatile role of -ph coupling in shaping the low-energy excitations of kagome metals.}, archive = {J_PRL}, author = {Jing-Yang You and Chih-En Hsu and Mauro Del Ben and Zhenglu Li}, doi = {10.1103/PhysRevLett.134.106401}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106401}, shortjournal = {Phys. Rev. Lett.}, title = {Diverse manifestations of electron-phonon coupling in a kagome superconductor}, volume = {134}, year = {2025}, }
• (2025). Giant gate-controlled odd-parity magnetoresistance in magnetized bilayer graphene at room temperature. PRL, 134(10), 106301. (www)

  @article{ , abstract = {In this Letter, we report the discovery of giant room-temperature odd-parity magnetoresistance (OMR) in a bilayer graphene heterostructure interfaced with (CGT). We show that the OMR is electrostatic gate-voltage tunable, exhibiting maximum value near the graphene band edges and diminishing rapidly with increasing charge carrier density. Our theoretical analysis reveals that the OMR originates from the coupling of out-of-plane components of Berry curvature and orbital magnetic moment with the applied magnetic field, signaling intrinsic time-reversal symmetry breaking in the system. This time-reversal symmetry breaking persists at room temperature within the CGT and bilayer graphene heterostructure despite the bulk CGT exhibiting ferromagnetic transition at 65 K. Our Letter opens new avenues for probing band geometric phenomena through magnetotransport measurements, especially in quantum materials where the anomalous Hall effects are immeasurably small due to the extrinsic scattering-dependent contributions canceling Berry curvature contributions.}, archive = {J_PRL}, author = {Divya Sahani and Sunit Das and Kenji Watanabe and Takashi Taniguchi and Amit Agarwal and Aveek Bid}, doi = {10.1103/PhysRevLett.134.106301}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106301}, shortjournal = {Phys. Rev. Lett.}, title = {Giant gate-controlled odd-parity magnetoresistance in magnetized bilayer graphene at room temperature}, volume = {134}, year = {2025}, }
• (2025). Fermiology and band structure of oxygen-terminated Ti3C2Tx MXene. PRL, 134(10), 106201. (www)

  @article{ , abstract = {The class of two-dimensional carbides and nitrides known as MXenes exhibit remarkable electronic properties. Tailoring these properties, however, requires an in-depth understanding of the band structure and Fermi-surface topology. Surface oxidation of MXenes has previously hampered the characterization of their Fermi surface, which is crucial for understanding the topology and anisotropy in the electronic structure and, ultimately, for tailoring electronic properties. Here, we reveal the Fermi surface topology and band structure of purely oxygen-terminated Ti 3 C 2 T x MXene achieved through rigorous thin film sample preparation and ultrahigh vacuum annealing. Polarized synchrotron radiation-based angle-resolved photoemission spectroscopy reveals electron pockets, bulk band gaps, and a Dirac-like feature in the anisotropic electronic band structure. This paves the way for a fundamental understanding of band engineering of electronic transport properties, providing insights of importance for energy storage devices, transparent conductors, and catalysis.}, archive = {J_PRL}, author = {Martin Magnuson and Per Eklund and Craig Polley}, doi = {10.1103/PhysRevLett.134.106201}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {106201}, shortjournal = {Phys. Rev. Lett.}, title = {Fermiology and band structure of oxygen-terminated Ti3C2Tx MXene}, volume = {134}, year = {2025}, }
• (2025). 3D periodic orbiting of a photothermal bubble. PRL, 134(10), 104004. (www)

  @article{ , abstract = {The spontaneous periodic oscillations of underwater bubbles are typically confined to a 1D direction or within a 2D plane, whereas realizing 3D autonomous motion of bubbles remains challenging. In this Letter, we present experimental observations of a 3D-periodic orbiting bubble, produced by directing a stationary near-infrared laser at hexane, thereby extending the spectrum of multimode motions beyond the 1D and 2D paradigms. Through numerical simulation by carefully investigating both the thermodynamic and hydrodynamic parameters of several liquids, this 3D-orbiting mode is attributed to the subtle interplay between the interfacial flow due to the thermal Marangoni effect and the bulk flow from the thermal buoyancy effect. Moreover, by developing a unified physical model to elucidate the effect of liquid properties on the motion modes, a phase diagram is constructed through a single dimensionless number ( Σ = R e S c / M a ), providing a theoretical guidance to tailor the periodic oscillation modes. These findings not only reveal the underlying intriguing physicochemical hydrodynamics, but also possibly shed light on the bubble-mediated technologies.}, archive = {J_PRL}, author = {Man Hu and Feng Wang and Yuqi Li and Li Chen and Wenna Wu and Peng Huo and Daosheng Deng}, doi = {10.1103/PhysRevLett.134.104004}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {104004}, shortjournal = {Phys. Rev. Lett.}, title = {3D periodic orbiting of a photothermal bubble}, volume = {134}, year = {2025}, }
• (2025). Unifying theory of scaling in drop impact: Forces and maximum spreading diameter. PRL, 134(10), 104003. (www)

  @article{ , abstract = {The dynamics of drop impact on a rigid surface strongly depends on the droplet’s velocity, its size, and its material properties. The main characteristics are the droplet’s force exerted on the surface and its maximal spreading radius. The crucial question is how do they depend on the (dimensionless) control parameters, which are the Weber number W e (nondimensionalized kinetic energy) and the Ohnesorge number O h (dimensionless viscosity). Here, we perform direct numerical simulations over the huge parameter range 1 ≤ W e ≤ 10 3 and 10 − 3 ≤ O h ≤ 10 2 and in particular develop a unifying theoretical approach, which is inspired by the Grossmann-Lohse theory for wall-bounded turbulence [Grossmann and Lohse, J. Fluid Mech. 407 , 27 (2000) ; Phys. Rev. Lett. 86 , 3316 (2001) ]. The key idea is to split the energy dissipation rate into the different phases of the impact process, in which different physical mechanisms dominate. The theory can consistently and quantitatively account for the W e and O h dependences of the maximal impact force and the maximal spreading diameter over the huge parameter space. It also clarifies why viscous dissipation plays a significant role during impact, even for low-viscosity droplets (low O h ), in contrast to what had been assumed in some prior theories.}, archive = {J_PRL}, author = {Vatsal Sanjay and Detlef Lohse}, doi = {10.1103/PhysRevLett.134.104003}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {104003}, shortjournal = {Phys. Rev. Lett.}, title = {Unifying theory of scaling in drop impact: Forces and maximum spreading diameter}, volume = {134}, year = {2025}, }
• (2025). Irreversible charging caused by energy dissipation from depinning of droplets on polymer surfaces. PRL, 134(10), 104002. (www)

  @article{ , abstract = {Interfacial energy dissipation during stick-slip motion of a liquid drop on a nonconductive polymer substrate is shown to lead to an irreversible increase in electrical charge. This previously unobserved phenomenon occurs during surface wetting, in contrast to the previously reported charge separation mechanism that occurs during dewetting. Understanding this electrification mechanism will facilitate the design of energy harvesters and aid the development of risk mitigation strategies for electrostatic buildup in liquid flow across a wide range of industrial applications.}, archive = {J_PRL}, author = {Shuaijia Chen and Ronald T. Leon and Rahmat Qambari and Yan Yan and Menghan Chen and Peter C. Sherrell and Amanda V. Ellis and Joseph D. Berry}, doi = {10.1103/PhysRevLett.134.104002}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {104002}, shortjournal = {Phys. Rev. Lett.}, title = {Irreversible charging caused by energy dissipation from depinning of droplets on polymer surfaces}, volume = {134}, year = {2025}, }
• (2025). Rayleigh-bénard convection with phase change close to the critical point. PRL, 134(10), 104001. (www)

  @article{ , abstract = {Rayleigh-Bénard convection is investigated with sulfur hexafluoride ( S F 6 ) in the vicinity of its critical point. In the supercritical domain, direct measurements of the heat flux 𝑄 as a function of the temperature difference Δ ⁢ 𝑇 are consistent with the usual scaling laws of single-phase turbulent convection. Along the liquid-vapor coexistence curve, heat fluxes are dramatically enhanced by condensation and boiling. Optical measurements are performed to document the size and velocity of the bubbles. We report 𝑄 ⁡ ( Δ ⁢ 𝑇 , 𝜀 ) in both domains, with 𝜀 the dimensionless distance to the critical point. Critical scaling laws are observed that can guide the development of theoretical models. In addition, this documents a system of diverging heat transfer coefficient, i.e., in which a significant heat flux can be achieved with an arbitrarily small temperature difference as 𝜀 → 0 .}, archive = {J_PRL}, author = {Valentin Mouet and Guillaume Michel and François Pétrélis and Stephan Fauve}, doi = {10.1103/PhysRevLett.134.104001}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {104001}, shortjournal = {Phys. Rev. Lett.}, title = {Rayleigh-bénard convection with phase change close to the critical point}, volume = {134}, year = {2025}, }
• (2025). Reconfigurable self-phase modulation enabled by cascaded nonlinear backaction in integrated photonics. PRL, 134(10), 103803. (www)

  @article{ , abstract = {Self-phase modulation is ubiquitous in optical systems: It provides foundational functionality to numerous photonic technologies, such as soliton generation and ultrafast pulse compression. However, it remains challenging to directly modify the coefficient of self-phase modulation, which is typically regarded as a fixed property of optical materials and structures. In this work, we overcome this limitation and demonstrate reconfigurable self-phase modulation with an integrated photonic cavity. This is achieved by introducing the engineered backaction from the reservoir photonic resonance through the cascaded second-order nonlinear coupling. The coefficient of self-phase modulation is tuned from to of its intrinsic value. With negative coefficients, we observe the anomalous self-phase modulation, where photonic resonances are shifted towards higher frequencies. With the reconfigurable self-phase modulation, we further demonstrate the control of spontaneous chiral symmetry breaking in the integrated photonic ring cavity.}, archive = {J_PRL}, author = {Chaohan Cui and Liang Zhang and Linran Fan}, doi = {10.1103/PhysRevLett.134.103803}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {103803}, shortjournal = {Phys. Rev. Lett.}, title = {Reconfigurable self-phase modulation enabled by cascaded nonlinear backaction in integrated photonics}, volume = {134}, year = {2025}, }
• (2025). Exceptional bound states in the continuum. PRL, 134(10), 103802. (www)

  @article{ , abstract = {Bound states in the continuum and exceptional points are unique singularities of non-Hermitian systems. In optical implementations, the former demonstrate strong enhancement of the electromagnetic field, while the latter exhibit high sensitivity to small perturbations. Hence, exceptional points are being actively investigated as next-generation optical sensors. However, at the nanoscale, their performance is strongly constrained by parasitic radiative losses. Here, we show that several bound states in the continuum can be merged into one exceptional point, forming a new kind of singularity. The resulting state inherits properties from both, namely, it does not radiate and shows extremely high sensitivity to perturbations, making it prospective for the realization of exceptional sensing at the nanoscale. We validate our theory with numerical simulations and demonstrate the formation of second- and third-order exceptional bound states in the continuum in stacked dielectric metasurfaces.}, archive = {J_PRL}, author = {Adrià Canós Valero and Zoltan Sztranyovszky and Egor A. Muljarov and Andrey Bogdanov and Thomas Weiss}, doi = {10.1103/PhysRevLett.134.103802}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {103802}, shortjournal = {Phys. Rev. Lett.}, title = {Exceptional bound states in the continuum}, volume = {134}, year = {2025}, }
• (2025). Observation of photonic chiral flatbands. PRL, 134(10), 103801. (www)

  @article{ , abstract = {Distinct selectivity to the spin angular momenta of photons has garnered significant attention in recent years, for its relevance in basic science and for imaging and sensing applications. While nonlocal metasurfaces with strong chiral responses to the incident light have been reported, these responses are typically limited to a narrow range of incident angles. In this study, we demonstrate a nonlocal metasurface that showcases strong chirality, characterized by circular dichroism ( ), over a wide range of incident angles . Its quality factor, circular dichroism and resonant frequency can be optimized by design. These findings pave the way to further advance the development of valley-selective optical cavities and augmented reality applications.}, archive = {J_PRL}, author = {Minho Choi and Andrea Alù and Arka Majumdar}, doi = {10.1103/PhysRevLett.134.103801}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {103801}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of photonic chiral flatbands}, volume = {134}, year = {2025}, }
• (2025). Zero-energy photoelectric effect. PRL, 134(10), 103201. (www)

  @article{ , abstract = {We predict a near-threshold (“zero energy”) peak in multiphoton ionization for a dynamical regime where the photon frequency is large compared to the binding energy of the electron. The peak position does not depend on the laser frequency but on the binding energy and the pulse duration. The effect originates from the fact that bound-continuum dipole transitions are stronger than continuum-continuum ones. To clearly observe this zero-energy photoelectric effect, the spectral width of the laser pulse should be comparable to the binding energy of the ionized orbital, and the second ionization potential should be larger than the photon energy. This suggests negative ions as ideal candidates for corresponding experiments.}, archive = {J_PRL}, author = {Sajad Azizi and Ulf Saalmann and Jan M. Rost}, doi = {10.1103/PhysRevLett.134.103201}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {103201}, shortjournal = {Phys. Rev. Lett.}, title = {Zero-energy photoelectric effect}, volume = {134}, year = {2025}, }
• (2025). Amplified collective auger decay of double inner-shell vacancy in xe. PRL, 134(10), 103001. (www)

  @article{ , abstract = {The collective Auger decay (CAD) of Xe 2 + 4 d − 2 double core-hole states in which two outer-shell electrons fill the double inner-shell vacancies while releasing a third energetic Auger electron is explored using multi-electron-ion coincidence spectroscopy. The CAD branching ratio relative to the total Auger emission of Xe 2 + 4 d − 2 states is estimated to be 2 × 10 − 2 ± 1 × 10 − 2 , surpassing the branching ratios of previously reported CAD paths by a factor of 10 or more. This amplified CAD in Xe 2 + 4 d − 2 states is primarily attributable to their near-degeneracy with intermediate configurations required to promote CAD in second-order perturbation theory. Such near degeneracy is characteristic of all double inner-shell vacancy states in medium and heavy elements, suggesting that CAD paths play a more pivotal role in the relaxation of core-excited matter than is currently understood.}, archive = {J_PRL}, author = {Yasumasa Hikosaka and Stephan Fritzsche}, doi = {10.1103/PhysRevLett.134.103001}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {103001}, shortjournal = {Phys. Rev. Lett.}, title = {Amplified collective auger decay of double inner-shell vacancy in xe}, volume = {134}, year = {2025}, }
• (2025). Observation of the open-charm tetraquark candidate tcs0*(2870)0 in the B−→D−D0KS0 decay. PRL, 134(10), 101901. (www)

  @article{ , abstract = {An amplitude analysis of B − → D − D 0 K S 0 decays is performed using proton-proton collision data, corresponding to an integrated luminosity of 9 fb − 1 , collected with the LHCb detector at center-of-mass energies of 7, 8, and 13 TeV. A resonant structure of spin-parity 0 + is observed in the D 0 K S 0 invariant-mass spectrum with a significance of 5.3 σ . The mass and width of the state, modeled with a Breit-Wigner line shape, are determined to be 2883 ± 11 ± 8 MeV / c 2 and 87 − 47 + 22 ± 17 MeV , respectively, where the first uncertainties are statistical and the second systematic. These properties and the quark content are consistent with those of the open-charm tetraquark candidate T c s 0 * ( 2870 ) 0 observed previously in the D + K − final state of the B − → D − D + K − decay. This result confirms the existence of the T c s 0 * ( 2870 ) 0 state in a new decay mode. The T c s 1 * ( 2900 ) 0 state, reported in the B − → D − D + K − decay, is also searched for in the D 0 K S 0 invariant-mass spectrum of the B − → D − D 0 K S 0 decay, without finding evidence for it.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. C. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and M. Hajheidari and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and B. Urbach and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.101901}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of the open-charm tetraquark candidate tcs0*(2870)0 in the B−→D−D0KS0 decay}, volume = {134}, year = {2025}, }
• (2025). Study of Λb0 and Ξb0 decays to Λh+h′− and evidence for CP violation in Λb0→ΛK+K− decays. PRL, 134(10), 101802. (www)

  @article{ , abstract = {A study of and decays to ( ) is performed using collision data collected by the LHCb experiment during LHC Runs 1–2, corresponding to an integrated luminosity of . The branching fractions for these decays are measured using the decay as a control channel. The decays and are observed for the first time. For decay modes with sufficient signal yields, asymmetries are measured in the full and localized regions of the final-state phase space. Evidence is found for violation in the decay, interpreted as originating primarily from an asymmetric decay amplitude. The measured asymmetries for other decays are compatible with zero.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. C. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and S. Collaviti and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and G. Darze and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and P. Gardner and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and M. Hajheidari and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. H. Harris and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and D. Parmar and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and M. J. Peters and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and I. Segal and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and B. Urbach and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and J. van Eldik and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.101802}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101802}, shortjournal = {Phys. Rev. Lett.}, title = {Study of Λb0 and Ξb0 decays to Λh+h′− and evidence for CP violation in Λb0→ΛK+K− decays}, volume = {134}, year = {2025}, }
• (2025). First evidence for direct CP violation in beauty to charmonium decays. PRL, 134(10), 101801. (www)

  @article{ , abstract = {The asymmetry and branching fraction of the Cabibbo-Kobayashi-Maskawa-suppressed decay are precisely measured relative to the favored decay using a sample of proton-proton collision data corresponding to an integrated luminosity of recorded at a center-of-mass energy of 13 TeV during 2016–2018. The results of the asymmetry difference and branching fraction ratio are , where the first uncertainties are statistical and the second are systematic. A combination with previous LHCb results based on data collected at 7 and 8 TeV in 2011 and 2012 yields and . The combined value deviates from zero by 3.2 standard deviations, providing the first evidence for direct violation in the amplitudes of beauty decays to charmonium final states.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and A. Balboni and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and V. Bellee and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and R. B. Bonacci and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. C. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and M. Firlej and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and T. Fiutowski and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and V. Franco Lima and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and S. Gomez Fernandez and W. Gomulka and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and J. Haimberger and M. Hajheidari and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and D. Hill and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and M. Idzik and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and E. D. Lesser and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and M. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and H. Linton and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and J. Lomba Castro and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and F. M. Manganella and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Gomez and D. Martinez Santos and F. Martinez Vidal and A. Martorell i Granollers and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and E. F. Molina Cardenas and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and J. Moron and W. Morren and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and X. Pan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perrevoort and A. Perro and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and L. Piccolo and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and D. Provenzano and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and A. Rodriguez Alvarez and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and N. S. Sommerfeld and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and K. Swientek and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and Y. Tang and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and B. Urbach and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Verdoglia and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and G. Vouters and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. J. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and M. Winn and W. Wislicki and M. Witek and L. Witola and G. Wormser and S. A. Wotton and H. Wu and J. Wu and X. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and D. Yang and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.101801}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101801}, shortjournal = {Phys. Rev. Lett.}, title = {First evidence for direct CP violation in beauty to charmonium decays}, volume = {134}, year = {2025}, }
• (2025). TT¯-like flows of yang-mills theories. PRL, 134(10), 101603. (www)

  @article{ , abstract = {We study -like deformations of Yang-Mills theories. The standard flows lead to multitrace Lagrangians, and the non-Abelian gauge structures make it challenging to find Lagrangians in a closed form. However, within the geometric approach to , we obtain the closed-form solution to the metric flow and stress-energy tensor, and show that instanton solutions are undeformed. We also introduce new symmetrized single-trace -like deformations, whose solutions in include the non-Abelian Born-Infeld Lagrangian proposed by Tseytlin in 1997.}, archive = {J_PRL}, author = {Christian Ferko and Jue Hou and Tommaso Morone and Gabriele Tartaglino-Mazzucchelli and Roberto Tateo}, doi = {10.1103/PhysRevLett.134.101603}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101603}, shortjournal = {Phys. Rev. Lett.}, title = {TT¯-like flows of yang-mills theories}, volume = {134}, year = {2025}, }
• (2025). Conservative spin-magnitude change in orbital evolution in general relativity. PRL, 134(10), 101602. (www)

  @article{ , abstract = {We show that physical scattering observables for compact spinning objects in general relativity can depend on additional degrees of freedom in the spin tensor beyond those described by the spin vector alone. The impulse, spin kick, and leading-order waveforms exhibit such a nontrivial dependence. A signal of this additional structure is the change in the magnitude of the spin vector under conservative Hamiltonian evolution, similar to our previous studies in electrodynamics. These additional degrees of freedom describe dynamical mass multipoles of compact objects and decouple for black holes. We also show that the conservative impulse, spin kick, and change of the additional degrees of freedom are encoded in the eikonal phase.}, archive = {J_PRL}, author = {Mark Alaverdian and Zvi Bern and Dimitrios Kosmopoulos and Andres Luna and Radu Roiban and Trevor Scheopner and Fei Teng}, doi = {10.1103/PhysRevLett.134.101602}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101602}, shortjournal = {Phys. Rev. Lett.}, title = {Conservative spin-magnitude change in orbital evolution in general relativity}, volume = {134}, year = {2025}, }
• (2025). T duality and TT¯-like deformations of sigma models. PRL, 134(10), 101601. (www)

  @article{ , abstract = {We initiate the study of the interplay between T duality and classical stress tensor deformations in two-dimensional sigma models. We first show that a general Abelian T duality commutes with the T T ¯ deformation, which can be engineered by a gravitational dressing. Then, by using an auxiliary field formulation of stress tensor deformations of the principal chiral model (PCM), we prove that non-Abelian T duality and arbitrary T T ¯ -like flows also commute for theories in this class. We argue that all such auxiliary field deformations of both the PCM and its T dual are classically integrable.}, archive = {J_PRL}, author = {Daniele Bielli and Christian Ferko and Liam Smith and Gabriele Tartaglino-Mazzucchelli}, doi = {10.1103/PhysRevLett.134.101601}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101601}, shortjournal = {Phys. Rev. Lett.}, title = {T duality and TT¯-like deformations of sigma models}, volume = {134}, year = {2025}, }
• (2025). Black hole singularity resolution in unimodular gravity from unitarity. PRL, 134(10), 101501. (www)

  @article{ , abstract = {We study the quantum dynamics of an interior planar anti–de Sitter black hole, requiring unitarity in the natural time coordinate conjugate to the cosmological “constant of motion” appearing in unimodular gravity. Both the classical singularity and the horizon are replaced by a nonsingular highly quantum region; semiclassical notions of spacetime evolution are only valid in an intermediate region. For the singularity, our results should be applicable to general black holes: unitarity in unimodular time always implies singularity resolution.}, archive = {J_PRL}, author = {Steffen Gielen and Lucía Menéndez-Pidal}, doi = {10.1103/PhysRevLett.134.101501}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101501}, shortjournal = {Phys. Rev. Lett.}, title = {Black hole singularity resolution in unimodular gravity from unitarity}, volume = {134}, year = {2025}, }
• (2025). Stochastic dark matter from curvature perturbations. PRL, 134(10), 101005. (www)

  @article{ , abstract = {We investigate the production of dark matter from metric perturbations produced during inflation or in standard cosmology. Perturbations break Weyl flatness of the Friedmann-Lemaître-Robertson-Walker metric, allowing conformally coupled fields—in particular, fermions studied here—to be produced even when their mass is negligible. Particle production can be computed by studying the Bogoliubov transformation induced by the stochastic background. For perturbations generated during inflation, we present a closed formula for the resulting abundance of particles that depends solely on the power spectrum of curvature perturbations at the end of inflation. This production mechanism can be dominant especially if the amplitude of curvature perturbations is enhanced for modes that exit the horizon toward the end of inflation. In the simplest scenario, the critical dark matter abundance is reproduced for .}, archive = {J_PRL}, author = {Raghuveer Garani and Michele Redi and Andrea Tesi}, doi = {10.1103/PhysRevLett.134.101005}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101005}, shortjournal = {Phys. Rev. Lett.}, title = {Stochastic dark matter from curvature perturbations}, volume = {134}, year = {2025}, }
• (2025). Cosmological spatial curvature with the alcock-paczyński effect. PRL, 134(10), 101004. (www)

  @article{ , abstract = {We propose a methodology to measure the cosmological spatial curvature by employing the deviation from statistical isotropy due to the Alcock-Paczyński effect of large scale galaxy clustering. This approach has a higher degree of model independence than most other proposed methods, being independent of the calibration of standard candles, rulers, or clocks, of the power spectrum shape (and thus also of the prerecombination physics), of the galaxy bias, of the theory of gravity, of the dark energy model, and of the background cosmology in general. We find that a combined Dark Energy Spectroscopic Instrument-Euclid galaxy survey can achieve at in the redshift range by combining power-spectrum and bispectrum measurements.}, archive = {J_PRL}, author = {Luca Amendola and Marco Marinucci and Miguel Quartin}, doi = {10.1103/PhysRevLett.134.101004}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101004}, shortjournal = {Phys. Rev. Lett.}, title = {Cosmological spatial curvature with the alcock-paczyński effect}, volume = {134}, year = {2025}, }
• (2025). Primordial neutrinos and new physics: Novel approach to solving the neutrino boltzmann equation. PRL, 134(10), 101003. (www)

  @article{ , abstract = {Understanding how new physics influences the dynamics of cosmic neutrinos during their decoupling is crucial in light of upcoming precise cosmological observations and the need to reconcile cosmological and laboratory probes. Existing approaches to solving the neutrino Boltzmann equation are often model dependent, computationally inefficient, and yield contradictory results. To solve this problem, we introduce a novel method to comprehensively study neutrino dynamics. We apply this method to several case studies, resolving the discrepancy in the literature about the impact of nonthermal neutrinos on and providing important insights about the role of decaying new physics particles on MeV plasma.}, archive = {J_PRL}, author = {Maksym Ovchynnikov and Vsevolod Syvolap}, doi = {10.1103/PhysRevLett.134.101003}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101003}, shortjournal = {Phys. Rev. Lett.}, title = {Primordial neutrinos and new physics: Novel approach to solving the neutrino boltzmann equation}, volume = {134}, year = {2025}, }
• (2025). New method to determine the hubble parameter from cosmological energy-density measurements. PRL, 134(10), 101002. (www)

  @article{ , abstract = {We introduce a new method for measuring the Hubble parameter from low-redshift large-scale observations that is independent of the comoving sound horizon. The method uses the baryon-to-photon ratio determined by the primordial deuterium abundance, together with big bang nucleosynthesis calculations and the present-day cosmic microwave background (CMB) temperature, to determine the physical baryon density . The baryon fraction is measured using the relative amplitude of the baryonic signature in galaxy clustering measured by the Baryon Oscillation Spectroscopic Survey, scaling the physical baryon density to the physical matter density. The physical density is then compared with the geometrical density from Alcock-Paczynski measurements from baryon acoustic oscillations (BAO) and voids to give . Including type Ia supernovae and uncalibrated BAO, we measure . We find similar results when varying analysis choices, such as measuring the baryon signature from the reconstructed correlation function or excluding supernovae or voids. This measurement is currently consistent with both the distance-ladder and CMB determinations, but near-future large-scale structure surveys will obtain to tighter constraints.}, archive = {J_PRL}, author = {Alex Krolewski and Will J. Percival and Alex Woodfinden}, doi = {10.1103/PhysRevLett.134.101002}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101002}, shortjournal = {Phys. Rev. Lett.}, title = {New method to determine the hubble parameter from cosmological energy-density measurements}, volume = {134}, year = {2025}, }
• (2025). Anomalous ionization in the central molecular zone by sub-GeV dark matter. PRL, 134(10), 101001. (www)

  @article{ , abstract = {We demonstrate that the anomalous ionization rate observed in the Central Molecular Zone can be attributed to MeV dark matter annihilations into e + e − pairs for galactic dark matter profiles with slopes γ > 1 . The low annihilation cross sections required avoid cosmological constraints and imply no detectable inverse Compton, bremsstrahlung, or synchrotron emission in radio, x- and γ rays. The possible connection with the source of the unexplained 511 keV line emission in the Galactic Center suggests that both observations could be correlated and have a common origin.}, archive = {J_PRL}, author = {Pedro De la Torre Luque and Shyam Balaji and Joseph Silk}, doi = {10.1103/PhysRevLett.134.101001}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {101001}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous ionization in the central molecular zone by sub-GeV dark matter}, volume = {134}, year = {2025}, }
• (2025). Linear-optical quantum computation with arbitrary error-correcting codes. PRL, 134(10), 100602. (www)

  @article{ , abstract = {High-rate quantum error-correcting codes mitigate the imposing scale of fault-tolerant quantum computers but require efficient generation of nonlocal, many-body entanglement. We provide a linear-optical architecture with these properties, compatible with arbitrary codes and Gottesman-Kitaev-Preskill qubits on generic lattices, and featuring a natural way to leverage physical noise bias. Simulations of hyperbolic surface codes and bivariate bicycle codes, promising families of quantum low-density parity-check codes, reveal a threshold comparable to the 2D surface code with substantially better encoding rates.}, archive = {J_PRL}, author = {Blayney W. Walshe and Ben Q. Baragiola and Hugo Ferretti and José Gefaell and Michael Vasmer and Ryohei Weil and Takaya Matsuura and Thomas Jaeken and Giacomo Pantaleoni and Zhihua Han and Timo Hillmann and Nicolas C. Menicucci and Ilan Tzitrin and Rafael N. Alexander}, doi = {10.1103/PhysRevLett.134.100602}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {100602}, shortjournal = {Phys. Rev. Lett.}, title = {Linear-optical quantum computation with arbitrary error-correcting codes}, volume = {134}, year = {2025}, }
• (2025). Benchmarking the readout of a superconducting qubit for repeated measurements. PRL, 134(10), 100601. (www)

  @article{ , abstract = {Readout of superconducting qubits faces a trade-off between measurement speed and unwanted backaction on the qubit caused by the readout drive, such as degradation and leakage out of the computational subspace. The readout is typically benchmarked by integrating the readout signal and choosing a binary threshold to extract the “readout fidelity.” We show that readout fidelity may significantly overlook readout-induced leakage errors. Such errors are detrimental for applications that rely on continuously repeated measurements, e.g., quantum error correction. We introduce a method to measure the readout-induced leakage rate by repeatedly executing a composite operation—a readout preceded by a randomized qubit flip. We apply this technique to characterize the readout of a superconducting qubit, optimized for fidelity across four different readout durations. Our technique highlights the importance of an independent leakage characterization by showing that the leakage rates vary from 0.12% to 7.76% across these readouts even though the fidelity exceeds 99.5% in all four cases.}, archive = {J_PRL}, author = {S. Hazra and W. Dai and T. Connolly and P. D. Kurilovich and Z. Wang and L. Frunzio and M. H. Devoret}, doi = {10.1103/PhysRevLett.134.100601}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {100601}, shortjournal = {Phys. Rev. Lett.}, title = {Benchmarking the readout of a superconducting qubit for repeated measurements}, volume = {134}, year = {2025}, }
• (2025). Optimally fast qubit reset. PRL, 134(10), 100401. (www)

  @article{ , abstract = {In practice, qubit reset must be operated in an extremely short time, which incurs a thermodynamic cost within multiple orders of magnitude above the Landauer bound. We present a general framework to determine the minimal thermodynamic cost and the corresponding optimal protocol for memory erasure under arbitrary erasure speeds. Our study reveals the divergent behavior of minimal entropy production in the short-time limit depends on the convergence and divergence of the jump operator. There is an inherent trade-off between the minimal required time and the set error probability for the convergent class. Moreover, we find the optimal protocol exhibits general features in the fast-driving regime. To illustrate these findings, we employ fermionic and bosonic baths as examples. Our results suggest that the super-Ohmic bosonic heat bath is suitable for qubit reset.}, archive = {J_PRL}, author = {Yue Liu and Chenlong Huang and Xingyu Zhang and Dahai He}, doi = {10.1103/PhysRevLett.134.100401}, journal = {Physical Review Letters}, month = {3}, number = {10}, pages = {100401}, shortjournal = {Phys. Rev. Lett.}, title = {Optimally fast qubit reset}, volume = {134}, year = {2025}, }
• (2025). Erratum: Centrality-dependent modification of jet-production rates in deuteron-gold collisions at sNN=200 GeV [Phys. rev. lett. 116, 122301 (2016)]. PRL, 134(9), 099901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 099901 (2025)}, archive = {J_PRL}, author = {PHENIX Collaboration and A. Adare and C. Aidala and N. N. Ajitanand and Y. Akiba and H. Al-Bataineh and J. Alexander and M. Alfred and A. Angerami and K. Aoki and N. Apadula and Y. Aramaki and H. Asano and E. T. Atomssa and R. Averbeck and T. C. Awes and B. Azmoun and V. Babintsev and M. Bai and G. Baksay and L. Baksay and N. S. Bandara and B. Bannier and K. N. Barish and B. Bassalleck and A. T. Basye and S. Bathe and V. Baublis and C. Baumann and A. Bazilevsky and M. Beaumier and S. Beckman and S. Belikov and R. Belmont and R. Bennett and A. Berdnikov and Y. Berdnikov and J. H. Bhom and D. S. Blau and J. S. Bok and K. Boyle and M. L. Brooks and J. Bryslawskyj and H. Buesching and V. Bumazhnov and G. Bunce and S. Butsyk and S. Campbell and A. Caringi and C.-H. Chen and C. Y. Chi and M. Chiu and I. J. Choi and J. B. Choi and R. K. Choudhury and P. Christiansen and T. Chujo and P. Chung and O. Chvala and V. Cianciolo and Z. Citron and B. A. Cole and Z. Conesa del Valle and M. Connors and M. Csanád and T. Csörgő and T. Dahms and S. Dairaku and I. Danchev and T. W. Danley and K. Das and A. Datta and M. S. Daugherity and G. David and M. K. Dayananda and K. DeBlasio and K. Dehmelt and A. Denisov and A. Deshpande and E. J. Desmond and K. V. Dharmawardane and O. Dietzsch and A. Dion and P. B. Diss and J. H. Do and M. Donadelli and L. D’Orazio and O. Drapier and A. Drees and K. A. Drees and J. M. Durham and A. Durum and D. Dutta and S. Edwards and Y. V. Efremenko and F. Ellinghaus and T. Engelmore and A. Enokizono and H. En’yo and S. Esumi and B. Fadem and N. Feege and D. E. Fields and M. Finger and M. Finger, Jr and F. Fleuret and S. L. Fokin and Z. Fraenkel and J. E. Frantz and A. Franz and A. D. Frawley and K. Fujiwara and Y. Fukao and T. Fusayasu and C. Gal and P. Gallus and P. Garg and I. Garishvili and H. Ge and F. Giordano and A. Glenn and H. Gong and M. Gonin and Y. Goto and R. Granier de Cassagnac and N. Grau and S. V. Greene and G. Grim and M. Grosse Perdekamp and T. Gunji and H.-Å. Gustafsson and T. Hachiya and J. S. Haggerty and K. I. Hahn and H. Hamagaki and J. Hamblen and H. F. Hamilton and R. Han and S. Y. Han and J. Hanks and S. Hasegawa and T. O. S. Haseler and K. Hashimoto and E. Haslum and R. Hayano and X. He and M. Heffner and T. K. Hemmick and T. Hester and J. C. Hill and M. Hohlmann and R. S. Hollis and W. Holzmann and K. Homma and B. Hong and T. Horaguchi and D. Hornback and T. Hoshino and N. Hotvedt and J. Huang and S. Huang and T. Ichihara and R. Ichimiya and Y. Ikeda and K. Imai and M. Inaba and A. Iordanova and D. Isenhower and M. Ishihara and M. Issah and D. Ivanishchev and Y. Iwanaga and B. V. Jacak and M. Jezghani and J. Jia and X. Jiang and J. Jin and B. M. Johnson and T. Jones and K. S. Joo and D. Jouan and D. S. Jumper and F. Kajihara and J. Kamin and S. Kanda and J. H. Kang and J. Kapustinsky and K. Karatsu and M. Kasai and D. Kawall and M. Kawashima and A. V. Kazantsev and T. Kempel and J. A. Key and V. Khachatryan and A. Khanzadeev and K. M. Kijima and J. Kikuchi and A. Kim and B. I. Kim and C. Kim and D. J. Kim and E.-J. Kim and G. W. Kim and M. Kim and Y.-J. Kim and B. Kimelman and E. Kinney and Á. Kiss and E. Kistenev and R. Kitamura and J. Klatsky and D. Kleinjan and P. Kline and T. Koblesky and L. Kochenda and B. Komkov and M. Konno and J. Koster and D. Kotov and A. Král and A. Kravitz and G. J. Kunde and K. Kurita and M. Kurosawa and Y. Kwon and G. S. Kyle and R. Lacey and Y. S. Lai and J. G. Lajoie and A. Lebedev and D. M. Lee and J. Lee and K. B. Lee and K. S. Lee and S. Lee and S. H. Lee and M. J. Leitch and M. A. L. Leite and X. Li and P. Lichtenwalner and P. Liebing and S. H. Lim and L. A. Linden Levy and T. Liška and H. Liu and M. X. Liu and B. Love and D. Lynch and C. F. Maguire and Y. I. Makdisi and M. Makek and M. D. Malik and A. Manion and V. I. Manko and E. Mannel and Y. Mao and H. Masui and F. Matathias and M. McCumber and P. L. McGaughey and D. McGlinchey and C. McKinney and N. Means and A. Meles and M. Mendoza and B. Meredith and Y. Miake and T. Mibe and A. C. Mignerey and K. Miki and A. Milov and D. K. Mishra and J. T. Mitchell and S. Miyasaka and S. Mizuno and A. K. Mohanty and P. Montuenga and H. J. Moon and T. Moon and Y. Morino and A. Morreale and D. P. Morrison and T. V. Moukhanova and T. Murakami and J. Murata and A. Mwai and S. Nagamiya and K. Nagashima and J. L. Nagle and M. Naglis and M. I. Nagy and I. Nakagawa and H. Nakagomi and Y. Nakamiya and K. R. Nakamura and T. Nakamura and K. Nakano and S. Nam and C. Nattrass and P. K. Netrakanti and J. Newby and M. Nguyen and M. Nihashi and T. Niida and S. Nishimura and R. Nouicer and T. Novák and N. Novitzky and A. S. Nyanin and C. Oakley and E. O’Brien and S. X. Oda and C. A. Ogilvie and M. Oka and K. Okada and Y. Onuki and J. D. Orjuela Koop and J. D. Osborn and A. Oskarsson and M. Ouchida and K. Ozawa and R. Pak and V. Pantuev and V. Papavassiliou and I. H. Park and J. S. Park and S. Park and S. K. Park and W. J. Park and S. F. Pate and M. Patel and H. Pei and J.-C. Peng and H. Pereira and D. V. Perepelitsa and G. D. N. Perera and D. Yu. Peressounko and J. Perry and R. Petti and C. Pinkenburg and R. Pinson and R. P. Pisani and M. Proissl and M. L. Purschke and H. Qu and J. Rak and B. J. Ramson and I. Ravinovich and K. F. Read and S. Rembeczki and K. Reygers and D. Reynolds and V. Riabov and Y. Riabov and E. Richardson and T. Rinn and D. Roach and G. Roche and S. D. Rolnick and M. Rosati and C. A. Rosen and S. S. E. Rosendahl and Z. Rowan and J. G. Rubin and P. Ružička and B. Sahlmueller and N. Saito and T. Sakaguchi and K. Sakashita and H. Sako and V. Samsonov and S. Sano and M. Sarsour and S. Sato and T. Sato and S. Sawada and B. Schaefer and B. K. Schmoll and K. Sedgwick and J. Seele and R. Seidl and A. Sen and R. Seto and P. Sett and A. Sexton and D. Sharma and I. Shein and T.-A. Shibata and K. Shigaki and M. Shimomura and K. Shoji and P. Shukla and A. Sickles and C. L. Silva and D. Silvermyr and C. Silvestre and K. S. Sim and B. K. Singh and C. P. Singh and V. Singh and M. Slunečka and M. Snowball and R. A. Soltz and W. E. Sondheim and S. P. Sorensen and I. V. Sourikova and P. W. Stankus and E. Stenlund and M. Stepanov and S. P. Stoll and T. Sugitate and A. Sukhanov and T. Sumita and J. Sun and J. Sziklai and E. M. Takagui and A. Taketani and R. Tanabe and Y. Tanaka and S. Taneja and K. Tanida and M. J. Tannenbaum and S. Tarafdar and A. Taranenko and H. Themann and D. Thomas and T. L. Thomas and R. Tieulent and A. Timilsina and T. Todoroki and M. Togawa and A. Toia and L. Tomášek and M. Tomášek and H. Torii and C. L. Towell and R. Towell and R. S. Towell and I. Tserruya and Y. Tsuchimoto and C. Vale and H. Valle and H. W. van Hecke and E. Vazquez-Zambrano and A. Veicht and J. Velkovska and R. Vértesi and M. Virius and V. Vrba and E. Vznuzdaev and X. R. Wang and D. Watanabe and K. Watanabe and Y. Watanabe and Y. S. Watanabe and F. Wei and R. Wei and J. Wessels and A. S. White and S. N. White and D. Winter and C. L. Woody and R. M. Wright and M. Wysocki and B. Xia and L. Xue and S. Yalcin and Y. L. Yamaguchi and K. Yamaura and R. Yang and A. Yanovich and J. Ying and S. Yokkaichi and J. H. Yoo and I. Yoon and Z. You and G. R. Young and I. Younus and H. Yu and I. E. Yushmanov and W. A. Zajc and A. Zelenski and S. Zhou and L. Zou}, doi = {10.1103/PhysRevLett.134.099901}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {099901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Centrality-dependent modification of jet-production rates in deuteron-gold collisions at sNN=200 GeV [Phys. rev. lett. 116, 122301 (2016)]}, volume = {134}, year = {2025}, }
• (2025). Xu et al. reply: . PRL, 134(9), 099302. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 099302 (2025)}, archive = {J_PRL}, author = {Shupeng Xu and Yuhui Wang and Ritesh Agarwal}, doi = {10.1103/PhysRevLett.134.099302}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {099302}, shortjournal = {Phys. Rev. Lett.}, title = {Xu et al. reply: }, volume = {134}, year = {2025}, }
• (2025). Comment on “Absence of topological protection of the interface states in z2 photonic crystals”. PRL, 134(9), 099301. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 099301 (2025)}, archive = {J_PRL}, author = {Xing-Xiang Wang and Toshikaze Kariyado and Xiao Hu}, doi = {10.1103/PhysRevLett.134.099301}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {099301}, shortjournal = {Phys. Rev. Lett.}, title = {Comment on “Absence of topological protection of the interface states in z2 photonic crystals”}, volume = {134}, year = {2025}, }
• (2025). Hotter is not faster for a melting RNA hairpin. PRL, 134(9), 098401. (www)

  @article{ , abstract = {We investigate the denaturation dynamics of nucleic acids through extensive molecular dynamics simulations of a coarse-grained RNA hairpin model. In apparent contradiction to Arrhenius’ law, our findings reveal that the denaturation time of RNA hairpins is a nonmonotonous function of temperature for molecules longer than few persistence lengths, with an optimal temperature above the melting point, T m , at which denaturation occurs fastest. This anomaly arises from the existence of two distinct pathways: “unidirectional” unzipping, progressing from one end to the other and favored near T m , and “bidirectional” denaturation, where competing unzipping events initiate from both ends at higher temperatures. The two regimes manifest distinct scaling laws for the melting time vs length, L , and are separated by a crossover temperature T × , with ( T × − T m ) ∼ L − 1 . The results highlight the significant role of the helical structure in the out-of-equilibrium dynamics of RNA and DNA denaturation and unveil multiple surprises in a decades-old problem.}, archive = {J_PRL}, author = {Huaping Li and E. M. Bahçeci and M. Sayar and A. Kabakç𝚤oğlu}, doi = {10.1103/PhysRevLett.134.098401}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {098401}, shortjournal = {Phys. Rev. Lett.}, title = {Hotter is not faster for a melting RNA hairpin}, volume = {134}, year = {2025}, }
• (2025). Activity-driven emulsification of phase-separating binary mixtures. PRL, 134(9), 098301. (www)

  @article{ , abstract = {Active particles self-assemble into emergent structures that respond sensitively to external constraints. Consequently, their behavior under confinement is complex, especially in soft confined media, leading to diverse emergent morphologies. Through computer simulations, we investigate the dynamical interplay between active Brownian particles and a binary mixture. Our results show that active particles stabilize nonequilibrium morphologies, arresting coarsening by exerting active pressure that competes with surface tension. For moderate activities, particles stabilize an active emulsion with a well-defined droplet size. At higher activities, when particles can cross the liquid domains, a dynamic emulsion with large droplet dispersion is sustained. Furthermore, active particles drive phase-separated mixtures away from equilibrium configurations, demonstrating a rich coassembly behavior due to competing energy scales in the system.}, archive = {J_PRL}, author = {Javier Díaz and Ignacio Pagonabarraga}, doi = {10.1103/PhysRevLett.134.098301}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {098301}, shortjournal = {Phys. Rev. Lett.}, title = {Activity-driven emulsification of phase-separating binary mixtures}, volume = {134}, year = {2025}, }
• (2025). Mechanistic picture for the slow arrhenius process in glass forming systems: The collective small displacements model. PRL, 134(9), 098203. (www)

  @article{ , abstract = {Recent experiments reveal increasing detail about the so-called slow Arrhenius process (SAP), which leads to molecular relaxation in glassy systems. The SAP operates over a temperature range that spans melt and glassy states and acts alongside the familiar α -relaxation. In this Letter, we propose a mechanistic picture for SAP relaxation wherein local amorphous packing is reshaped by molecular movements that are small in comparison to those in the α -modes. Our approach, the collective small displacements (CSD) model, captures a number of experimentally observed SAP characteristics, including its connection to rheology and shear flow. Using a statistical mechanics-based equation of state to obtain nonbonded segmental interaction energies, the CSD model predicts the SAP’s activation energies a priori , based solely on thermodynamic analysis of material properties. The other parameters are all shown to be reasonably material-independent, which means that the model is able to predict SAP relaxation rates and SAP-driven equilibration rates (e.g., adsorption) without using any data on the SAP at all.}, archive = {J_PRL}, author = {Ronald P. White and Simone Napolitano and Jane E. G. Lipson}, doi = {10.1103/PhysRevLett.134.098203}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {098203}, shortjournal = {Phys. Rev. Lett.}, title = {Mechanistic picture for the slow arrhenius process in glass forming systems: The collective small displacements model}, volume = {134}, year = {2025}, }
• (2025). Crack propagation by activated avalanches during creep and fatigue from elastic interface theory. PRL, 134(9), 098202. (www)

  @article{ , abstract = {The growth of cracks combines materials science, fracture mechanics, and statistical physics. The importance of fluctuations in the crack velocity is fundamental since it signals that the crack overcomes local barriers such as tough spots by avalanches. In ductile materials the omnipresent plasticity close to the crack tip influences the growth by history effects, which we here study in polymethylmetacrylate by various fatigue and creep protocols. We show how the crack tip local history may be encompassed in a time- and protocol-dependent length scale, which allows us to apply a statistical fracture description to the time-dependent crack growth rate, resolving the well-known paradox why fatigue cracks grow faster if the stress during a cycle is let to relax more from the peak value. The results open up novel directions for understanding fracture by statistical physics.}, archive = {J_PRL}, author = {Tero Mäkinen and Lumi Tuokkola and Joonas Lahikainen and Ivan V. Lomakin and Juha Koivisto and Mikko J. Alava}, doi = {10.1103/PhysRevLett.134.098202}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {098202}, shortjournal = {Phys. Rev. Lett.}, title = {Crack propagation by activated avalanches during creep and fatigue from elastic interface theory}, volume = {134}, year = {2025}, }
• (2025). Diffusioosmotic reversal of colloidal focusing direction in a microfluidic T-junction. PRL, 134(9), 098201. (www)

  @article{ , abstract = {Solute gradients next to an interface drive a diffusioosmotic flow, the origin of which lies in the intermolecular interactions between the solute and the interface. These flows on the surface of colloids introduce an effective slip velocity, driving their diffusiophoretic migration. In confined environments, the interplay between diffusiophoresis and diffusioosmosis governs the motion of colloids. Previous studies have indeed demonstrated the quantitative modulation of phoretic migration by the osmotic flows. Here, we show that diffusioosmotic flows can lead to qualitatively distinct outcomes, reversing the direction of colloidal focusing expected from diffusiophoresis alone. Using microfluidic experiments in a T-junction, numerical simulations, and theoretical modeling, we explain our observations to be due to an interplay between diffusiophoretic migration of colloids toward the walls and their entrainment in a diffusioosmotic vortex. We show this focusing to be persistent for a range of salt types, salt gradients, and flow rates, and establish a criterion for its emergence. Our work sheds light on how boundaries modulate the solute-mediated transport of colloids in confined environments and how the colloidal trajectories can be utilized to infer the surface properties.}, archive = {J_PRL}, author = {Haoyu Liu and Amir A. Pahlavan}, doi = {10.1103/PhysRevLett.134.098201}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {098201}, shortjournal = {Phys. Rev. Lett.}, title = {Diffusioosmotic reversal of colloidal focusing direction in a microfluidic T-junction}, volume = {134}, year = {2025}, }
• (2025). Mesoscopic dynamics in molecular liquids: Universality of nondispersive structural mode and its reflection in self-atomic motions. PRL, 134(9), 098001. (www)

  @article{ , abstract = {Neutron spin echo experiments on deuterated and protonated molecular liquids with different interactions have revealed their coherent and incoherent scattering functions at the mesoscale. The coherent one decays by a nondiffusive exponential relaxation process that can be related to stress fluctuations. For self-dynamics, we show that even though diffusion is, as expected, the predominant relaxation channel at the mesoscale, the process observed for collective dynamics also appears at short times, evidencing the influence of stress fluctuations on translational motions even at high temperatures.}, archive = {J_PRL}, author = {Arantxa Arbe and Silvia Arrese-Igor and María Dolores Ruiz-Martín and Bela Farago and Fernando Alvarez and Gøran J. Nilsen and Juan Colmenero}, doi = {10.1103/PhysRevLett.134.098001}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {098001}, shortjournal = {Phys. Rev. Lett.}, title = {Mesoscopic dynamics in molecular liquids: Universality of nondispersive structural mode and its reflection in self-atomic motions}, volume = {134}, year = {2025}, }
• (2025). Flux hypothesis for odd transport phenomena. PRL, 134(9), 097105. (www)

  @article{ , abstract = {Onsager’s regression hypothesis makes a fundamental connection between macroscopic transport phenomena and the average relaxation of spontaneous microscopic fluctuations. This relaxation, however, is agnostic to odd transport phenomena, in which fluxes run orthogonal to the gradients driving them. To account for odd transport, we generalize the regression hypothesis, postulating that macroscopic linear constitutive laws are, on average, obeyed by microscopic fluctuations, whether they contribute to relaxation or not. From this “flux hypothesis,” Green-Kubo and reciprocal relations follow, elucidating the separate roles of broken time-reversal and parity symmetries underlying various odd transport coefficients. As an application, we derive and verify the Green-Kubo relation for odd collective diffusion in chiral active matter, first in an analytically tractable model and subsequently through molecular dynamics simulations of concentrated active spinners.}, archive = {J_PRL}, author = {Cory Hargus and Alhad Deshpande and Ahmad K. Omar and Kranthi K. Mandadapu}, doi = {10.1103/PhysRevLett.134.097105}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {097105}, shortjournal = {Phys. Rev. Lett.}, title = {Flux hypothesis for odd transport phenomena}, volume = {134}, year = {2025}, }
• (2025). Partial yet definite emergence of the kardar-parisi-zhang class in isotropic spin chains. PRL, 134(9), 097104. (www)

  @article{ , abstract = {Integrable spin chains with a continuous non-Abelian symmetry, such as the one-dimensional isotropic Heisenberg model, show superdiffusive transport with little theoretical understanding. Although recent studies reported a surprising connection to the Kardar-Parisi-Zhang (KPZ) universality class in that case, this view was most recently questioned by discrepancies in full counting statistics. Here, by combining extensive numerical simulations of classical and quantum integrable isotropic spin chains with a framework developed by exact studies of the KPZ class, we characterize various two-point quantities that remain hitherto unexplored in spin chains, and find full agreement with KPZ scaling laws without adjustable parameters. This establishes the partial emergence of the KPZ class in integrable isotropic spin chains. Moreover, we reveal that the KPZ scaling laws are intact in the presence of an energy current, under the appropriate Galilean boost required by the propagation of spacetime correlation.}, archive = {J_PRL}, author = {Kazumasa A. Takeuchi and Kazuaki Takasan and Ofer Busani and Patrik L. Ferrari and Romain Vasseur and Jacopo De Nardis}, doi = {10.1103/PhysRevLett.134.097104}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {097104}, shortjournal = {Phys. Rev. Lett.}, title = {Partial yet definite emergence of the kardar-parisi-zhang class in isotropic spin chains}, volume = {134}, year = {2025}, }
• (2025). Classical origins of landau-incompatible transitions. PRL, 134(9), 097103. (www)

  @article{ , abstract = {Continuous phase transitions where symmetry is spontaneously broken are ubiquitous in physics and often found between “Landau-compatible” phases where residual symmetries of one phase are a subset of the other. However, continuous “deconfined quantum critical” transitions between Landau-incompatible symmetry-breaking phases are known to exist in certain quantum systems, often with anomalous microscopic symmetries. In this Letter, we investigate the need for such special conditions. We show that Landau-incompatible transitions can be found in a family of well-known classical statistical mechanical models with anomaly-free symmetries, introduced by José et al. [ Phys. Rev. B 16 , 1217 (1977) .]. The models are anisotropic deformations of the classical 2D XY model labeled by a positive integer Q . For a range of temperatures, even Q models exhibit two Landau-incompatible partial symmetry-breaking phases and a direct transition between them for Q ≥ 4 . Characteristic features of deconfined quantum criticality, such as enhanced symmetries and melting of charged defects, are easily seen in a classical setting. For odd Q and corresponding temperature ranges, two regions of a single partial symmetry-breaking phase appear, split by a stable “unnecessary critical” line. We discuss experimental systems that realize these transitions and present anomaly-free quantum models that also exhibit similar phase diagrams.}, archive = {J_PRL}, author = {Abhishodh Prakash and Nick G. Jones}, doi = {10.1103/PhysRevLett.134.097103}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {097103}, shortjournal = {Phys. Rev. Lett.}, title = {Classical origins of landau-incompatible transitions}, volume = {134}, year = {2025}, }
• (2025). Effective grand canonical description of condensation in negative-temperature regimes. PRL, 134(9), 097102. (www)

  @article{ , abstract = {The observation of negative-temperature states in the localized phase of the discrete nonlinear Schrödinger equation has challenged statistical mechanics for a long time. For isolated systems, they can emerge as stationary extended states through a large-deviation mechanism occurring for finite sizes, while they are formally unstable in grand canonical setups, being associated to an unlimited growth of the condensed fraction. Here, we show that negative-temperature states in open setups are metastable and their lifetime is exponentially long with the temperature, (for ). A general expression for is obtained in the case of a simplified stochastic model of noninteracting particles. In the discrete nonlinear Schrödinger model, the presence of an adiabatic invariant makes even larger because of the resulting freezing of the breather dynamics. This mechanism, based on the existence of two conservation laws, provides a new perspective over the statistical description of condensation processes.}, archive = {J_PRL}, author = {Stefano Iubini and Antonio Politi}, doi = {10.1103/PhysRevLett.134.097102}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {097102}, shortjournal = {Phys. Rev. Lett.}, title = {Effective grand canonical description of condensation in negative-temperature regimes}, volume = {134}, year = {2025}, }
• (2025). Computing nonequilibrium responses with score-shifted stochastic differential equations. PRL, 134(9), 097101. (www)

  @article{ , abstract = {Using equilibrium fluctuations to understand the response of a physical system to an externally imposed perturbation is the basis for linear response theory, which is widely used to interpret experiments and shed light on microscopic dynamics. For nonequilibrium systems, perturbations cannot be interpreted simply by monitoring fluctuations in a conjugate observable and general response results rely on path ensemble averaging. These techniques do not apply to perturbations that affect the diffusion tensor in a stochastic system. Here, we introduce an “effective” physical process that represents the diffusion perturbed dynamics and enables accurate calculations of responses to a change in the diffusion. Interestingly, the effective dynamics contain an additional drift involving the instantaneous “score” of the system, and we leverage score matching algorithms to carry out nonequilibrium response calculations on systems for which the exact stationary distribution is unknown.}, archive = {J_PRL}, author = {Jérémie Klinger and Grant M. Rotskoff}, doi = {10.1103/PhysRevLett.134.097101}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {097101}, shortjournal = {Phys. Rev. Lett.}, title = {Computing nonequilibrium responses with score-shifted stochastic differential equations}, volume = {134}, year = {2025}, }
• (2025). Eliminating surface oxides of superconducting circuits with noble metal encapsulation. PRL, 134(9), 097001. (www)

  @article{ , abstract = {The lifetime of superconducting qubits is limited by dielectric loss, and a major source of dielectric loss is the native oxide present at the surface of the superconducting metal. Specifically, tantalum-based superconducting qubits have been demonstrated with record lifetimes, but a major source of loss is the presence of two-level systems in the surface tantalum oxide. Here, we demonstrate a strategy for avoiding oxide formation by encapsulating the tantalum with noble metals that do not form native oxide. By depositing a few nanometers of Au or AuPd alloy before breaking vacuum, we completely suppress tantalum oxide formation. Microwave loss measurements of superconducting resonators reveal that the noble metal is proximitized, with a superconducting gap over 80% of the bare tantalum at thicknesses where the oxide is fully suppressed. Our findings suggest that losses in resonators fabricated by subtractive etching are dominated by oxides on the sidewalls, pointing to total surface encapsulation by additive fabrication as a promising strategy for eliminating surface oxide two-level system loss in superconducting qubits.}, archive = {J_PRL}, author = {Ray D. Chang and Nana Shumiya and Russell A. McLellan and Yifan Zhang and Matthew P. Bland and Faranak Bahrami and Junsik Mun and Chenyu Zhou and Kim Kisslinger and Guangming Cheng and Basil M. Smitham and Alexander C. Pakpour-Tabrizi and Nan Yao and Yimei Zhu and Mingzhao Liu and Robert J. Cava and Sarang Gopalakrishnan and Andrew A. Houck and Nathalie P. de Leon}, doi = {10.1103/PhysRevLett.134.097001}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {097001}, shortjournal = {Phys. Rev. Lett.}, title = {Eliminating surface oxides of superconducting circuits with noble metal encapsulation}, volume = {134}, year = {2025}, }
• (2025). Raman forbidden layer-breathing modes in layered semiconductor materials activated by phonon and optical cavity effects. PRL, 134(9), 096903. (www)

  @article{ , abstract = {We report Raman forbidden layer-breathing modes (LBMs) in layered semiconductor materials (LSMs). The intensity distribution of all observed LBMs depends on layer number, incident light wavelength, and refractive index mismatch between LSM and underlying substrate. These results are understood by a Raman scattering theory via the proposed spatial interference model, where the naturally occurring optical and phonon cavities in LSMs enable spatially coherent photon-phonon coupling mediated by the corresponding one-dimensional periodic electronic states. Our work reveals the impact of spatial coherence of photon and phonon fields on phonon excitation via photon or phonon cavity engineering.}, archive = {J_PRL}, author = {Miao-Ling Lin and Jiang-Bin Wu and Xue-Lu Liu and Tao Liu and Rui Mei and Heng Wu and Shan Guan and Jia-Liang Xie and Jun-Wei Luo and Lin-Wang Wang and Andrea C. Ferrari and Ping-Heng Tan}, doi = {10.1103/PhysRevLett.134.096903}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096903}, shortjournal = {Phys. Rev. Lett.}, title = {Raman forbidden layer-breathing modes in layered semiconductor materials activated by phonon and optical cavity effects}, volume = {134}, year = {2025}, }
• (2025). Bound states in the continuum in cylindrical all-dielectric metasurface cavities. PRL, 134(9), 096902. (www)

  @article{ , abstract = {Bound states in the continuum are presently demonstrated in all-dielectric, metasurface-based cavities of circularly cylindrical shapes. While their cross-sectional sizes may be arbitrary, emphasis is put on the much-needed excitation of these intriguing states in subwavelength cavities. The employed metasurfaces are characterized by effective electric and magnetic surface impedances, allowing for a swift analytical analysis of the underlying problem. The inclusion of magnetic responses, in addition to the electric one, enhances the versatility of the proposed cavities, significantly extending their application, particularly in optical contexts where magnetism is absent. To demonstrate the potential of the proposed method, an all-dielectric metasurface composed of appropriately arranged silicon particles is designed and investigated in the optical frequency range, resulting in a quality factor of .}, archive = {J_PRL}, author = {Pietro Brugnolo and Samel Arslanagić and Rasmus E. Jacobsen}, doi = {10.1103/PhysRevLett.134.096902}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096902}, shortjournal = {Phys. Rev. Lett.}, title = {Bound states in the continuum in cylindrical all-dielectric metasurface cavities}, volume = {134}, year = {2025}, }
• (2025). Exploring single-photon recoil on free electrons. PRL, 134(9), 096901. (www)

  @article{ , abstract = {Recent advancements in time-resolved electron and photon detection enable novel correlative measurements of electrons and their associated cathodoluminescence (CL) photons within a transmission electron microscope. These studies are pivotal for understanding the underlying physics in coherent CL processes. We present experimental investigations of energy-momentum conservation on the single particle level, achieved through coincidence detection of electron-photon pairs. This not only enables unprecedented clarity in detecting weak signals otherwise obscured by nonradiative processes but also provides a new experimental pathway to investigate momentum-position correlations to explore entanglement within electron-photon pairs.}, archive = {J_PRL}, author = {Alexander Preimesberger and Dominik Hornof and Theo Dorfner and Thomas Schachinger and Martin Hrtoň and Andrea Konečná and Philipp Haslinger}, doi = {10.1103/PhysRevLett.134.096901}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096901}, shortjournal = {Phys. Rev. Lett.}, title = {Exploring single-photon recoil on free electrons}, volume = {134}, year = {2025}, }
• (2025). Mirror chern bands and weyl nodal loops in altermagnets. PRL, 134(9), 096703. (www)

  @article{ , abstract = {The electronic spectra of altermagnets are a fertile ground for nontrivial topology due to the unique interplay between time-reversal and crystalline symmetries. This is reflected in the unconventional Zeeman splitting between bands of opposite spins, which emerges in the absence of spin-orbit coupling (SOC) and displays nodes along high-symmetry directions. Here, we argue that even for a small SOC, the direction of the magnetic moments in the altermagnetic state has a profound impact on the electronic spectrum, enabling novel topological phenomena to appear. By investigating microscopic models for two-dimensional (2D) and three-dimensional (3D) altermagnets, motivated in part by rutile materials, we demonstrate the emergence of hitherto unexplored Dirac crossings between bands of the same spin but opposite sublattices. The direction of the moments determines the fate of these crossings when the SOC is turned on. We focus on the case of out-of-plane moments, which forbid an anomalous Hall effect and thus ensure that no weak magnetization is triggered in the altermagnetic state. In the 2D model, the SOC gaps out the Dirac crossings, resulting in mirror Chern bands that enable the Quantum Spin Hall Effect and undergo a topological transition to trivial bands upon increasing the magnitude of the magnetic moment. On the other hand, in the 3D model the crossings persist even in the presence of SOC, forming Weyl nodal loops protected by mirror symmetry. Finally, we discuss possible ways to control these effects in altermagnetic material candidates.}, archive = {J_PRL}, author = {Daniil S. Antonenko and Rafael M. Fernandes and Jörn W. F. Venderbos}, doi = {10.1103/PhysRevLett.134.096703}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096703}, shortjournal = {Phys. Rev. Lett.}, title = {Mirror chern bands and weyl nodal loops in altermagnets}, volume = {134}, year = {2025}, }
• (2025). Satisfaction and violation of the fluctuation-dissipation relation in spin ice materials. PRL, 134(9), 096702. (www)

  @article{ , abstract = {We test the fluctuation-dissipation relation (FDR) in spin ice materials and by measuring both the magnetic noise and the out-of-phase part of the susceptibility and comparing their ratio. We show that it is satisfied at temperatures well into the nonergodic region below 600 mK, indicating local equilibrium. In both materials, below 400 mK, low frequency violations develop, showing an excess of noise as in spin glasses, with a frequency threshold of 0.1 Hz. New relaxation pathways and aging properties are unveiled in this frequency range in the ac susceptibility. The FDR remains valid at higher frequencies down to 150 mK.}, archive = {J_PRL}, author = {F. Morineau and V. Cathelin and P. C. W. Holdsworth and S. R. Giblin and G. Balakhrishnan and K. Matsuhira and C. Paulsen and E. Lhotel}, doi = {10.1103/PhysRevLett.134.096702}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096702}, shortjournal = {Phys. Rev. Lett.}, title = {Satisfaction and violation of the fluctuation-dissipation relation in spin ice materials}, volume = {134}, year = {2025}, }
• (2025). Unconventional spin hall magnetoresistance in noncollinear Antiferromagnet/Heavy metal stacks. PRL, 134(9), 096701. (www)

  @article{ , abstract = {We study the spin Hall magnetoresistance (SMR) in noncollinear antiferromagnet metal stacks. The measured SMR exhibits peculiar magnetic field angle and magnitude dependence that sharply deviates from the conventional SMR theory based on the dampinglike spin-transfer torque. An alternative model based on a coherent fieldlike torque reproduces the observations well. Our work reveals a previously unrecognized mechanism of interfacial exchange that indicates a precession of the conduction-electron spins in the collective local exchange fields of the noncollinear antiferromagnetic order. The unraveled physics is essential to understanding and controlling spin transport in unconventional magnetic materials.}, archive = {J_PRL}, author = {Tomohiro Uchimura and Jiahao Han and Ping Tang and Ju-Young Yoon and Yutaro Takeuchi and Yuta Yamane and Shun Kanai and Gerrit E. W. Bauer and Hideo Ohno and Shunsuke Fukami}, doi = {10.1103/PhysRevLett.134.096701}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096701}, shortjournal = {Phys. Rev. Lett.}, title = {Unconventional spin hall magnetoresistance in noncollinear Antiferromagnet/Heavy metal stacks}, volume = {134}, year = {2025}, }
• (2025). Characterizing dynamic hybridization of majorana zero modes for universal quantum computing. PRL, 134(9), 096601. (www)

  @article{ , abstract = {Qubits built out of Majorana zero modes (MZMs) have long been theorized as a potential pathway toward fault-tolerant topological quantum computation. Almost unavoidable in these processes is Majorana wave function overlap, known as hybridization, which arises throughout the process when Majorana modes get close to each other. This breaks the ground state degeneracy, leading to qubit errors in the braiding process. This work presents a simple but precise method to predict qubit errors for dynamic hybridization which varies in space and time. This includes hybridization between four or more MZMs through topological or trivial regions or both of them. As an illustration, we characterize qubit errors for an X gate. We demonstrate how to utilize the hybridization to implement not only arbitrary one-qubit rotations but also a two-qubit controlled variable phase gate, providing a demonstration of universal quantum computing.}, archive = {J_PRL}, author = {Themba Hodge and Eric Mascot and Dan Crawford and Stephan Rachel}, doi = {10.1103/PhysRevLett.134.096601}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096601}, shortjournal = {Phys. Rev. Lett.}, title = {Characterizing dynamic hybridization of majorana zero modes for universal quantum computing}, volume = {134}, year = {2025}, }
• (2025). Many-body effects on high-harmonic generation in hubbard ladders. PRL, 134(9), 096504. (www)

  @article{ , abstract = {We unveil multifaceted effects of spin-charge couplings on the high-harmonic generation (HHG) in Mott insulators by analyzing the two-leg ladder Hubbard model, where spin dynamics activated by the interchain hopping t y drastically modifies the HHG features. When the two chains are decoupled ( t y = 0 ), HHG originates from the dynamics of coherent doublon-holon pairs because of spin-charge separation. With increasing t y , the doublon-holon pairs lose their coherence due to their interchain hopping and resultant nonlocal spin strings. Furthermore, the HHG signal from spin polarons—charges dressed by spin clouds—leads to an additional plateau in the HHG spectrum. For large t y , we identify unconventional HHG processes involving three elementary excitations—two polarons and one magnon. Our study is an essential step toward a microscopic understanding of nontrivial many-body effects on HHG in correlated materials beyond conventional semiconductors.}, archive = {J_PRL}, author = {Yuta Murakami and Thomas Hansen and Shintaro Takayoshi and Lars Bojer Madsen and Philipp Werner}, doi = {10.1103/PhysRevLett.134.096504}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096504}, shortjournal = {Phys. Rev. Lett.}, title = {Many-body effects on high-harmonic generation in hubbard ladders}, volume = {134}, year = {2025}, }
• (2025). Decoherence through ancilla anyon reservoirs. PRL, 134(9), 096503. (www)

  @article{ , abstract = {We explore the decoherence of the critical (gapless) boundary of a topological order, through interactions with the bulk reservoir of “ancilla anyons.” We take the critical boundary of the Toric code as an example. The intrinsic nonlocal nature of the anyons demands the strong and weak symmetry condition for the ordinary decoherence problem be extended to the strong or weak gauge invariance conditions. We demonstrate that in the doubled Hilbert space, the partition function of the boundary is mapped to two layers of the critical Ising model with an interlayer line defect that depends on the species of the anyons causing the decoherence. The line defects associated with the tunneling of bosonic and anyons are relevant, and result in long-range correlations for either the or anyon, respectively, on the boundary in the doubled Hilbert space. In contrast, the defect of the anyon is marginal and leads to a line of fixed points with varying effective central charges, and power-law correlations having continuously varying scaling dimensions. We also demonstrate that decoherence-analogs of Majorana zero modes are localized at the spatial interface of the relevant and anyon decoherence channels, which leads to a universal logarithmic scaling of the Rényi entropy of the boundary.}, archive = {J_PRL}, author = {Nayan Myerson-Jain and Taylor L. Hughes and Cenke Xu}, doi = {10.1103/PhysRevLett.134.096503}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096503}, shortjournal = {Phys. Rev. Lett.}, title = {Decoherence through ancilla anyon reservoirs}, volume = {134}, year = {2025}, }
• (2025). Signature of preformed pairs in angle-resolved photoemission spectroscopy. PRL, 134(9), 096502. (www)

  @article{ , abstract = {We use density matrix renormalization group (DMRG) and variational exact diagonalization (VED) to calculate the single-electron removal spectral weight for the Hubbard-Holstein model at low electron densities. Tuning the strength of the electron-phonon coupling and of the Hubbard repulsion allows us to contrast the results for a liquid of polarons versus a liquid of bipolarons. The former shows spectral weight up to the Fermi energy, as expected for a metal. The latter has a gap in its spectral weight, set by the bipolaron binding energy, although this is also a (strongly correlated) metal. This difference suggests that angle-resolved photoemission spectroscopy could be used to identify liquids of pre-formed pairs. Furthermore, we show that the one-dimensional liquid of incoherent bipolarons is well approximated by a “Bose sea” of bosons that are hard-core in momentum space, occupying the momenta inside the Fermi sea but otherwise noninteracting. This new proposal for a strongly correlated many-body wave function opens the way for studying various other properties of incoherent (nonsuperconducting) liquids of preformed pairs in any dimension.}, archive = {J_PRL}, author = {Klemen Kovač and Alberto Nocera and Andrea Damascelli and Janez Bonča and Mona Berciu}, doi = {10.1103/PhysRevLett.134.096502}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096502}, shortjournal = {Phys. Rev. Lett.}, title = {Signature of preformed pairs in angle-resolved photoemission spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Connecting high-field and high-pressure superconductivity in UTe2. PRL, 134(9), 096501. (www)

  @article{ , abstract = {The existence of multiple superconducting phases induced by either pressure or magnetic field is one of the most striking features of superconductivity of U T e 2 , among the many unusual superconducting properties of this system. Here we report thermodynamic measurements of the superconducting phase diagram combining pressure and magnetic fields up to 30 T. We show that the high-field superconducting phase at ambient pressure continuously evolves under pressure into the zero-field high-temperature superconducting phase, which occurs above 0.2 GPa.}, archive = {J_PRL}, author = {T. Vasina and D. Aoki and A. Miyake and G. Seyfarth and A. Pourret and C. Marcenat and M. Amano Patino and G. Lapertot and J. Flouquet and J.-P. Brison and D. Braithwaite and G. Knebel}, doi = {10.1103/PhysRevLett.134.096501}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096501}, shortjournal = {Phys. Rev. Lett.}, title = {Connecting high-field and high-pressure superconductivity in UTe2}, volume = {134}, year = {2025}, }
• (2025). Chirality in the kagome metal CsV3Sb5. PRL, 134(9), 096401. (www)

  @article{ , abstract = {Using x-ray photoelectron diffraction (XPD) and angle-resolved photoemission spectroscopy, we study photoemission intensity changes related to changes in the geometric and electronic structure in the kagome metal CsV 3 Sb 5 upon transition to an unconventional charge density wave (CDW) state. The XPD patterns reveal the presence of a chiral atomic structure in the CDW phase. Furthermore, using circularly polarized x-rays, we have found a pronounced nontrivial circular dichroism in the angular distribution of the valence band photoemission in the CDW phase, indicating a chirality of the electronic structure. This observation is consistent with the proposed orbital loop current order. In view of a negligible spontaneous Kerr signal in recent magneto-optical studies, the results suggest an antiferromagnetic coupling of the orbital magnetic moments along the c axis. While the inherent structural chirality may also induce circular dichroism, the observed asymmetry values seem to be too large in the case of the weak structural distortions caused by the CDW.}, archive = {J_PRL}, author = {H. J. Elmers and O. Tkach and Y. Lytvynenko and P. Yogi and M. Schmitt and D. Biswas and J. Liu and S. V. Chernov and Quynh Nguyen and M. Hoesch and D. Kutnyakhov and N. Wind and L. Wenthaus and M. Scholz and K. Rossnagel and A. Gloskovskii and C. Schlueter and A. Winkelmann and A.-A. Haghighirad and T.-L. Lee and M. Sing and R. Claessen and M. Le Tacon and J. Demsar and G. Schönhense and O. Fedchenko}, doi = {10.1103/PhysRevLett.134.096401}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096401}, shortjournal = {Phys. Rev. Lett.}, title = {Chirality in the kagome metal CsV3Sb5}, volume = {134}, year = {2025}, }
• (2025). Landscapes of an out-of-equilibrium anyonic sea. PRL, 134(9), 096303. (www)

  @article{ , abstract = {The low-energy dynamics of two-dimensional topological matter hinges on its one-dimensional edge modes. Tunneling between fractional quantum Hall edge modes facilitates the study of anyonic statistics: it induces time-domain braiding that dominates signals from diluted anyon beams. We develop a framework for characterizing one-dimensional out-of-equilibrium anyonic states and define their effective potential and temperature, both arising from anyonic braiding, as well as the landscape of their excitations. Unlike fermions, the effective anyon potential depends on the type of the tunneling quasiparticles; nonequilibrium anyonic states are underlain by power-law energy distributions. This allows “hot” anyons to tunnel above the chemical potential of the source, which we capture by a measurable universal witness function. Our analysis raises the prospect of generalizing the kinetic approach to compressible anyonic matter in higher dimensions.}, archive = {J_PRL}, author = {Gu Zhang and Igor Gornyi and Yuval Gefen}, doi = {10.1103/PhysRevLett.134.096303}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096303}, shortjournal = {Phys. Rev. Lett.}, title = {Landscapes of an out-of-equilibrium anyonic sea}, volume = {134}, year = {2025}, }
• (2025). Domain-wall ferroelectric polarons in a two-dimensional rotor lattice model. PRL, 134(9), 096302. (www)

  @article{ , abstract = {We demonstrate the formation of ferroelectric domain-wall polarons in a minimal two-dimensional lattice model of electrons interacting with rotating dipoles. Along the domain wall, the rotors polarize in opposite directions, causing the electron to localize along a particular lattice direction. The rotor-electron coupling is identified as the origin of a structural instability in the crystal that leads to the domain-wall formation via a symmetry-breaking process. Our results provide the first theoretical description of ferroelectric polarons, as discussed in the context of soft semiconductors.}, archive = {J_PRL}, author = {Florian Kluibenschedl and Georgios M. Koutentakis and Ragheed Alhyder and Mikhail Lemeshko}, doi = {10.1103/PhysRevLett.134.096302}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096302}, shortjournal = {Phys. Rev. Lett.}, title = {Domain-wall ferroelectric polarons in a two-dimensional rotor lattice model}, volume = {134}, year = {2025}, }
• (2025). Coherent detection of the oscillating acoustoelectric effect in graphene. PRL, 134(9), 096301. (www)

  @article{ , abstract = {In recent years, surface acoustic waves (SAWs) have emerged as a novel technique for generating quasiparticle transport and band modulation in condensed matter systems. SAWs interact with adjacent materials through piezoelectric and strain fields, dragging carriers in the direction of wave propagation. Most studies on the acoustoelectric effect have focused on the collective directional motion of carriers, which generates a steady electric potential difference, while the oscillating component from dynamic spatial charge modulation has remained challenging to probe. In this Letter, we report the coherent detection of the oscillating acoustoelectric effect in graphene. This is achieved through the coherent rectification of spatial-temporal charge oscillation with electromagnetic waves emitted by interdigital transducers. We systematically investigate the frequency and gate dependence of rectified signals and quantitatively probe the carrier redistribution dynamics driven by SAWs. The observation of the oscillating acoustoelectric effect provides direct access to the dynamic spatial charge modulation induced by SAWs through transport experiments.}, archive = {J_PRL}, author = {Yicheng Mou and Jiayu Wang and Haonan Chen and Yingchao Xia and Hailong Li and Qing Yan and Xue Jiang and Yijia Wu and Wu Shi and Hua Jiang and X. C. Xie and Cheng Zhang}, doi = {10.1103/PhysRevLett.134.096301}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096301}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent detection of the oscillating acoustoelectric effect in graphene}, volume = {134}, year = {2025}, }
• (2025). Independently tunable flat bands and correlations in a graphene double moiré system. PRL, 134(9), 096204. (www)

  @article{ , abstract = {We report on a double moiré system consisting of four graphene layers, where the top and bottom pairs form small-twist-angle bilayer graphene, and the middle interface has a large rotational mismatch. This system shows clear signatures of two sets of spatially separated flat bands associated with the top and bottom twisted bilayer graphene subsystems, each independently tunable. Thermodynamic analysis reveals weak correlations between bilayers that allow the chemical potential to be measured as a function of carrier density for each constituent TBG. We find that correlated insulating states at integer number of electrons per moiré unit cell are most robust near magic angle, whereas gapped states at neutrality are more robust at larger twist angles.}, archive = {J_PRL}, author = {Yimeng Wang and Jihang Zhu and G. William Burg and Anand Swain and Kenji Watanabe and Takashi Taniguchi and Yuebing Zheng and Allan H. MacDonald and Emanuel Tutuc}, doi = {10.1103/PhysRevLett.134.096204}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096204}, shortjournal = {Phys. Rev. Lett.}, title = {Independently tunable flat bands and correlations in a graphene double moiré system}, volume = {134}, year = {2025}, }
• (2025). Auroralike light from a polymer p−n junction emitting free electrons. PRL, 134(9), 096203. (www)

  @article{ , abstract = {Luminescent conjugated polymers are organic semiconductors possessing unique electrical and optical properties. Luminescent polymers have been extensively investigated because of their potential applications in light sources and display devices. Here, we provide the first evidence that a luminescent polymer is also a strong emitter of free electrons and a source of new light. Vivid green light flashes have been observed from a red-emitting polymer junction under a large reverse bias. The junctions have a planar configuration, revealing that the green light flashes are emitted into free space, far beyond the confines of electrodes. Moreover, the green flashes can be strongly distorted by a permanent magnet placed nearby, generating a light show resembling an aurora. Like the aurora, the green light flashes are caused by charged particles. By applying a known transverse magnetic field to bend the flashes into circular arcs, a charge to mass ratio is determined for the charged particles. The auroralike green light coincides with the formation of electrical trees in the -doped region of the junction. We postulate that the green light is caused by field-emitted electrons exciting an unknown organic vapor released in the treeing process.}, archive = {J_PRL}, author = {Dongze Wang and Jun Gao}, doi = {10.1103/PhysRevLett.134.096203}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096203}, shortjournal = {Phys. Rev. Lett.}, title = {Auroralike light from a polymer p−n junction emitting free electrons}, volume = {134}, year = {2025}, }
• (2025). Intrinsic high-fidelity spin polarization of charged vacancies in hexagonal boron nitride. PRL, 134(9), 096202. (www)

  @article{ , abstract = {The negatively charged boron vacancy ( ) in hexagonal boron nitride (hBN) has garnered significant attention among defects in two-dimensional materials. This owes, in part, to its deterministic generation, well-characterized atomic structure, and optical polarizability at room temperature. We investigate the latter through extensive measurements probing both the ground and excited state polarization dynamics. We develop a semiclassical model based on these measurements that predicts a near-unity degree of spin polarization, surpassing other solid-state spin defects under ambient conditions. Building upon our model, we include the presence of nuclear spin degrees of freedom adjacent to the and perform a comprehensive set of Lindbladian numerics to investigate the hyperfine-induced polarization of the nuclear spins. Our simulations predict a number of important features that emerge as a function of magnetic field which are borne out by experiment.}, archive = {J_PRL}, author = {W. Lee and V. S. Liu and Z. Zhang and S. Kim and R. Gong and X. Du and K. Pham and T. Poirier and Z. Hao and J. H. Edgar and P. Kim and C. Zu and E. J. Davis and N. Y. Yao}, doi = {10.1103/PhysRevLett.134.096202}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096202}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic high-fidelity spin polarization of charged vacancies in hexagonal boron nitride}, volume = {134}, year = {2025}, }
• (2025). Automatic process exploration through machine learning assisted transition state searches. PRL, 134(9), 096201. (www)

  @article{ , abstract = {We present an efficient automatic process explorer (APE) framework to overcome the reliance on human intuition to empirically establish relevant elementary processes of a given system, e.g., in prevalent kinetic Monte Carlo (kMC) simulations based on fixed process lists. Use of a fuzzy machine learning classification algorithm minimizes redundancy in the transition-state searches by driving them toward hitherto unexplored local atomic environments. APE application to island diffusion at a Pd(100) surface immediately reveals a large number of, up to now, disregarded low-barrier collective processes that lead to a significant increase in the kMC-determined island diffusivity as compared to classic surface hopping and exchange diffusion mechanisms.}, archive = {J_PRL}, author = {King Chun Lai and Patricia Poths and Sebastian Matera and Christoph Scheurer and Karsten Reuter}, doi = {10.1103/PhysRevLett.134.096201}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096201}, shortjournal = {Phys. Rev. Lett.}, title = {Automatic process exploration through machine learning assisted transition state searches}, volume = {134}, year = {2025}, }
• (2025). Thermodynamic evidence for density wave order in a two dimensional he4 supersolid. PRL, 134(9), 096002. (www)

  @article{ , abstract = {We previously reported the discovery of a two-dimensional He 4 supersolid; a state with intertwined density wave and superfluid order, observed in the second layer of He 4 adsorbed on graphite. In this Letter we provide direct evidence for the density wave order, obtained by doping the layer with a small concentration of He 3 atoms (impuritons). The heat capacity, magnetization and NMR relaxation times of the He 3 were measured over a wide temperature range from 200 μ K to 500 mK. They provide evidence for changes in the ground state in the second layer film as the amount of He 4 is increased at various fixed He 3 doses. Clear evidence is obtained for a solid second layer film, matching the regime of superfluid response previously observed in pure He 4 films.}, archive = {J_PRL}, author = {J. Knapp and J. Nyéki and H. Patel and F. Ziouzia and B. P. Cowan and J. Saunders}, doi = {10.1103/PhysRevLett.134.096002}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096002}, shortjournal = {Phys. Rev. Lett.}, title = {Thermodynamic evidence for density wave order in a two dimensional he4 supersolid}, volume = {134}, year = {2025}, }
• (2025). Universal phenomenology of charge-spin interconversion and dynamics in diffusive systems with spin-orbit coupling. PRL, 134(9), 096001. (www)

  @article{ , abstract = {We present a unified description of transport in normal and superconducting metals in the presence of generic spin-orbit coupling (SOC). The structure of the quantum kinetic theory in the diffusive regime is determined by a set of fundamental constraints—charge conjugation symmetry, the causality principle, and the crystal symmetry of a material. These symmetries uniquely fix the action of the Keldysh nonlinear model (NLSM), which at the saddle point yields the quantum kinetic Usadel-type equation, the equation that describes the main transport features of a system. Our phenomenological approach is reminiscent of the Ginzburg-Landau theory but is valid for superconductors in the whole temperature range, describes the diffusive transport in the normal state, and naturally captures the effects of superconducting fluctuations. As an application, we derive the NLSM and the corresponding quantum transport equations, which include all effects of spin-orbit coupling, allowed by the crystal symmetry, for example, the spin Hall, spin current swapping, or spin-galvanic effects. Our approach can be extended to derive transport equations in systems with broken time reversal symmetry, as well as to the description of hybrid interfaces, where the spin-charge interconversion can be enhanced due to strong interfacial SOC.}, archive = {J_PRL}, author = {Tim Kokkeler and F. Sebastian Bergeret and I. V. Tokatly}, doi = {10.1103/PhysRevLett.134.096001}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {096001}, shortjournal = {Phys. Rev. Lett.}, title = {Universal phenomenology of charge-spin interconversion and dynamics in diffusive systems with spin-orbit coupling}, volume = {134}, year = {2025}, }
• (2025). Measurement of zero-frequency fluctuations generated by coupling between alfvén modes in the JET tokamak. PRL, 134(9), 095103. (www)

  @article{ , abstract = {We report the first experimental detection of a zero-frequency fluctuation that is pumped by an Alfvén mode in a magnetically confined plasma. Core-localized Alfvén modes of frequency inside the toroidicity-induced gap (and its harmonics) exhibit three-wave coupling interactions with a zero-frequency fluctuation. The observation of the zero-frequency fluctuation is consistent with theoretical and numerical predictions of zonal modes pumped by Alfvén modes, and is correlated with an increase in the deep core ion temperature, temperature gradient, confinement factor , and a reduction in the main ion heat diffusivity. Despite the energetic particle transport induced by the Alfvén eigenmodes, the generation of a zero-frequency fluctuation that can suppress the turbulence leads to an overall improvement of confinement.}, archive = {J_PRL}, author = {the JET Contributors and the EUROfusion Tokamak Exploitation Team and J. Ruiz Ruiz and J. Garcia and M. Barnes and M. Dreval and C. Giroud and V. H. Hall-Chen and M. R. Hardman and J. C. Hillesheim and Y. Kazakov and S. Mazzi and B. S. Patel and F. I. Parra and A. A. Schekochihin and Ž. Štancar}, doi = {10.1103/PhysRevLett.134.095103}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {095103}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of zero-frequency fluctuations generated by coupling between alfvén modes in the JET tokamak}, volume = {134}, year = {2025}, }
• (2025). Group conductivity and nonadiabatic born effective charges of disordered metals, warm dense matter, and hot dense plasma. PRL, 134(9), 095102. (www)

  @article{ , abstract = {The average ionization state is a critical parameter in plasma models for charged particle transport, equations of state, and optical response. The dynamical or nonadiabatic Born effective charge (NBEC), calculated via first principles time-dependent density-functional theory, provides exact ionic partitioning of bulk electron response for both metallic and insulating materials. The NBEC can be transformed into a “group conductivity,” i.e., the electron conductivity ascribed to a subset of ions. We show that for disordered metallic systems, such as warm dense matter (WDM) and hot dense plasma, the static limit of the NBEC is different from the average ionization states, but that the ionization state can be extracted from the group conductivity even in mixed systems. We demonstrate this approach using a set of archetypical examples, including cold and warm aluminium, low- and high-density WDM carbon, and a WDM carbon-beryllium-hydrogen mixture.}, archive = {J_PRL}, author = {Vidushi Sharma and Alexander J. White}, doi = {10.1103/PhysRevLett.134.095102}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {095102}, shortjournal = {Phys. Rev. Lett.}, title = {Group conductivity and nonadiabatic born effective charges of disordered metals, warm dense matter, and hot dense plasma}, volume = {134}, year = {2025}, }
• (2025). First measurement of z opacity sample evolution near solar interior conditions using time-resolved spectroscopy. PRL, 134(9), 095101. (www)

  @article{ , abstract = {Opacity model differences with Fe opacity measurements at high temperature ( ) and high electron density ( ) at nearly solar interior conditions have remained unresolved [Bailey et al. , Nature 517 , 56 (2015) and Nagayama et al. , Phys. Rev. Lett. 122 , 235001 (2019) ]. Systematic errors from temporal gradients are one hypothesis for the discrepancy. Past data recorded on x-ray film provided spectral measurements over a time determined by the 2.8-ns backlighter duration. Here, we present the first measurements of opacity sample temporal evolution using novel hCMOS ultrafast x-ray camera technology. The measured conditions, measured backlighter time history, and modeled opacities are used to show that temporal gradients do not resolve the model-data discrepancy. The methods demonstrated provide potential advantages, including opacities at more extreme conditions, spectral line shift measurements, and improved measurements at other facilities.}, archive = {J_PRL}, author = {G. P. Loisel and J. E. Bailey and T. Nagayama and S. B. Hansen and G. S. Dunham and P. D. Gard and A. P. Colombo and A. D. Edens and R. Speas and Q. Looker and M. Kimmel and J. L. Porter and E. C. Harding and G. A. Rochau and C. J. Fontes and J. P. Colgan and C. Blancard and Ph. Cossé and G. Faussurier and F. Gilleron and J.-Ch. Pain and D. Aberg}, doi = {10.1103/PhysRevLett.134.095101}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {095101}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of z opacity sample evolution near solar interior conditions using time-resolved spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Invariant forms of dissolution fingers. PRL, 134(9), 094101. (www)

  @article{ , abstract = {Dissolution of fractured and porous media introduces a positive feedback between fluid flow and reactant transport, leading to the emergence of pronounced, fingerlike channels. We investigate the formation of these structures using a microfluidic Hele-Shaw cell with a soluble bottom. Our experiments show that the shape of dissolution fingers is invariant and reveals itself over time as the fingers extend into the system. By combining reactive-transport theory and conformal mapping techniques we derive these invariant forms. We relate these results to natural dissolution fingers in karst landscapes, and illustrate how to determine the groundwater flow rate responsible for their formation based on the finger shape.}, archive = {J_PRL}, author = {Stanisław Żukowski and Silvana Magni and Florian Osselin and Filip Dutka and Max Cooper and Anthony J. C. Ladd and Piotr Szymczak}, doi = {10.1103/PhysRevLett.134.094101}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {094101}, shortjournal = {Phys. Rev. Lett.}, title = {Invariant forms of dissolution fingers}, volume = {134}, year = {2025}, }
• (2025). Direct measurement of the viscocapillary lift force near a liquid interface. PRL, 134(9), 094001. (www)

  @article{ , abstract = {Lift force of viscous origin is widespread across disciplines, from mechanics to biology. Here, we present the first direct measurement of the lift force acting on a particle moving in a viscous fluid along the liquid interface that separates two liquids. The force arises from the coupling between the viscous flow induced by the particle motion and the capillary deformation of the interface. The measurements show that the lift force increases as the distance between the sphere and the interface decreases, reaching saturation at small distances. The experimental results are in good agreement with the model and numerical calculation developed within the framework of the soft lubrication theory.}, archive = {J_PRL}, author = {Hao Zhang and Zaicheng Zhang and Aditya Jha and Yacine Amarouchene and Thomas Salez and Thomas Guérin and Chaouqi Misbah and Abdelhamid Maali}, doi = {10.1103/PhysRevLett.134.094001}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {094001}, shortjournal = {Phys. Rev. Lett.}, title = {Direct measurement of the viscocapillary lift force near a liquid interface}, volume = {134}, year = {2025}, }
• (2025). Resolving the orientations of and angular separation between a pair of dipole emitters. PRL, 134(9), 093805. (www)

  @article{ , abstract = {We prove that it is impossible to distinguish two spatially coinciding fluorescent molecules from a single rotating molecule using polarization-sensitive imaging, even if one modulates the polarization of the illumination or the detection dipole-spread function (DSF). If the target is known to be a dipole pair, existing imaging methods perform poorly for measuring their angular separation. We propose simultaneously modulating the excitation polarization and DSF, which demonstrates robust discrimination between dipole pairs versus single molecules. Our method improves the precision of measuring centroid orientation by 50% and angular separation by two- to four-fold over existing techniques.}, archive = {J_PRL}, author = {Yiyang Chen and Yuanxin Qiu and Matthew D. Lew}, doi = {10.1103/PhysRevLett.134.093805}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093805}, shortjournal = {Phys. Rev. Lett.}, title = {Resolving the orientations of and angular separation between a pair of dipole emitters}, volume = {134}, year = {2025}, }
• (2025). Mid-infrared energy deposition spectroscopy. PRL, 134(9), 093804. (www)

  @article{ , abstract = {It is generally assumed that the spectral acquisition speed in photothermal spectroscopy is fundamentally limited by the thermal diffusion process. Here, we demonstrate midinfrared energy deposition (MIRED) spectroscopy that offers both microsecond-scale temporal resolution and submicron spatial resolution. In this approach, the photothermal process is optically probed while the infrared pulses from a quantum cascade laser array are rapidly tuned. Based on Newton’s law of heating and cooling, the energy deposition is the first derivative of local temperature rise over time and gives the instantaneous absorption. By employing time-resolved measurement of transient energy deposition, the upper limit for spectrum encoding shifts to the vibrational relaxation level, which occurs on the picosecond scale. This method significantly increases the detection bandwidth while retaining the sensitivity and resolution benefits of photothermal detection.}, archive = {J_PRL}, author = {Jiaze Yin and Christian Pfluegl and Chu C. Teng and Rylie Bolarinho and Guo Chen and Xinrui Gong and Dashan Dong and Daryoosh Vakhshoori and Ji-Xin Cheng}, doi = {10.1103/PhysRevLett.134.093804}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093804}, shortjournal = {Phys. Rev. Lett.}, title = {Mid-infrared energy deposition spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Observation of a giant goos-hänchen shift for matter waves. PRL, 134(9), 093803. (www)

  @article{ , abstract = {The Goos-Hänchen (GH) shift describes a phenomenon in which a specularly reflected beam is translated along the reflecting surface such that the incident and reflected rays no longer intersect at the surface. Using a neutron spin-echo technique and a specially designed magnetic multilayer mirror, we have measured the relative phase between the reflected up and down neutron spin states in total reflection. The relative GH shift calculated from this phase shows a strong resonant enhancement at a particular incident neutron wave vector, which is due to a waveguiding effect in one of the magnetic layers. Calculations based on the observed phase difference between the neutron states indicate a propagation distance along the waveguide layer of 0.65 mm for the spin-down state, which we identify with the magnitude of the giant GH shift. The existence of a physical GH shift is confirmed by the observation of neutron absorption in the waveguide layer. We propose ways in which our experimental method may be exploited for neutron quantum-enhanced sensing of thin magnetic layers.}, archive = {J_PRL}, author = {S. McKay and V. O. de Haan and J. Leiner and S. R. Parnell and R. M. Dalgliesh and P. Boeni and L. J. Bannenberg and Q. Le Thien and D. V. Baxter and G. Ortiz and R. Pynn}, doi = {10.1103/PhysRevLett.134.093803}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093803}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of a giant goos-hänchen shift for matter waves}, volume = {134}, year = {2025}, }
• (2025). Entangled-beam reflectometry and goos-hänchen shift. PRL, 134(9), 093802. (www)

  @article{ , abstract = {We introduce the technique of entangled-beam reflectometry for extracting spatially correlated (magnetic or nonmagnetic) information from material surfaces or thin films. Our amplitude- and phase-sensitive technique exploits the coherent nature of an incoming entangled probe beam, of matter or light waves, undergoing reflection from the surface. Such reflection encodes the surface spatial structure into the probe’s geometric and phase-derived Goos-Hänchen shifts, which can then be measured to unveil the structure. We investigate the way these shifts depend on the wave packet widths, and illustrate our technique in the case of in-plane periodic (non)magnetic structures by utilizing spin-path mode-entangled neutron beams.}, archive = {J_PRL}, author = {Q. Le Thien and R. Pynn and G. Ortiz}, doi = {10.1103/PhysRevLett.134.093802}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093802}, shortjournal = {Phys. Rev. Lett.}, title = {Entangled-beam reflectometry and goos-hänchen shift}, volume = {134}, year = {2025}, }
• (2025). Thouless pumping in a driven-dissipative kerr resonator array. PRL, 134(9), 093801. (www)

  @article{ , abstract = {Thouless pumping is an emblematic manifestation of topology in physics, referring to the ability to induce a quantized transport of charge across a system by simply varying one of its parameters periodically in time. The original concept of Thouless pumping involves a noninteracting system, and has been implemented in several platforms. One current challenge in the field is to extend this concept to interacting systems. In this Letter, we propose a Thouless pump that solely relies on nonlinear physics, within a chain of coupled Kerr resonators. Leveraging the driven-dissipative nature of the system, we modulate in space and time the on-site Kerr interaction energies, and generate -dimensional topological bands in the Bogoliubov spectrum of excitations. These bands present the same topology as the ones obtained within the Harper-Hofstadter framework, and the Wannier states associated to each band experience a net displacement and show quantized transport according to the band Chern numbers. Remarkably, we find driving configurations leading to band inversion, revealing an interaction-induced topological transition. Our numerical simulations are performed using realistic parameters inspired from exciton polaritons, which form a platform of choice for investigating driven topological phases of matter.}, archive = {J_PRL}, author = {S. Ravets and N. Pernet and N. Mostaan and N. Goldman and J. Bloch}, doi = {10.1103/PhysRevLett.134.093801}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093801}, shortjournal = {Phys. Rev. Lett.}, title = {Thouless pumping in a driven-dissipative kerr resonator array}, volume = {134}, year = {2025}, }
• (2025). Test of nonlocal energy alteration between two quantum memories. PRL, 134(9), 093601. (www)

  @article{ , abstract = {When two particles are spin entangled, one may exhibit behavior that suggests its spin can nonlocally influence the spin of the other. This implies that the energy of the latter particle can be altered by a nonlocal quantum correlation, without enabling any form of superluminal communication. This energy alteration, however, remains to be experimentally testified. To test this phenomenon, we construct an incomplete Mach-Zehnder interferometer utilizing two quantum memories. The Stokes photon generated by the quantum memories serves as the first particle, while the atomic excitation stored within the memories acts as the second particle. Our results demonstrate that if the de Broglie–Bohm interpretation is realistic, the trajectory of the Stokes photon can be nonlocally influenced by a slight probe of the atomic excitation. Conversely, the position of the atomic excitation, as well as the energy ℏ ω hf it carries, can also be nonlocally altered by controlling the Stokes photon. These findings underscore the continued relevance of nonlocality in hidden variable theories, consistent with Bell’s theorem and recent experimental validations, while making clear that such phenomena do not violate the principles of relativity.}, archive = {J_PRL}, author = {Jian-Peng Dou and Feng Lu and Hao Tang and Xian-Min Jin}, doi = {10.1103/PhysRevLett.134.093601}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093601}, shortjournal = {Phys. Rev. Lett.}, title = {Test of nonlocal energy alteration between two quantum memories}, volume = {134}, year = {2025}, }
• (2025). Dynamical formation of multiple quantum droplets in a bose-bose mixture. PRL, 134(9), 093401. (www)

  @article{ , abstract = {We report on the formation of multiple quantum droplets in a heteronuclear mixture released in an optical waveguide. By a sudden change of the interspecies interaction from the noninteracting to the strongly attractive regime, we initially form a single droplet in an excited compression-elongation mode. The latter axially expands up to a critical length and then splits into two or more smaller fragments, recognizable as quantum droplets. We find that the number of formed droplets increases with decreasing interspecies attraction and increasing atom number. We show, by combining theory and experiment, that this behavior is consistent with capillary instability, which causes the breakup of the stretching droplet due to the surface tension. Our results open new possibilities to explore the properties of quantum liquids and systems of multiple quantum droplets in two-component bosonic mixtures.}, archive = {J_PRL}, author = {L. Cavicchioli and C. Fort and F. Ancilotto and M. Modugno and F. Minardi and A. Burchianti}, doi = {10.1103/PhysRevLett.134.093401}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093401}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical formation of multiple quantum droplets in a bose-bose mixture}, volume = {134}, year = {2025}, }
• (2025). Spin-polarized photoelectrons in the vicinity of spectral features. PRL, 134(9), 093202. (www)

  @article{ , abstract = {It has been shown by Fano [1] that photoionization of a cesium atom by a laser pulse tuned to the vicinity of a Cooper minimum generates spin-polarized electrons. Here we show that while photoionization of rare gases does not provide large spin polarization in the vicinity of the Cooper minimum, the Fano resonances yield much higher overall spin polarization ( ≥ 40 % ) . The spin polarization increases in angle-resolved photoelectron spectra, and reaches 100% when measured in coincidence with the photoion. A common feature of both Cooper minima and Fano resonances, is the large variation of the photoinization cross section over photon energy, which proves to be vital for efficient generation of spin-polarized electrons. We provide a general framework for achieving spin polarization in photoionization irrespective of the ionization regime.}, archive = {J_PRL}, author = {Stefanos Carlström and Rezvan Tahouri and Asimina Papoulia and Jan Marcus Dahlström and Misha Yu Ivanov and Olga Smirnova and Serguei Patchkovskii}, doi = {10.1103/PhysRevLett.134.093202}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093202}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-polarized photoelectrons in the vicinity of spectral features}, volume = {134}, year = {2025}, }
• (2025). Exploring the dynamical interplay between mass-energy equivalence, interactions, and entanglement in an optical lattice clock. PRL, 134(9), 093201. (www)

  @article{ , abstract = {We propose protocols that probe manifestations of the mass-energy equivalence in an optical lattice clock interrogated with spin coherent and entangled quantum states. To tune and uniquely distinguish the mass-energy equivalence effects (gravitational redshift and second-order Doppler shift) in such a setting, we devise a dressing protocol using an additional nuclear spin state. We then analyze the dynamical interplay between photon-mediated interactions and gravitational redshift and show that such interplay can lead to entanglement generation and frequency synchronization dynamics. In the regime where all atomic spins synchronize, we show the synchronization time depends on the initial entanglement of the state and can be used as a proxy of its metrological gain compared to a classical state. Our work opens new possibilities for exploring the effects of general relativity on quantum coherence and entanglement in optical lattice clock experiments.}, archive = {J_PRL}, author = {Anjun Chu and Victor J. Martínez-Lahuerta and Maya Miklos and Kyungtae Kim and Peter Zoller and Klemens Hammerer and Jun Ye and Ana Maria Rey}, doi = {10.1103/PhysRevLett.134.093201}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093201}, shortjournal = {Phys. Rev. Lett.}, title = {Exploring the dynamical interplay between mass-energy equivalence, interactions, and entanglement in an optical lattice clock}, volume = {134}, year = {2025}, }
• (2025). Smallness of the nuclear polarization effect in the hyperfine structure of heavy muonic atoms as a stimulus for next-generation experiments. PRL, 134(9), 093003. (www)

  @article{ , abstract = {There is renewed interest in studies of muonic atoms, which may provide detailed information on nuclear structure. A major limiting factor in the interpretation of measurements is the nuclear polarization contribution. We propose a method to determine this contribution to the hyperfine structure in muonic atoms from a combination of theory and experiment for hydrogenlike ions and muonic atoms. Applying the method to and , for which there are H-like ion and muonic atom hyperfine experimental data, we find that the nuclear polarization contribution for these systems is small and place a limit on its size of less than 10% the total hyperfine splitting. We have also performed direct calculations of the nuclear polarization contribution using a semianalytical model, which indicate that it may be as much as two orders of magnitude smaller. Therefore, the nuclear polarization correction to the hyperfine structure of muonic atoms does not represent a limiting factor for next-generation experiments.}, archive = {J_PRL}, author = {J. Vandeleur and G. Sanamyan and O. R. Smits and I. A. Valuev and N. S. Oreshkina and J. S. M. Ginges}, doi = {10.1103/PhysRevLett.134.093003}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093003}, shortjournal = {Phys. Rev. Lett.}, title = {Smallness of the nuclear polarization effect in the hyperfine structure of heavy muonic atoms as a stimulus for next-generation experiments}, volume = {134}, year = {2025}, }
• (2025). Sequential synchronous mechanism for double-electron capture: Insights into unforeseen large cross sections in low-energy Sn3++H2 collisions. PRL, 134(9), 093002. (www)

  @article{ , abstract = {Remarkably large double electron capture cross sections, on the scale of , are observed in low-energy ( ) collisions between and . Given that the reaction is energetically highly unfavorable, one would expect negligibly small cross sections. Through the propagation of vibrational wave packets on coupled multiple potential energy surfaces, a novel charge transfer mechanism, driven in tandem by ion motion and molecular vibration, is revealed, offering insights into the unusual energy dependence of the measured cross sections.}, archive = {J_PRL}, author = {Lamberto Oltra and Luis Méndez and Ismanuel Rabadán and Klaas Bijlsma and Emiel de Wit and Ronnie Hoekstra}, doi = {10.1103/PhysRevLett.134.093002}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093002}, shortjournal = {Phys. Rev. Lett.}, title = {Sequential synchronous mechanism for double-electron capture: Insights into unforeseen large cross sections in low-energy Sn3++H2 collisions}, volume = {134}, year = {2025}, }
• (2025). Turning on the fluorescence from isolated GFP chromophore anions at cryogenic temperatures. PRL, 134(9), 093001. (www)

  @article{ , abstract = {The chromophore anion derived from the green fluorescent protein is one of the best-studied chromophores in the gas phase, but attempts to measure fluorescence have failed at room temperature. Here we unequivocally show that the chromophore exhibits fluorescence in the gas phase when cooled to low temperatures ( ), thereby validating previous hypotheses. The experimental confirmation is enabled by a unique mass-spectroscopy setup, allowing for fluorescence observation near or at the 0-0 transition without inducing heat in the ions upon photon absorption. The low-temperature conditions effectively simulate the restricted motion experienced within the protein, inhibiting internal conversion via a conical intersection along a twist motion coordinate. Fluorescence-excitation experiments at 100 K reveal an absorption-band maximum at , while the dispersed fluorescence spectrum shows maximum emission at . Remarkably, both values closely resemble those for proteins cooled to 77 K. We estimate that after excitation at the band maximum, radiation is the only pathway back to the ground state. Franck-Condon simulations at the level of theory nicely reproduce the experimental spectra and identify the fluorescent form to be planar, and that an in-plane scissoring mode ( ) is active for both absorption and emission.}, archive = {J_PRL}, author = {Thomas Toft Lindkvist and Iden Djavani-Tabrizi and Lars Henrik Andersen and Steen Brøndsted Nielsen}, doi = {10.1103/PhysRevLett.134.093001}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {093001}, shortjournal = {Phys. Rev. Lett.}, title = {Turning on the fluorescence from isolated GFP chromophore anions at cryogenic temperatures}, volume = {134}, year = {2025}, }
• (2025). Increasing octupole collectivity across the z=64 isotopic chain: B(E3) values in gd150. PRL, 134(9), 092501. (www)

  @article{ , abstract = {An enhanced electric octupole (E3) strength of 45(5) W.u. has been measured for the transition in , providing direct evidence for large octupole collectivity in this nucleus. The value was determined following two sensitive experiments, to measure the mean lifetime of the level and the weak decay branch direct to the ground state. The systematics of the strength across the Gd isotopic chain reveals that enhanced octupole collectivity is obtained for . The increasing low-lying octupole strength in the Gd isotopes is analyzed with five state-of-the-art theoretical models. It is found to be best reproduced by quasiparticle random phase approximation calculations, providing a good understanding of octupole collectivity in the rare-earth region.}, archive = {J_PRL}, author = {S. Pascu and E. Yüksel and Abhishek and P. Stevenson and G. H. Bhat and R. N. Mao and K. Nomura and C. Costache and Z. P. Li and N. Mărginean and C. Mihai and T. Naz and Zs. Podolyák and P. H. Regan and A. E. Turturică and R. Borcea and M. Boromiza and D. Bucurescu and S. Călinescu and C. Clisu and A. Coman and I. Dinescu and S. Doshi and D. Filipescu and N. M. Florea and A. Gandhi and I. Gheorghe and A. Ionescu and R. Lică and R. Mărginean and R. E. Mihai and A. Mitu and N. Nazir and A. Negret and C. R. Niţă and E. B. O’Sullivan and C. Petrone and S. E. Poulton and J. A. Sheikh and H. K. Singh and L. Stan and S. Toma and G. Turturică and S. Ujeniuc}, doi = {10.1103/PhysRevLett.134.092501}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {092501}, shortjournal = {Phys. Rev. Lett.}, title = {Increasing octupole collectivity across the z=64 isotopic chain: B(E3) values in gd150}, volume = {134}, year = {2025}, }
• (2025). Next-to-leading-order weak-annihilation correction to rare B→{K,π}ℓ+ℓ− decays. PRL, 134(9), 091901. (www)

  @article{ , abstract = {We accomplish for the first time the next-to-leading-order computation of the weak annihilation contribution to the electroweak penguin decays , which is an essential missing piece of the complete QCD correction to the matrix elements of hadronic operators in the weak effective Hamiltonian. Both the hard functions and the jet functions in the perturbative factorization formulas from the short-distance fluctuations at the two distinct scales and are determined at . We then demonstrate that the one-loop weak annihilation correction can bring about the noticeable impacts on theory predictions for the asymmetries and the isospin asymmetry in the decays.}, archive = {J_PRL}, author = {Yong-Kang Huang and Yue-Long Shen and Chao Wang and Yu-Ming Wang}, doi = {10.1103/PhysRevLett.134.091901}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {091901}, shortjournal = {Phys. Rev. Lett.}, title = {Next-to-leading-order weak-annihilation correction to rare B→{K,π}ℓ+ℓ− decays}, volume = {134}, year = {2025}, }
• (2025). Measurement of atmospheric neutrino oscillation parameters using convolutional neural networks with 9.3 years of data in IceCube DeepCore. PRL, 134(9), 091801. (www)

  @article{ , abstract = {The DeepCore subdetector of the IceCube Neutrino Observatory provides access to neutrinos with energies above approximately 5 GeV. Data taken between 2012 and 2021 (3387 days) are utilized for an atmospheric ν μ disappearance analysis that studied 150 257 neutrino-candidate events with reconstructed energies between 5 and 100 GeV. An advanced reconstruction based on a convolutional neural network is applied, providing increased signal efficiency and background suppression, resulting in a measurement with both significantly increased statistics compared to previous DeepCore oscillation results and high neutrino purity. For the normal neutrino mass ordering, the atmospheric neutrino oscillation parameters and their 1 σ errors are measured to be Δ m 32 2 = 2.40 − 0.04 + 0.05 × 10 − 3 eV 2 and sin 2 θ 23 = 0.54 − 0.03 + 0.04 . The results are the most precise to date using atmospheric neutrinos, and are compatible with measurements from other neutrino detectors including long-baseline accelerator experiments.}, archive = {J_PRL}, author = {IceCube Collaboration and R. Abbasi and M. Ackermann and J. Adams and S. K. Agarwalla and J. A. Aguilar and M. Ahlers and J. M. Alameddine and N. M. Amin and K. Andeen and G. Anton and C. Argüelles and Y. Ashida and S. Athanasiadou and L. Ausborm and S. N. Axani and X. Bai and A. Balagopal V and M. Baricevic and S. W. Barwick and S. Bash and V. Basu and R. Bay and J. J. Beatty and J. Becker Tjus and J. Beise and C. Bellenghi and C. Benning and S. BenZvi and D. Berley and E. Bernardini and D. Z. Besson and E. Blaufuss and L. Bloom and S. Blot and F. Bontempo and J. Y. Book Motzkin and C. Boscolo Meneguolo and S. Böser and O. Botner and J. Böttcher and E. Bourbeau and J. Braun and B. Brinson and J. Brostean-Kaiser and L. Brusa and R. T. Burley and D. Butterfield and M. A. Campana and I. Caracas and K. Carloni and J. Carpio and S. Chattopadhyay and N. Chau and Z. Chen and D. Chirkin and S. Choi and B. A. Clark and A. Coleman and G. H. Collin and A. Connolly and J. M. Conrad and P. Coppin and R. Corley and P. Correa and D. F. Cowen and P. Dave and C. De Clercq and J. J. DeLaunay and D. Delgado and S. Deng and A. Desai and P. Desiati and K. D. de Vries and G. de Wasseige and T. DeYoung and A. Diaz and J. C. Díaz-Vélez and P. Dierichs and M. Dittmer and A. Domi and L. Draper and H. Dujmovic and K. Dutta and M. A. DuVernois and T. Ehrhardt and L. Eidenschink and A. Eimer and P. Eller and E. Ellinger and S. El Mentawi and D. Elsässer and R. Engel and H. Erpenbeck and J. Evans and P. A. Evenson and K. L. Fan and K. Fang and K. Farrag and A. R. Fazely and A. Fedynitch and N. Feigl and S. Fiedlschuster and C. Finley and L. Fischer and D. Fox and A. Franckowiak and S. Fukami and P. Fürst and J. Gallagher and E. Ganster and A. Garcia and M. Garcia and G. Garg and E. Genton and L. Gerhardt and A. Ghadimi and C. Girard-Carillo and C. Glaser and T. Glüsenkamp and J. G. Gonzalez and S. Goswami and A. Granados and D. Grant and S. J. Gray and O. Gries and S. Griffin and S. Griswold and K. M. Groth and C. Günther and P. Gutjahr and C. Ha and C. Haack and A. Hallgren and L. Halve and F. Halzen and H. Hamdaoui and M. Ha Minh and M. Handt and K. Hanson and J. Hardin and A. A. Harnisch and P. Hatch and A. Haungs and J. Häußler and K. Helbing and J. Hellrung and J. Hermannsgabner and L. Heuermann and N. Heyer and S. Hickford and A. Hidvegi and J. Hignight and C. Hill and G. C. Hill and K. D. Hoffman and S. Hori and K. Hoshina and M. Hostert and W. Hou and T. Huber and K. Hultqvist and M. Hünnefeld and R. Hussain and K. Hymon and A. Ishihara and W. Iwakiri and M. Jacquart and O. Janik and M. Jansson and G. S. Japaridze and M. Jeong and M. Jin and B. J. P. Jones and N. Kamp and D. Kang and W. Kang and X. Kang and A. Kappes and D. Kappesser and L. Kardum and T. Karg and M. Karl and A. Karle and A. Katil and U. Katz and M. Kauer and J. L. Kelley and M. Khanal and A. Khatee Zathul and A. Kheirandish and J. Kiryluk and S. R. Klein and A. Kochocki and R. Koirala and H. Kolanoski and T. Kontrimas and L. Köpke and C. Kopper and D. J. Koskinen and P. Koundal and M. Kovacevich and M. Kowalski and T. Kozynets and J. Krishnamoorthi and K. Kruiswijk and E. Krupczak and A. Kumar and E. Kun and N. Kurahashi and N. Lad and C. Lagunas Gualda and M. Lamoureux and M. J. Larson and S. Latseva and F. Lauber and J. P. Lazar and J. W. Lee and K. Leonard DeHolton and A. Leszczyńska and J. Liao and M. Lincetto and Y. T. Liu and M. Liubarska and E. Lohfink and C. Love and C. J. Lozano Mariscal and L. Lu and F. Lucarelli and W. Luszczak and Y. Lyu and W. Y. Ma and J. Madsen and E. Magnus and K. B. M. Mahn and Y. Makino and E. Manao and S. Mancina and W. Marie Sainte and I. C. Mariş and S. Marka and Z. Marka and M. Marsee and I. Martinez-Soler and R. Maruyama and F. Mayhew and F. McNally and J. V. Mead and K. Meagher and S. Mechbal and A. Medina and M. Meier and Y. Merckx and L. Merten and J. Micallef and J. Mitchell and T. Montaruli and R. W. Moore and Y. Morii and R. Morse and M. Moulai and T. Mukherjee and R. Naab and R. Nagai and M. Nakos and U. Naumann and J. Necker and A. Negi and L. Neste and M. Neumann and H. Niederhausen and M. U. Nisa and K. Noda and A. Noell and A. Novikov and A. Obertacke Pollmann and V. O’Dell and B. Oeyen and A. Olivas and R. Orsoe and J. Osborn and E. O’Sullivan and H. Pandya and N. Park and G. K. Parker and E. N. Paudel and L. Paul and C. Pérez de los Heros and T. Pernice and J. Peterson and S. Philippen and A. Pizzuto and M. Plum and A. Pontén and Y. Popovych and M. Prado Rodriguez and B. Pries and R. Procter-Murphy and G. T. Przybylski and C. Raab and J. Rack-Helleis and M. Ravn and K. Rawlins and Z. Rechav and A. Rehman and P. Reichherzer and E. Resconi and S. Reusch and W. Rhode and B. Riedel and A. Rifaie and E. J. Roberts and S. Robertson and S. Rodan and G. Roellinghoff and M. Rongen and A. Rosted and C. Rott and T. Ruhe and L. Ruohan and D. Ryckbosch and I. Safa and J. Saffer and D. Salazar-Gallegos and P. Sampathkumar and A. Sandrock and M. Santander and S. Sarkar and J. Savelberg and P. Savina and P. Schaile and M. Schaufel and H. Schieler and S. Schindler and B. Schlüter and F. Schlüter and N. Schmeisser and T. Schmidt and J. Schneider and F. G. Schröder and L. Schumacher and S. Sclafani and D. Seckel and M. Seikh and M. Seo and S. Seunarine and P. Sevle Myhr and R. Shah and S. Shefali and N. Shimizu and M. Silva and B. Skrzypek and B. Smithers and R. Snihur and J. Soedingrekso and A. Søgaard and D. Soldin and P. Soldin and G. Sommani and C. Spannfellner and G. M. Spiczak and C. Spiering and M. Stamatikos and T. Stanev and T. Stezelberger and T. Stürwald and T. Stuttard and G. W. Sullivan and I. Taboada and S. Ter-Antonyan and A. Terliuk and M. Thiesmeyer and W. G. Thompson and J. Thwaites and S. Tilav and K. Tollefson and C. Tönnis and S. Toscano and D. Tosi and A. Trettin and R. Turcotte and J. P. Twagirayezu and M. A. Unland Elorrieta and A. K. Upadhyay and K. Upshaw and A. Vaidyanathan and N. Valtonen-Mattila and J. Vandenbroucke and N. van Eijndhoven and D. Vannerom and J. van Santen and J. Vara and J. Veitch-Michaelis and M. Venugopal and M. Vereecken and S. Verpoest and D. Veske and A. Vijai and C. Walck and A. Wang and C. Weaver and P. Weigel and A. Weindl and J. Weldert and A. Y. Wen and C. Wendt and J. Werthebach and M. Weyrauch and N. Whitehorn and C. H. Wiebusch and D. R. Williams and J. Willison and L. Witthaus and A. Wolf and M. Wolf and G. Wrede and X. W. Xu and J. P. Yanez and E. Yildizci and S. Yoshida and R. Young and S. Yu and T. Yuan and Z. Zhang and P. Zhelnin and P. Zilberman and M. Zimmerman}, doi = {10.1103/PhysRevLett.134.091801}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {091801}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of atmospheric neutrino oscillation parameters using convolutional neural networks with 9.3 years of data in IceCube DeepCore}, volume = {134}, year = {2025}, }
• (2025). Dissipation and decay of three-dimensional holographic quantum turbulence. PRL, 134(9), 091603. (www)

  @article{ , abstract = {Quantum turbulence is a far-from-equilibrium process characterized by high nonlinearity. Holographic duality provides a systematic framework for simulating the decaying ( 3 + 1 )-dimensional quantum turbulence by numerically solving the dual Abelian-Higgs theory in a ( 4 + 1 )-dimensional black hole background. We reveal that different types of decay behavior of the total vortex line density L emerge depending on the initial vortex line density, ranging from L ∼ t − 1.5 to L ∼ t − 1 , similar to the experimental observation of He 3 in Bradley et al. [ Phys. Rev. Lett. 96 , 035301 (2006) ], and of He 4 in Stalp et al. [ Phys. Rev. Lett. 82 , 4831 (1999) ] and in Walmsley and Golov [ Phys. Rev. Lett. 118 , 134501 (2017) ]. Furthermore, by measuring the energy flux at the black hole horizon, we determine that the energy dissipation rate d E / d t is proportional to the square of the total vortex line density, consistent with the vortex line decay equation proposed by W. F. Vinen and also the experimental measurement in Nat. Phys. 7 , 473 (2011) .}, archive = {J_PRL}, author = {Hua-Bi Zeng and Chuan-Yin Xia and Wei-Can Yang and Yu Tian and Makoto Tsubota}, doi = {10.1103/PhysRevLett.134.091603}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {091603}, shortjournal = {Phys. Rev. Lett.}, title = {Dissipation and decay of three-dimensional holographic quantum turbulence}, volume = {134}, year = {2025}, }
• (2025). Holographic correlators with bogomol’nyi-prasad-sommerfield bound states in n=4 supersymmetric yang-mills theory. PRL, 134(9), 091602. (www)

  @article{ , abstract = {We compute four-point correlators in super-Yang-Mills theory with both single and double-particle -Bogomol’nyi-Prasad-Sommerfield (BPS) operators in the regime of large ’t Hooft coupling and large . In particular, we give explicit expressions up to for the lightest correlator with two double-particle and two single-particle operators built out of the stress-tensor multiplet. Our derivation makes use of the general holographic prescription applied to an asymptotically geometry that describes a coherent superposition of multigraviton operators. The final result can be written in terms of a natural generalization of the standard functions and takes a compact form in Mellin space. The correlator we compute here is the simplest of a more general class of correlators where two inserted operators are multiparticles. These can be derived with the same approach, suggesting that the structure found here is general.}, archive = {J_PRL}, author = {Francesco Aprile and Stefano Giusto and Rodolfo Russo}, doi = {10.1103/PhysRevLett.134.091602}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {091602}, shortjournal = {Phys. Rev. Lett.}, title = {Holographic correlators with bogomol’nyi-prasad-sommerfield bound states in n=4 supersymmetric yang-mills theory}, volume = {134}, year = {2025}, }
• (2025). Fundamental physics with the lyman-alpha forest: Constraints on the growth of structure and neutrino masses from SDSS with effective field theory. PRL, 134(9), 091001. (www)

  @article{ , abstract = {We present an effective field theory (EFT) approach to extract fundamental cosmological parameters from the Lyman-alpha forest flux fluctuations as an alternative to the standard simulation-based techniques. As a first application, we reanalyze the publicly available one-dimensional Lyman-alpha flux power spectrum data from the Sloan Digital Sky Survey. Our analysis relies on informative priors on EFT parameters that we extract from a combination of public hydrodynamic simulation and emulator data. Assuming the concordance cosmological model, our one-parameter analysis yields a 2% measurement of the late time mass fluctuation amplitude σ 8 = 0.841 ± 0.017 , or equivalently, the structure growth parameter S 8 = 0.852 ± 0.017 , consistent with the standard cosmology. This result is obtained assuming that nonlinear EFT parameters are cosmology-independent functions of the linear bias parameter. When this assumption is loosened, the limit degrades by a factor of 3, suggesting that informative priors are necessary for competitive constraints. Combining our EFT likelihood with Planck + baryon acoustic oscillation data, we find a new constraint on the total neutrino mass, ∑ m ν < 0.08 eV (at 95% CL). Our study defines priorities for the development of EFT methods and sets the benchmark for cosmological analyses of the Lyman-alpha forest data from the Dark Energy Spectroscopic Instrument.}, archive = {J_PRL}, author = {Mikhail M. Ivanov and Michael W. Toomey and Naim Göksel Karaçayl𝚤}, doi = {10.1103/PhysRevLett.134.091001}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {091001}, shortjournal = {Phys. Rev. Lett.}, title = {Fundamental physics with the lyman-alpha forest: Constraints on the growth of structure and neutrino masses from SDSS with effective field theory}, volume = {134}, year = {2025}, }
• (2025). Semidefinite relaxations for high-dimensional entanglement in the steering scenario. PRL, 134(9), 090802. (www)

  @article{ , abstract = {We introduce semidefinite programming hierarchies for benchmarking relevant entanglement properties in the high-dimensional steering scenario. Firstly, we provide a general method for detecting the entanglement dimensionality through certification of the Schmidt number. Its key feature is that the computational cost is independent of the Schmidt number under consideration. Secondly, we provide a method to estimate the fidelity of the source with any maximally entangled state. Using only basic computational means, we demonstrate the usefulness of these methods, which can be directly used to analyze experiments on high-dimensional systems.}, archive = {J_PRL}, author = {Nicola D’Alessandro and Carles Roch i Carceller and Armin Tavakoli}, doi = {10.1103/PhysRevLett.134.090802}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090802}, shortjournal = {Phys. Rev. Lett.}, title = {Semidefinite relaxations for high-dimensional entanglement in the steering scenario}, volume = {134}, year = {2025}, }
• (2025). Stability of classical shadows under gate-dependent noise. PRL, 134(9), 090801. (www)

  @article{ , abstract = {Expectation values of observables are routinely estimated using so-called classical shadows—the outcomes of randomized bases measurements on a repeatedly prepared quantum state. In order to trust the accuracy of shadow estimation in practice, it is crucial to understand the behavior of the estimators under realistic noise. In this Letter, we prove that any shadow estimation protocol involving Clifford unitaries is stable under gate-dependent noise for observables with bounded stabilizer norm —originally introduced in the context of simulating Clifford circuits. In contrast, we demonstrate with concrete examples that estimation of “magic” observables can lead to highly misleading results in the presence of miscalibration errors and a worst case bias scaling exponentially in the system size. We further find that so-called robust shadows , aiming at mitigating noise, can introduce a large bias in the presence of gate-dependent noise compared to unmitigated classical shadows. Nevertheless, we guarantee the functioning of robust shadows for a more general noise setting than in previous works. On a technical level, we identify average noise channels that affect shadow estimators and allow for a more fine-grained control of noise-induced biases.}, archive = {J_PRL}, author = {Raphael Brieger and Markus Heinrich and Ingo Roth and Martin Kliesch}, doi = {10.1103/PhysRevLett.134.090801}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090801}, shortjournal = {Phys. Rev. Lett.}, title = {Stability of classical shadows under gate-dependent noise}, volume = {134}, year = {2025}, }
• (2025). Low-cost noise reduction for clifford circuits. PRL, 134(9), 090603. (www)

  @article{ , abstract = {We propose a Clifford noise reduction (CliNR) scheme that provides a reduction of the logical error rate of Clifford circuit with lower overhead than error correction and without the exponential sampling overhead of error mitigation. CliNR implements Clifford circuits by splitting them into subcircuits that are performed using gate teleportation. A few random stabilizer measurements are used to detect errors in the resources states consumed by the gate teleportation. This can be seen as a teleported version of the coherent parity-check scheme [1–3], with offline fault-detection making it scalable. We prove that CliNR achieves a vanishing logical error rate for families of n -qubit Clifford circuits with size s such that n s p 2 goes to 0, where p is the physical error rate, meaning that it reaches the regime n s = o ( 1 / p 2 ) , whereas the direct implementation is limited to s = o ( 1 / p ) . Moreover, CliNR uses only 3 n + 1 qubits, 2 s + o ( s ) gates and has zero rejection rate. This small overhead makes it more practical than quantum error correction in the near term and our numerical simulations show that CliNR provides a reduction of the logical error rate in relevant noise regimes.}, archive = {J_PRL}, author = {Nicolas Delfosse and Edwin Tham}, doi = {10.1103/PhysRevLett.134.090603}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090603}, shortjournal = {Phys. Rev. Lett.}, title = {Low-cost noise reduction for clifford circuits}, volume = {134}, year = {2025}, }
• (2025). Lowering connectivity requirements for bivariate bicycle codes using morphing circuits. PRL, 134(9), 090602. (www)

  @article{ , abstract = {In reference Bravyi et al. , [ Nature (London) 627 , 778 (2024) ], Bravyi et al. found examples of bivariate bicycle (BB) codes with similar logical performance to the surface code but with an improved encoding rate. In this work, we generalize a novel parity-check circuit design principle called morphing circuits and apply it to BB codes. We define a new family of BB codes whose parity check circuits require a qubit connectivity of degree five instead of six while maintaining their numerical performance. Logical input or output to an ancillary surface code is also possible in a biplanar layout. Finally, we develop a general framework for designing morphing circuits and present a sufficient condition for its applicability to two-block group algebra codes.}, archive = {J_PRL}, author = {Mackenzie H. Shaw and Barbara M. Terhal}, doi = {10.1103/PhysRevLett.134.090602}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090602}, shortjournal = {Phys. Rev. Lett.}, title = {Lowering connectivity requirements for bivariate bicycle codes using morphing circuits}, volume = {134}, year = {2025}, }
• (2025). Establishing a new benchmark in quantum computational advantage with 105-qubit zuchongzhi 3.0 processor. PRL, 134(9), 090601. (www)

  @article{ , abstract = {In the relentless pursuit of quantum computational advantage, we present a significant advancement with the development of Zuchongzhi 3.0. This superconducting quantum computer prototype, comprising 105 qubits, achieves high operational fidelities, with single-qubit gates, two-qubit gates, and readout fidelity at 99.90%, 99.62%, and 99.13%, respectively. Our experiments with an 83-qubit, 32-cycle random circuit sampling on the Zuchongzhi 3.0 highlight its superior performance, achieving samples in just a few hundred seconds. This task is estimated to be infeasible on the most powerful classical supercomputers, Frontier, which would require approximately to replicate the task. This leap in processing power places the classical simulation cost 6 orders of magnitude beyond Google’s SYC-67 and SYC-70 experiments [Morvan et al. , Nature 634 , 328 (2024) ], firmly establishing a new benchmark in quantum computational advantage. Our work not only advances the frontiers of quantum computing but also lays the groundwork for a new era where quantum processors play an essential role in tackling sophisticated real-world challenges.}, archive = {J_PRL}, author = {Dongxin Gao and Daojin Fan and Chen Zha and Jiahao Bei and Guoqing Cai and Jianbin Cai and Sirui Cao and Fusheng Chen and Jiang Chen and Kefu Chen and Xiawei Chen and Xiqing Chen and Zhe Chen and Zhiyuan Chen and Zihua Chen and Wenhao Chu and Hui Deng and Zhibin Deng and Pei Ding and Xun Ding and Zhuzhengqi Ding and Shuai Dong and Yupeng Dong and Bo Fan and Yuanhao Fu and Song Gao and Lei Ge and Ming Gong and Jiacheng Gui and Cheng Guo and Shaojun Guo and Xiaoyang Guo and Lianchen Han and Tan He and Linyin Hong and Yisen Hu and He-Liang Huang and Yong-Heng Huo and Tao Jiang and Zuokai Jiang and Honghong Jin and Yunxiang Leng and Dayu Li and Dongdong Li and Fangyu Li and Jiaqi Li and Jinjin Li and Junyan Li and Junyun Li and Na Li and Shaowei Li and Wei Li and Yuhuai Li and Yuan Li and Futian Liang and Xuelian Liang and Nanxing Liao and Jin Lin and Weiping Lin and Dailin Liu and Hongxiu Liu and Maliang Liu and Xinyu Liu and Xuemeng Liu and Yancheng Liu and Haoxin Lou and Yuwei Ma and Lingxin Meng and Hao Mou and Kailiang Nan and Binghan Nie and Meijuan Nie and Jie Ning and Le Niu and Wenyi Peng and Haoran Qian and Hao Rong and Tao Rong and Huiyan Shen and Qiong Shen and Hong Su and Feifan Su and Chenyin Sun and Liangchao Sun and Tianzuo Sun and Yingxiu Sun and Yimeng Tan and Jun Tan and Longyue Tang and Wenbing Tu and Cai Wan and Jiafei Wang and Biao Wang and Chang Wang and Chen Wang and Chu Wang and Jian Wang and Liangyuan Wang and Rui Wang and Shengtao Wang and Xiaomin Wang and Xinzhe Wang and Xunxun Wang and Yeru Wang and Zuolin Wei and Jiazhou Wei and Dachao Wu and Gang Wu and Jin Wu and Shengjie Wu and Yulin Wu and Shiyong Xie and Lianjie Xin and Yu Xu and Chun Xue and Kai Yan and Weifeng Yang and Xinpeng Yang and Yang Yang and Yangsen Ye and Zhenping Ye and Chong Ying and Jiale Yu and Qinjing Yu and Wenhu Yu and Xiangdong Zeng and Shaoyu Zhan and Feifei Zhang and Haibin Zhang and Kaili Zhang and Pan Zhang and Wen Zhang and Yiming Zhang and Yongzhuo Zhang and Lixiang Zhang and Guming Zhao and Peng Zhao and Xianhe Zhao and Xintao Zhao and Youwei Zhao and Zhong Zhao and Luyuan Zheng and Fei Zhou and Liang Zhou and Na Zhou and Naibin Zhou and Shifeng Zhou and Shuang Zhou and Zhengxiao Zhou and Chengjun Zhu and Qingling Zhu and Guihong Zou and Haonan Zou and Qiang Zhang and Chao-Yang Lu and Cheng-Zhi Peng and Xiaobo Zhu and Jian-Wei Pan}, doi = {10.1103/PhysRevLett.134.090601}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090601}, shortjournal = {Phys. Rev. Lett.}, title = {Establishing a new benchmark in quantum computational advantage with 105-qubit zuchongzhi 3.0 processor}, volume = {134}, year = {2025}, }
• (2025). Engineering nonequilibrium steady states through floquet liouvillians. PRL, 134(9), 090402. (www)

  @article{ , abstract = {We experimentally study the transient dynamics of a dissipative superconducting qubit under periodic drive toward its nonequilibrium steady states. The corresponding stroboscopic evolution, given by the qubit states at times equal to integer multiples of the drive period, is determined by a (generically non-Hermitian) Floquet Liouvillian. The drive period controls both the transients across its non-Hermitian degeneracies and the resulting nonequilibrium steady states. These steady states can exhibit higher purity compared to those achieved with a constant drive. We further study the dependence of the steady states on the direction of parameter variation and relate these findings to the recent studies of dynamically encircling exceptional points. Our Letter provides a new approach to control non-Hermiticity in dissipative quantum systems and presents a new paradigm in quantum state preparation and stabilization.}, archive = {J_PRL}, author = {Weijian Chen and Maryam Abbasi and Serra Erdamar and Jacob Muldoon and Yogesh N. Joglekar and Kater W. Murch}, doi = {10.1103/PhysRevLett.134.090402}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090402}, shortjournal = {Phys. Rev. Lett.}, title = {Engineering nonequilibrium steady states through floquet liouvillians}, volume = {134}, year = {2025}, }
• (2025). Frustration elimination and excited state search in coherent ising machines. PRL, 134(9), 090401. (www)

  @article{ , abstract = {Frustration, that is, the impossibility of satisfying the energetic preferences between all spin pairs simultaneously, underlies the complexity of many fundamental properties in spin systems, including the computational difficulty in determining their ground states. Coherent Ising machines (CIMs) have been proposed as a promising analog computational approach to efficiently find different degenerate ground states of large and complex Ising models. However, CIMs also face challenges in solving frustrated Ising models: frustration not only reduces the probability of finding good solutions, but it also prohibits the leveraging of quantum effects in doing so. To circumvent these detrimental effects of frustration, we show how frustrated Ising models can be mapped to frustration-free CIM configurations by including ancillary modes and modifying the coupling protocol used in current CIM designs. Such frustration elimination may empower current CIMs to benefit from quantum effects in dealing with frustrated Ising models. In addition, these ancillary modes can also enable error detection and searching for excited states.}, archive = {J_PRL}, author = {Zheng-Yang Zhou and Clemens Gneiting and J. Q. You and Franco Nori}, doi = {10.1103/PhysRevLett.134.090401}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090401}, shortjournal = {Phys. Rev. Lett.}, title = {Frustration elimination and excited state search in coherent ising machines}, volume = {134}, year = {2025}, }
• (2025). Computable entanglement cost under positive partial transpose operations. PRL, 134(9), 090202. (www)

  @article{ , abstract = {Quantum information theory is plagued by the problem of regularizations, which require the evaluation of formidable asymptotic quantities. This makes it computationally intractable to gain a precise quantitative understanding of the ultimate efficiency of key operational tasks such as entanglement manipulation. Here, we consider the problem of computing the asymptotic entanglement cost of preparing noisy quantum states under quantum operations with positive partial transpose (PPT). By means of an analytical example, a previously claimed solution to this problem is shown to be incorrect. Building on a previous characterization of the PPT entanglement cost in terms of a regularized formula, we construct instead a hierarchy of semidefinite programs that bypasses the issue of regularization altogether, and converges to the true asymptotic value of the entanglement cost. Our main result establishes that this convergence happens exponentially fast, thus yielding an efficient algorithm that approximates the cost up to an additive error ϵ in time poly ( D , log ( 1 / ϵ ) ) , where D is the underlying Hilbert space dimension. To our knowledge, this is the first time that an asymptotic entanglement measure is shown to be efficiently computable despite no closed-form formula being available.}, archive = {J_PRL}, author = {Ludovico Lami and Francesco Anna Mele and Bartosz Regula}, doi = {10.1103/PhysRevLett.134.090202}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090202}, shortjournal = {Phys. Rev. Lett.}, title = {Computable entanglement cost under positive partial transpose operations}, volume = {134}, year = {2025}, }
• (2025). Randomness versus nonlocality in multiple-input and multiple-output quantum scenario. PRL, 134(9), 090201. (www)

  @article{ , abstract = {Device-independent randomness certification based on Bell nonlocality does not require any assumptions about the devices, thus provides adequate security. Great effort has been made to demonstrate that nonlocality is necessary for generating quantum randomness, but the minimal resource required has not been clarified. Here we prove and experimentally demonstrate that violating any two-input Bell inequality is both necessary and sufficient for certifying randomness, however, for the multiple-input cases, this sufficiency ceases to apply, leading to certain states exhibiting Bell nonlocality without the capability to certify randomness. We examine two typical classes of Bell inequalities with multiple input and multiple output, the facet inequalities and Salavrakos-Augusiak-Tura-Wittek-Acín-Pironio inequalities, in the high-dimensional photonic system, and observe that the violation of the latter one can always certify randomness which is not true for the former. The private randomness with a generation rate of 1.867 ± 0.018 bits per photon pair is obtained in the scenario of Salavrakos-Augusiak-Tura-Wittek-Acín-Pironio inequalities with 3-input and 4-output. Our Letter unravels the internal connection between randomness and nonlocality, effectively enhancing the performance of tasks such as device-independent random number generation.}, archive = {J_PRL}, author = {Chao Zhang and Yi Li and Xiao-Min Hu and Yu Xiang and Chuan-Feng Li and Guang-Can Guo and Jordi Tura and Qihuang Gong and Qiongyi He and Bi-Heng Liu}, doi = {10.1103/PhysRevLett.134.090201}, journal = {Physical Review Letters}, month = {3}, number = {9}, pages = {090201}, shortjournal = {Phys. Rev. Lett.}, title = {Randomness versus nonlocality in multiple-input and multiple-output quantum scenario}, volume = {134}, year = {2025}, }
• (2025). Erratum: Emergent Sp(3,R) dynamical symmetry in the nuclear many-body system from an ab initio description [Phys. rev. lett. 125, 102505 (2020)]. PRL, 134(8), 089901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 089901 (2025)}, archive = {J_PRL}, author = {Anna E. McCoy and Mark A. Caprio and Tomáš Dytrych and Patrick J. Fasano}, doi = {10.1103/PhysRevLett.134.089901}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {089901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Emergent Sp(3,R) dynamical symmetry in the nuclear many-body system from an ab initio description [Phys. rev. lett. 125, 102505 (2020)]}, volume = {134}, year = {2025}, }
• (2025). Onset of intermittency and multiscaling in active turbulence. PRL, 134(8), 088302. (www)

  @article{ , abstract = {Recent results suggest that highly active, chaotic, nonequilibrium states of living fluids might share much in common with high Reynolds number, inertial turbulence. We now show, by using a hydrodynamical model, the onset of intermittency and the consequent multiscaling of Eulerian and Lagrangian structure functions as a function of the bacterial activity. Our results bridge the worlds of low and high Reynolds number flows as well as open up intriguing possibilities of what makes flows intermittent.}, archive = {J_PRL}, author = {Kolluru Venkata Kiran and Kunal Kumar and Anupam Gupta and Rahul Pandit and Samriddhi Sankar Ray}, doi = {10.1103/PhysRevLett.134.088302}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {088302}, shortjournal = {Phys. Rev. Lett.}, title = {Onset of intermittency and multiscaling in active turbulence}, volume = {134}, year = {2025}, }
• (2025). Beyond dipolar activity: Quadrupolar stress drives collapse of nematic order on frictional substrates. PRL, 134(8), 088301. (www)

  @article{ , abstract = {The field of active nematics has traditionally employed descriptions based on dipolar activity. However, it is theoretically predicted that interactions with a substrate, prevalent in most biological systems, lead to novel forms of activity, such as quadrupolar activity, that are governed by hydrodynamic screening. Here, combining experiments and numerical simulations, we show that upon light-induced solidification of the underlying medium, microtubule-kinesin mixtures undergo a transformation that leads to a biphasic active suspension. Using an active lyotropic model, we prove that the transition is governed by screening effects that alter the dominant form of active stress. Specifically, the combined effect of friction and quadrupolar activity leads to a hierarchical folding that follows the intrinsic bend instability of the active nematic layer. Our results demonstrate the dynamics of the collapse of orientational order in active nematics and present a new route for controlling active matter by modifying the activity through changing the surrounding environment.}, archive = {J_PRL}, author = {Aleksandra Ardaševa and Ignasi Vélez-Cerón and Martin Cramer Pedersen and Jordi Ignés-Mullol and Francesc Sagués and Amin Doostmohammadi}, doi = {10.1103/PhysRevLett.134.088301}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {088301}, shortjournal = {Phys. Rev. Lett.}, title = {Beyond dipolar activity: Quadrupolar stress drives collapse of nematic order on frictional substrates}, volume = {134}, year = {2025}, }
• (2025). Mediation of colloidal encounter dynamics by surface roughness. PRL, 134(8), 088201. (www)

  @article{ , abstract = {Rigorous understanding of assembly in colloidal systems is crucial to the development of tailored nanostructured materials. Despite extensive studies, a mechanistic understanding of the dynamics governing encounters of colloidal particles remains an ongoing challenge. We study colloidal encounter dynamics by inducing assembly through optical tweezers that impose an external attractive field for cubic-phase sodium yttrium fluoride nanocrystals. We show that surface roughness of the nanocrystals is a decisive factor for contact leading to assembly between the nanocrystals, manifested by the roughness-dependent hydrodynamic resistivity. This provides direct evidence that dynamics are equally important to energetics in understanding assembly.}, archive = {J_PRL}, author = {Robert G. Felsted and Jaehun Chun and Gregory K. Schenter and Alexander B. Bard and Xiaojing Xia and Peter J. Pauzauskie}, doi = {10.1103/PhysRevLett.134.088201}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {088201}, shortjournal = {Phys. Rev. Lett.}, title = {Mediation of colloidal encounter dynamics by surface roughness}, volume = {134}, year = {2025}, }
• (2025). Interface dynamics of wet active systems. PRL, 134(8), 087105. (www)

  @article{ , abstract = {We study the roughening of interfaces in phase-separated active suspensions on substrates. At both large length and time scales, we show that the interfacial dynamics belongs to the | q | KPZ universality class discussed in Besse et al. [ Phys. Rev. Lett. 130 , 187102 (2023) ]. This holds despite the presence of long-ranged fluid flows. At early times, however, or for sufficiently small systems, the roughening exponents are the same as those in the presence of a momentum-conserving fluid. Surprisingly, when the effect of substrate friction can be ignored, the interface becomes random beyond a de Gennes–Taupin length scale that depends on the interfacial tension.}, archive = {J_PRL}, author = {Fernando Caballero and Ananyo Maitra and Cesare Nardini}, doi = {10.1103/PhysRevLett.134.087105}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {087105}, shortjournal = {Phys. Rev. Lett.}, title = {Interface dynamics of wet active systems}, volume = {134}, year = {2025}, }
• (2025). Nonequilibrium relaxation inequality on short timescales. PRL, 134(8), 087104. (www)

  @article{ , abstract = {An integral relation is derived from the Fokker-Planck equation which connects the steady-state probability currents with the dynamics of relaxation on short timescales in the limit of small perturbation fields. As a consequence of this integral relation, a general lower bound on the steady-state entropy production is obtained. Two particular ensembles of perturbation fields are then considered, respectively constant gradients and density displacements, and correspondingly two different averaging-based thermodynamic bounds are derived from the integral relation. These provide feasible methods to estimate the steady-state entropy production from relaxation experiments.}, archive = {J_PRL}, author = {Andrea Auconi}, doi = {10.1103/PhysRevLett.134.087104}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {087104}, shortjournal = {Phys. Rev. Lett.}, title = {Nonequilibrium relaxation inequality on short timescales}, volume = {134}, year = {2025}, }
• (2025). Parameter inference and nonequilibrium identification for markov networks based on coarse-grained observations. PRL, 134(8), 087103. (www)

  @article{ , abstract = {Most experiments can only detect a set of coarse-grained clusters of a molecular system, while the internal microstates are often inaccessible. Here, based on an infinitely long coarse-grained trajectory, we obtain a set of sufficient statistics that extracts all statistic information of coarse-grained observations. Based on these sufficient statistics, we set up a theoretical framework of parameter inference and nonequilibrium identification for a general Markov network with an arbitrary number of microstates and arbitrary coarse-grained partitioning. Our framework can be used to identify whether the sufficient statistics are enough for empirical estimation of all unknown parameters and we can also provide a quantitative criterion that reveals nonequilibrium. Our nonequilibrium criterion generalizes the one obtained [ J. Chem. Phys. 132 , 041102 (2010) ] for a three-state system with two coarse-grained clusters and is capable of detecting a larger nonequilibrium region compared to the classical criterion based on autocorrelation functions.}, archive = {J_PRL}, author = {Bingjie Wu and Chen Jia}, doi = {10.1103/PhysRevLett.134.087103}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {087103}, shortjournal = {Phys. Rev. Lett.}, title = {Parameter inference and nonequilibrium identification for markov networks based on coarse-grained observations}, volume = {134}, year = {2025}, }
• (2025). Nonorthogonal eigenvectors, fluctuation-dissipation relations, and entropy production. PRL, 134(8), 087102. (www)

  @article{ , abstract = {Celebrated fluctuation-dissipation theorem (FDT) linking the response function to time dependent correlations of observables measured in the reference unperturbed state is one of the central results in equilibrium statistical mechanics. In this Letter we discuss an extension of the standard FDT to the case when multidimensional matrix representing transition probabilities is strictly non-normal. This feature dramatically modifies the dynamics, by incorporating the effect of eigenvector nonorthogonality via the associated overlap matrix of Chalker-Mehlig type. In particular, the rate of entropy production per unit time is strongly enhanced by that matrix. We suggest, that this mechanism has an impact on the studies of collective phenomena in neural matrix models, leading, via transient behavior, to such phenomena as synchronization and emergence of the memory. We also expect, that the described mechanism generating the entropy production is generic for wide class of phenomena, where dynamics is driven by non-normal operators. For the case of driving by a large Ginibre matrix the entropy production rate is evaluated analytically, as well as for the Rajan-Abbott model for neural networks.}, archive = {J_PRL}, author = {Yan V. Fyodorov and Ewa Gudowska-Nowak and Maciej A. Nowak and Wojciech Tarnowski}, doi = {10.1103/PhysRevLett.134.087102}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {087102}, shortjournal = {Phys. Rev. Lett.}, title = {Nonorthogonal eigenvectors, fluctuation-dissipation relations, and entropy production}, volume = {134}, year = {2025}, }
• (2025). Exponential change of relaxation rate by quenched disorder. PRL, 134(8), 087101. (www)

  @article{ , abstract = {We determine the asymptotic relaxation rate of a Brownian particle in a harmonic potential perturbed by quenched Gaussian disorder, a simplified model for rugged energy landscapes in complex systems. Depending on the properties of the disorder, we show that the mean and variance of the asymptotic relaxation rate are nonmonotonous functions of the parameters for a broad class of disorders. In particular, the rate of relaxation may either increase or decrease exponentially compared to the unperturbed case. This implies that disorder may, depending on its properties, both significantly speed up and slow down relaxation. In the limit of weak disorder, we derive the probability distribution of the asymptotic relaxation rate and show that it is Gaussian, with analytic expressions for the mean and variance that feature universal limits. Our findings indicate that controlled disorder may serve to tune the relaxation speed in complex systems.}, archive = {J_PRL}, author = {Jan Meibohm and Sabine H. L. Klapp}, doi = {10.1103/PhysRevLett.134.087101}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {087101}, shortjournal = {Phys. Rev. Lett.}, title = {Exponential change of relaxation rate by quenched disorder}, volume = {134}, year = {2025}, }
• (2025). Charge dynamics of an unconventional three-dimensional charge density wave in kagome FeGe. PRL, 134(8), 086902. (www)

  @article{ , abstract = {We report on the charge dynamics of kagome FeGe, an antiferromagnet with a charge density wave (CDW) transition at T CDW ≃ 105 K , using polarized infrared spectroscopy and band structure calculations. We reveal pronounced optical anisotropy along the a and c axis, as well as an unusual response associated with three-dimensional CDW order. Above T CDW , there is a notable transfer of spectral weight (SW) from high to low energies, promoted by the magnetic splitting-induced shift in bands. Across the CDW transition, we observe a sudden SW transfer from low to high energies over a broad range, along with the emergence of new excitations around 1200 cm − 1 . These results contrast with observations from other kagome metals like CsV 3 Sb 5 , where the nesting of VHSs leads to a clear CDW gap feature. Instead, our findings can be accounted for by a 2 × 2 × 2 CDW ground state driven by a first-order structural transition involving large partial Ge1 dimerization. Our Letter thus unveils a complex interplay among structure, magnetism, and charge order, offering valuable insights for a comprehensive understanding of CDW order in FeGe.}, archive = {J_PRL}, author = {Shaohui Yi and Zhiyu Liao and Qi Wang and Haiyang Ma and Jianpeng Liu and Xiaokun Teng and Bin Gao and Pengcheng Dai and Yaomin Dai and Jianzhou Zhao and Yanpeng Qi and Bing Xu and Xianggang Qiu}, doi = {10.1103/PhysRevLett.134.086902}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086902}, shortjournal = {Phys. Rev. Lett.}, title = {Charge dynamics of an unconventional three-dimensional charge density wave in kagome FeGe}, volume = {134}, year = {2025}, }
• (2025). Electromagnon signatures of a metastable multiferroic state. PRL, 134(8), 086706. (www)

  @article{ , abstract = {Magnetoelectric multiferroic materials, particularly type-II multiferroics where ferroelectric polarizations arise from magnetic order, offer significant potential for the simultaneous control of magnetic and electric properties. However, it remains an open question as to how the multiferroic ground states are stabilized on the free-energy landscape in the presence of intricate competition between the magnetoelectric coupling and thermal fluctuations. In this work, by using terahertz time-domain spectroscopy in combination with an applied magnetic field, photoexcitation, and single-shot detection, we reveal the spectroscopic signatures of a magnetic-field-induced metastable multiferroic state in a hexaferrite. This state remains robust until thermal influences cause the sample to revert to the original paraelectric state. Our findings shed light on the emergence of metastable multiferroicity and its interplay with thermal dynamics.}, archive = {J_PRL}, author = {Blake S. Dastrup and Zhuquan Zhang and Peter R. Miedaner and Yu-Che Chien and Young Sun and Yan Wu and Huibo Cao and Edoardo Baldini and Keith A. Nelson}, doi = {10.1103/PhysRevLett.134.086706}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086706}, shortjournal = {Phys. Rev. Lett.}, title = {Electromagnon signatures of a metastable multiferroic state}, volume = {134}, year = {2025}, }
• (2025). Four-wave mixing at peV energy scales. PRL, 134(8), 086705. (www)

  @article{ , abstract = {We measure the nonlinear magnetic susceptibility χ ( 3 ) of the disordered quantum Ising magnet LiHo 0.045 Y 0.955 F 4 and demonstrate four-wave mixing due to coherent (anti-)Stokes Raman scattering at ∼ 100 Hz (peV) energy scales. The temperature dependence of χ ( 3 ) approximately follows a ( 1 / T ) form, with a high- T cutoff that can be linked to dissipation in the coherent spin clusters. χ ( 3 ) also decreases monotonically with a transverse field, approaching a constant offset above a few kOe, suggesting the presence of both coherent and spontaneous Raman scattering.}, archive = {J_PRL}, author = {C. Simon and D. M. Silevitch and T. F. Rosenbaum}, doi = {10.1103/PhysRevLett.134.086705}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086705}, shortjournal = {Phys. Rev. Lett.}, title = {Four-wave mixing at peV energy scales}, volume = {134}, year = {2025}, }
• (2025). Real space imaging of field-driven decision-making in nanomagnetic galton boards. PRL, 134(8), 086704. (www)

  @article{ , abstract = {A possible spintronic route to hardware implementation for decision-making involves injecting a domain wall into a bifurcated magnetic nanostrip resembling a Y-shaped junction. A decision is made when the domain wall chooses a particular path through the bifurcation. Recently, it was shown that a structure like a nanomagnetic Galton board, which is essentially an array of interconnected Y-shaped junctions, produces outcomes that are stochastic and therefore relevant to artificial neural networks. However, the exact mechanism leading to the robust nature of randomness is unknown. Here, we directly image the decision-making process in nanomagnetic Galton boards using Lorentz transmission electron microscopy. We identify that the stochasticity in nanomagnetic Galton boards arises as a culmination of (1) the topology of the injected domain wall, (2) dissimilarly sized vertices, and (3) the strength of the applied field. Our results pave the way to a detailed understanding of stochasticity in nanomagnetic networks.}, archive = {J_PRL}, author = {H. Arava and D. Sanz-Hernandez and J. Grollier and A. K. Petford-Long}, doi = {10.1103/PhysRevLett.134.086704}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086704}, shortjournal = {Phys. Rev. Lett.}, title = {Real space imaging of field-driven decision-making in nanomagnetic galton boards}, volume = {134}, year = {2025}, }
• (2025). Magnetic lyddane-sachs-teller relation. PRL, 134(8), 086703. (www)

  @article{ , abstract = {We describe a magnetic relation in analogy to the well-known dielectric Lyddane-Sachs-Teller relation [R. H. Lyddane et al. , Phys. Rev. 59 , 673 (1941) ]. This magnetic relation follows directly from the model equations for nuclear induction due to fast oscillating electromagnetic fields [F. Bloch, Phys. Rev. 70 , 460 (1946) ] and relates the static permeability with the product over all ratios of antiresonance and resonance frequencies associated with all magnetic excitations within a given specimen. The magnetic relation differs significantly from its dielectric analog where the static properties are related to ratios of the squares of resonance frequencies. We demonstrate the validity of the magnetic Lyddane-Sachs-Teller relation using optical magnetization data from terahertz electron magnetic resonance spectroscopic ellipsometry measurements in the presence of an external magnetic field on an iron-doped semiconductor crystal of gallium nitride.}, archive = {J_PRL}, author = {Viktor Rindert and Vanya Darakchieva and Tapati Sarkar and Mathias Schubert}, doi = {10.1103/PhysRevLett.134.086703}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086703}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic lyddane-sachs-teller relation}, volume = {134}, year = {2025}, }
• (2025). Spin-peierls transition in the frustrated spinels ZnCr2O4 and MgCr2O4. PRL, 134(8), 086702. (www)

  @article{ , abstract = {The chromium spinels and are prime examples of the highly frustrated pyrochlore lattice antiferromagnet. Experiment has carefully established that both materials, upon cooling, distort to lower symmetry and order magnetically. We study the nature of this process by a combination of density-functional-theory–based energy mapping and classical Monte Carlo simulations. We first computationally establish precise Heisenberg Hamiltonian parameters for the high temperature cubic and the low temperature tetragonal and orthorhombic structures of both spinels. We then investigate the respective ordering temperatures of high symmetry and low symmetry structures. We carefully compare our results with experimental facts and find that our simulations are remarkably consistent with a type of spin-Peierls mechanism, adapted to three dimensions, where the structural distortion is mediated by a magnetic energy gain due to a lower degree of frustration.}, archive = {J_PRL}, author = {Ludovic D. C. Jaubert and Yasir Iqbal and Harald O. Jeschke}, doi = {10.1103/PhysRevLett.134.086702}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086702}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-peierls transition in the frustrated spinels ZnCr2O4 and MgCr2O4}, volume = {134}, year = {2025}, }
• (2025). Giant strain-induced spin splitting effect in MnTe, a g-wave altermagnetic semiconductor. PRL, 134(8), 086701. (www)

  @article{ , abstract = {Hexagonal MnTe is an altermagnetic semiconductor with g -wave symmetry of spin polarization in momentum space. In the nonrelativistic limit, this symmetry mandates that electric current flowing in any crystallographic direction is unpolarized. However, here I show that elastic strain is effective in inducing the spin splitting effect in MnTe. For this analysis, a spin-orbit-coupled k · p Hamiltonian for the valence band maximum at the A point is derived and fitted to eigenvalues calculated from first principles. The spin splitting angle is calculated using the Boltzmann approach in the relaxation-time approximation. The spin splitting gauge factor exceeds 30 near the valence band maximum. Thus, with suitable substrate engineering, MnTe can be used as an efficient source and detector of spin current in spintronic devices. Proper inclusion of the Rashba-Dresselhaus spin-orbit coupling is crucial for the correct description of the transport properties of MnTe.}, archive = {J_PRL}, author = {K. D. Belashchenko}, doi = {10.1103/PhysRevLett.134.086701}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086701}, shortjournal = {Phys. Rev. Lett.}, title = {Giant strain-induced spin splitting effect in MnTe, a g-wave altermagnetic semiconductor}, volume = {134}, year = {2025}, }
• (2025). Renormalized classical spin liquid on the ruby lattice. PRL, 134(8), 086601. (www)

  @article{ , abstract = {The recent experimental detection of the onset of a dynamically prepared, gapped quantum spin liquid on the ruby lattice brought the physics of frustrated magnetism and lattice gauge theory to Rydberg tweezer arrays [Semeghini et al. , Probing topological spin liquids on a programmable quantum simulator, Science 374 , 1242 (2021) ]. The thermodynamic properties of such models remain inadequately addressed, yet knowledge thereof is indispensable if one wants to prepare large, robust, and long-lived quantum spin liquids. Using large scale quantum Monte Carlo simulations we find in the PXP model a renormalized classical spin liquid with constant entropy density approaching in the thermodynamic limit for all moderate and large values of the detuning and starting from (in units of the Rabi frequency ) down to the lowest temperatures we could simulate, . With van der Waals interactions, constant entropy plateaus are still found but its value shifts with . We comment on the implications of the adiabatic approximation to the dynamical ramps for the electric degrees of freedom, which leads to a reinterpretation of the experimental observations.}, archive = {J_PRL}, author = {Zhenjiu Wang and Lode Pollet}, doi = {10.1103/PhysRevLett.134.086601}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086601}, shortjournal = {Phys. Rev. Lett.}, title = {Renormalized classical spin liquid on the ruby lattice}, volume = {134}, year = {2025}, }
• (2025). Gauged cooling of topological excitations and emergent fermions on quantum simulators. PRL, 134(8), 086503. (www)

  @article{ , abstract = {Simulated cooling is a robust method for preparing low-energy states of many-body Hamiltonians on near-term quantum simulators. In such schemes, a subset of the simulator’s spins (or qubits) are treated as a “bath” that extracts energy and entropy from the system of interest. However, such protocols are inefficient when applied to systems whose excitations are highly nonlocal in terms of the microscopic degrees of freedom, such as topological phases of matter; such excitations are difficult to extract by a local coupling to a bath. We explore a route to overcome this obstacle by encoding the microscopic degrees of freedom into those of the quantum simulator in a nonlocal manner. To illustrate the approach, we show how to efficiently cool the ferromagnetic phase of the quantum Ising model, whose excitations are domain walls, via a “gauged cooling” protocol in which the Ising spins are coupled to a gauge field that simultaneously acts as a reservoir for removing excitations. We show that our protocol can prepare the ground states of the ferromagnetic and paramagnetic phases equally efficiently. The gauged cooling protocol naturally extends to (interacting) fermionic systems, where it is equivalent to cooling by coupling to a fermionic bath via single-fermion hopping.}, archive = {J_PRL}, author = {Gilad Kishony and Mark S. Rudner and Achim Rosch and Erez Berg}, doi = {10.1103/PhysRevLett.134.086503}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086503}, shortjournal = {Phys. Rev. Lett.}, title = {Gauged cooling of topological excitations and emergent fermions on quantum simulators}, volume = {134}, year = {2025}, }
• (2025). Orbital competition in bilayer graphene’s fractional quantum hall effect. PRL, 134(8), 086502. (www)

  @article{ , abstract = {The lowest Landau level of bilayer graphene has an octet of internal degrees of freedom, composed from spin, valley, and orbital two-level systems. Dominance of orbitals over orbitals in low energy quantum fluctuations leads to distinct fractional quantum Hall characteristics compared dominance of over . The competition between and orbitals depends sensitively on particle-hole asymmetry in the single-particle Hamiltonian and on Lamb shifts due to exchange interactions with the negative energy sea, which must be accounted for simultaneously in assessing the orbital competition. We identify the circumstances under which , which supports strong even-denominator fractional quantum Hall states with non-Abelian quasiparticles, emerges robustly as the low-energy Landau level.}, archive = {J_PRL}, author = {Bishoy M. Kousa and Nemin Wei and Allan H. MacDonald}, doi = {10.1103/PhysRevLett.134.086502}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086502}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital competition in bilayer graphene’s fractional quantum hall effect}, volume = {134}, year = {2025}, }
• (2025). Ground state of the s=1/2 heisenberg spin chain with random ferromagnetic and antiferromagnetic couplings. PRL, 134(8), 086501. (www)

  @article{ , abstract = {We study the Heisenberg S = 1 / 2 chain with random ferro- and antiferromagnetic couplings using quantum Monte Carlo simulations at ultra-low temperatures, converging to the ground state. Finite-size scaling of correlation functions and excitation gaps demonstrate an exotic critical state in qualitative agreement with previous strong-disorder renormalization group calculations but with scaling exponents depending on the coupling distribution. We find dual scaling regimes of the transverse correlations versus the distance, with an L independent form C ( r ) = r − μ for r ≪ L and C ( r , L ) = L − η f ( r / L ) for r / L > 0 , where μ > η and the scaling function is delivered by our analysis. These results are at variance with previous spin-wave and density-matrix renormalization group calculations, thus highlighting the power of unbiased quantum Monte Carlo simulations.}, archive = {J_PRL}, author = {Sibei Li and Hui Shao and Anders W. Sandvik}, doi = {10.1103/PhysRevLett.134.086501}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086501}, shortjournal = {Phys. Rev. Lett.}, title = {Ground state of the s=1/2 heisenberg spin chain with random ferromagnetic and antiferromagnetic couplings}, volume = {134}, year = {2025}, }
• (2025). Unexpected 18-fold overlapped feathery fermi pockets in typical thermoelectric Bi0.5Sb1.5Te3. PRL, 134(8), 086401. (www)

  @article{ , abstract = {is the most widely used -type commercial thermoelectric materials over six decades, yet its complex electronic structure remains uncertain especially in band degeneracy and dispersions. Here we show an unexpected band structure of 18-fold overlapped feathery Fermi pockets through substantial angle-resolved photoelectron spectroscopy data. Complemented with transport tests, we suggest that the high performance originates in the cooperation of four electronic features—momentum overlap of Fermi pockets, 18-fold band degeneracy, ultrasharp dispersions, and heavy bands. This cooperation of band features proposes a new paradigm for promising thermoelectrics.}, archive = {J_PRL}, author = {Chenxi Zhao and Shengtao Cui and Tongrui Li and Yunbo Wu and Mengruizhe Kong and Wei Bai and Kai Li and Yi Liu and Zhanfeng Liu and Zhengming Shang and Zhe Sun and Chong Xiao and Yi Xie}, doi = {10.1103/PhysRevLett.134.086401}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086401}, shortjournal = {Phys. Rev. Lett.}, title = {Unexpected 18-fold overlapped feathery fermi pockets in typical thermoelectric Bi0.5Sb1.5Te3}, volume = {134}, year = {2025}, }
• (2025). Intrinsic breakdown strength: Theoretical derivation and first-principles calculations. PRL, 134(8), 086301. (www)

  @article{ , abstract = {Intrinsic breakdown strength ( ), as the theoretical upper limit of electric field strength that a material can sustain, plays important roles in determining dielectric and safety performance. The well accepted concept is that a larger band gap ( ) often leads to a larger intrinsic breakdown strength. In this work, we analytically derive a simplified model of , showing a linear relationship between and the maximum electron density of states ( ) within the energy range spanning from the conduction band minimum (CBM) to . Using the Wannier interpolation technique to reduce the cost of calculating the for various three- and two-dimensional materials, we find that the calculated did not show any simple relationship with band gap, but it behaves linearly with the , consistent with our theoretical derivation. Our work shows that the is more fundamental than the band gap value in determining the , thus providing useful physical insights into the intrinsic dielectric breakdown strength and opening directions for improving high-power devices. The dimensional effects on has also been revealed that monolayers tend to have larger due to reduced screening effects.}, archive = {J_PRL}, author = {Shixu Liu and Hongjun Xiang and Xin-Gao Gong and Ji-Hui Yang}, doi = {10.1103/PhysRevLett.134.086301}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086301}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic breakdown strength: Theoretical derivation and first-principles calculations}, volume = {134}, year = {2025}, }
• (2025). Flat bands and temperature-driven phase transition in quasi-one-dimensional zigzag chains. PRL, 134(8), 086202. (www)

  @article{ , abstract = {Flat-band materials have garnered extensive attention due to their captivating properties associated with strong correlation effects. While flat bands have been discovered in several types of 2D materials, their existence in 1D systems remains elusive. Here, we propose a 1D frustrated lattice, specifically the 1D zigzag lattice, as a platform for hosting flat bands. This lattice can be experimentally realized by growing CuTe chains on Cu(111). The presence of flat bands was confirmed by tight-binding model analysis, first-principles calculations, and angle-resolved photoemission spectroscopy measurements. In addition, we discovered a temperature-driven phase transition at approximately 250 K. Detailed analyses demonstrate that the system has a Tomonaga-Luttinger liquid behavior, accompanied by spin-charge separation effects. Our work unveils new prospects for investigating strongly correlated electron behaviors and topological properties in the 1D limit.}, archive = {J_PRL}, author = {Jisong Gao and Haijun Cao and Xuegao Hu and Hui Zhou and Zhihao Cai and Qiaoxiao Zhao and Dong Li and Zhicheng Gao and Shin-ichiro Ideta and Kenya Shimada and Peng Cheng and Lan Chen and Kehui Wu and Sheng Meng and Baojie Feng}, doi = {10.1103/PhysRevLett.134.086202}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086202}, shortjournal = {Phys. Rev. Lett.}, title = {Flat bands and temperature-driven phase transition in quasi-one-dimensional zigzag chains}, volume = {134}, year = {2025}, }
• (2025). Origin of nonlinear circular photocurrent in 2D semiconductor MoS2. PRL, 134(8), 086201. (www)

  @article{ , abstract = {Nonlinear photogalvanic effects in two-dimensional materials, particularly the nonlinear circular photocurrents (NCPs) that belong to the helicity-dependent spin photocurrents, have sparked enormous research interest. Although notable progress has been witnessed, the underling origin of NCPs remains elusive. Here, we present systematic photocurrent characteristics, symmetry analysis and theoretical calculations to uncover the physical origin of NCPs in MoS 2 , a prototypical 2D semiconductor. Our results show that the NCP responses in 2D semiconductor MoS 2 result from the circular photon drag effect (CPDE), rather than the generally believed circular photogalvanic effect. Furthermore, we demonstrate that the NCPs are highly tunable with electrostatic doping and increase progressively with MoS 2 thickness, evidencing the interlayer constructive nature of CPDE responses. Our Letter unravels the critical role of the previously overlooked CPDE contribution to NCPs, revolutionizing previous understanding and thus providing deep insights into further fundamental studies and technological advances in nonlinear photovoltaic and opto-spintronic devices.}, archive = {J_PRL}, author = {Yanchong Zhao and Fengyu Chen and Jing Liang and Mohammad Saeed Bahramy and Mingwei Yang and Yao Guang and Xiaomei Li and Zheng Wei and Jian Tang and Jiaojiao Zhao and Mengzhou Liao and Cheng Shen and Qinqin Wang and Rong Yang and Kenji Watanabe and Takashi Taniguchi and Zhiheng Huang and Dongxia Shi and Kaihui Liu and Zhipei Sun and Ji Feng and Luojun Du and Guangyu Zhang}, doi = {10.1103/PhysRevLett.134.086201}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086201}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of nonlinear circular photocurrent in 2D semiconductor MoS2}, volume = {134}, year = {2025}, }
• (2025). Observation of floppy flexural modes in a 3D polarized maxwell beam. PRL, 134(8), 086101. (www)

  @article{ , abstract = {Beams are fundamental objects in solid mechanics, displaying flexural and torsional modes in three dimensions, and support important applications across all fields of engineering. Here, we introduce Maxwell lattice topological mechanics to beams and present a Maxwell beam model that supports topological floppy flexural modes, localized exclusively at one of its ends. We introduce a modified topological index for this Maxwell beam which lacks a complete band gap, and establish a relation between Maxwell topological polarization and frozen evanescent phonons, shedding new light on the bulk origin of the topological localization. The floppy eigenmodes and their exceptional robustness against defects are experimentally validated through vibration measurements on 3D laser-printed samples at kHz frequencies. This study opens new avenues in fields from mechanical and civil engineering to robotics by introducing topologically polarized mechanics in slender structures.}, archive = {J_PRL}, author = {Yi Chen and James P. McInerney and Paul N. Krause and Jonathan L. G. Schneider and Martin Wegener and Xiaoming Mao}, doi = {10.1103/PhysRevLett.134.086101}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086101}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of floppy flexural modes in a 3D polarized maxwell beam}, volume = {134}, year = {2025}, }
• (2025). Quantum coulomb drag mediated by cotunneling of fluxons and cooper pairs. PRL, 134(8), 086001. (www)

  @article{ , abstract = {We predict two novel quantum drag effects which can occur in macroscopically quantum coherent Josephson circuits. We demonstrate that biasing one resistively shunted Josephson junction by an external current one can induce a nonzero voltage drop across another such junction capacitively coupled to the first one. This quantum Coulomb drag is caused by cotunneling of magnetic flux quanta across both junctions which remain in the “superconducting” regime. Likewise, Cooper pair cotunneling across a pair of connected in series Josephson junctions in the “insulating” regime is responsible for another—dual—quantum Coulomb drag effect.}, archive = {J_PRL}, author = {Andrew G. Semenov and Alex Latyshev and Andrei D. Zaikin}, doi = {10.1103/PhysRevLett.134.086001}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {086001}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum coulomb drag mediated by cotunneling of fluxons and cooper pairs}, volume = {134}, year = {2025}, }
• (2025). Experimental generation of extreme electron beams for advanced accelerator applications. PRL, 134(8), 085001. (www)

  @article{ , abstract = {In this Letter, we report on the experimental generation of high energy (10 GeV), ultrashort (femtosecond-duration), ultrahigh current ( ∼ 0.1 MA ), petawatt peak power electron beams in a particle accelerator. These extreme beams enable the exploration of a new frontier of high-intensity beam-light and beam-matter interactions broadly relevant across fields ranging from laboratory astrophysics to strong field quantum electrodynamics and ultrafast quantum chemistry. We demonstrate our ability to generate and control the properties of these electron beams by means of a laser-electron beam shaping technique. This experimental demonstration opens the door to on-the-fly customization of extreme beam current profiles for desired experiments and is poised to benefit a broad swath of cross-cutting applications of relativistic electron beams.}, archive = {J_PRL}, author = {C. Emma and N. Majernik and K. K. Swanson and R. Ariniello and S. Gessner and R. Hessami and M. J. Hogan and A. Knetsch and K. A. Larsen and A. Marinelli and B. O’Shea and S. Perez and I. Rajkovic and R. Robles and D. Storey and G. Yocky}, doi = {10.1103/PhysRevLett.134.085001}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {085001}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental generation of extreme electron beams for advanced accelerator applications}, volume = {134}, year = {2025}, }
• (2025). Formation of iron-helium compounds under high pressure. PRL, 134(8), 084101. (www)

  @article{ , abstract = {We report the formation of fcc and distorted hcp iron-helium compounds with in up to 0.13 and 0.48, respectively, based on experiments at 5–54 GPa and . Upon releasing pressure under room temperature, these fcc and distorted hcp were still observed by XRD and SIMS measurements. Our first-principles calculations indicate that fcc and hcp , with helium atoms occupying the tetrahedral and trigonal-planar interstitial sites (instead of the octahedral sites), are dynamically stable throughout 0–50 GPa. These results support that the Earth’s core can be a large reservoir of primordial .}, archive = {J_PRL}, author = {Haruki Takezawa and Han Hsu and Kei Hirose and Fumiya Sakai and Suyu Fu and Hitoshi Gomi and Shiro Miwa and Naoya Sakamoto}, doi = {10.1103/PhysRevLett.134.084101}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {084101}, shortjournal = {Phys. Rev. Lett.}, title = {Formation of iron-helium compounds under high pressure}, volume = {134}, year = {2025}, }
• (2025). Restoration of axisymmetric flow structure in turbulent thermal convection by polymer additives. PRL, 134(8), 084001. (www)

  @article{ , abstract = {We present an experimental study of turbulent Rayleigh-Bénard convection in a cylindrical cell. With the addition of a tiny amount of long-chain polymers, we find, surprisingly, that the large-scale flow structure possesses axisymmetric topologies, rather than the well-known single-roll large-scale circulation (LSC), itself a result of spontaneous symmetry breaking. This symmetry restoration is found to arise from anisotropic suppression of velocity fluctuations, i.e., horizontal rms velocity becomes much less than the vertical one, as compared to the nearly isotropic bulk turbulence in the Newtonian case. This mechanism of symmetry restoration resulting from reduced fluctuations contrasts sharply with known symmetry restorations occurring in nature that usually result from increased thermal fluctuations. We further find that the net energy transfer between mean flow and turbulent fluctuations vanishes for axisymmetric topologies, whereas there is a positive net energy transfer from mean flow to turbulence for the lower-symmetry LSC topology (with or without polymers). A comparison of measured heat transfer efficiency and the large-scale flow topology points to a possible explanation for the original spontaneous symmetry breaking, in that the lower-symmetry LSC provides a higher transport efficiency. The present study provides an example of manipulating large-scale flow structures and their symmetries through small-scale properties, leading ultimately to the manipulation of turbulent transport.}, archive = {J_PRL}, author = {Fang Xu (许放 and Xiao-Shen Liu (刘小深 and Xiao-Ming Li (李小明 and Ke-Qing Xia (夏克青}, doi = {10.1103/PhysRevLett.134.084001}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {084001}, shortjournal = {Phys. Rev. Lett.}, title = {Restoration of axisymmetric flow structure in turbulent thermal convection by polymer additives}, volume = {134}, year = {2025}, }
• (2025). Weakly dispersive band in synthetic moiré superlattice inducing optimal compact comb generation. PRL, 134(8), 083803. (www)

  @article{ , abstract = {The moiré superlattices attract growing interest for holding exotic physics due to their fascinating properties from electronics to photonics. Much attention has been focused on the localization effect for waves in the flat band regime or the delocalization effect from the strongly dispersive band feature. Here, we study the weakly dispersive band in between the two above scenarios in a one-dimensional synthetic frequency moiré superlattice and observe the wave packet distributions therein toward novel frequency comb generation. Mode spacing in the spectral wave packet is reduced compared to the free spectral range of individual rings due to the mode couplings from the unequal sublattice periods of the synthetic moiré lattice. We unveil that the optimal compact frequency comb generation occurs in the weakly dispersive regime holding simultaneously uniform power distribution and broad frequency spanning in our experiment, benefiting from the interplay between the band flatness and power uniformity of mode distribution. Our results study the fundamental physics of the weakly dispersive moiré band in the synthetic frequency dimension and also show a new way for the future compact frequency comb generation in on-chip devices with small footprint size.}, archive = {J_PRL}, author = {Guangzhen Li and Yanyan He and Luojia Wang and Yiwen Yang and Danying Yu and Yuanlin Zheng and Luqi Yuan and Xianfeng Chen}, doi = {10.1103/PhysRevLett.134.083803}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083803}, shortjournal = {Phys. Rev. Lett.}, title = {Weakly dispersive band in synthetic moiré superlattice inducing optimal compact comb generation}, volume = {134}, year = {2025}, }
• (2025). Q-plates: From optical vortices to optical skyrmions. PRL, 134(8), 083802. (www)

  @article{ , abstract = {We report on the extension of the q-plate concept, a hallmark of spin-orbit optical vortex generation since its introduction in 2006, to the generation of optical skyrmions. Stokes skyrmions of arbitrary order with polarization-controlled Skyrme number and reconfigurable multiskyrmions are obtained. This is done by endowing q-plates with a winding number associated with the radial degree of freedom that adds to the usual one associated with the azimuthal degree of freedom.}, archive = {J_PRL}, author = {Vagharshak Hakobyan and Etienne Brasselet}, doi = {10.1103/PhysRevLett.134.083802}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083802}, shortjournal = {Phys. Rev. Lett.}, title = {Q-plates: From optical vortices to optical skyrmions}, volume = {134}, year = {2025}, }
• (2025). Room temperature superfluorescence from an electron-hole liquid. PRL, 134(8), 083801. (www)

  @article{ , abstract = {Superfluorescence, a coherent burst of light from an excited ensemble of emitters, is a crucial quantum optical phenomenon with far-reaching implications in nanophotonics and many-body optical processes. Despite its observation in various systems, realizing superfluorescence in an electron-hole plasma (EHP) at room temperature has remained a formidable challenge, hindering the development of continuous-wave and electrically excited superfluorescence devices. Herein, we address this challenge by condensing the high-density EHP into an electron-hole liquid (EHL) at room temperature, thereby preserving quantum coherence. Using a model system of nanocrystal thin films, we demonstrate the first experimental observation of room temperature superfluorescence from an EHL. Key attributes heralding superfluorescence include a redshift of from uncorrelated exciton emission, a fluence-dependent delayed growth of macroscopic coherence with abrupt radiative decay times faster than spontaneous emission, a distinct quadratic fluence dependence with a clear threshold, and Burnham-Chiao ringing. These findings open up exciting possibilities for developing electrically pumped colloidal nanocrystals lasers and quantum technologies operating at room temperature.}, archive = {J_PRL}, author = {Naresh Aggarwal and Ajay Kumar Poonia and Dmitry N. Dirin and Ihor Cherniukh and Arijit Sinha and Umesh V. Waghmare and Maryna I. Bodnarchuk and Sebastian Wüster and Maksym V. Kovalenko and K. V. Adarsh}, doi = {10.1103/PhysRevLett.134.083801}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083801}, shortjournal = {Phys. Rev. Lett.}, title = {Room temperature superfluorescence from an electron-hole liquid}, volume = {134}, year = {2025}, }
• (2025). Spin self-organization in an optical cavity facilitated by inhomogeneous broadening. PRL, 134(8), 083603. (www)

  @article{ , abstract = {We study the onset of collective spin self-organization in a thermal ensemble of driven two-level atoms confined in an optical cavity. The atoms spontaneously form a spin pattern above a critical driving strength that sets a threshold and is determined by the cavity parameters, the initial temperature, and the transition frequency of the atomic spin. Remarkably, we find that inhomogeneous Doppler broadening facilitates the onset of spin self-organization. In particular, the threshold is nonmonotonic when increasing the spin transition frequency and reaches a minimum when the Doppler broadening is of similar magnitude. This feature emerges due to Doppler-induced resonances. Above the threshold, we find cooperative dynamics of spin, spatial, and momentum degrees of freedom leading to density modulations, fast reduction of kinetic energy, and the emergence of nonthermal states. More broadly, our work demonstrates how broadening can facilitate strong light-matter interactions in many-body systems.}, archive = {J_PRL}, author = {Marc Nairn and Luigi Giannelli and Giovanna Morigi and Sebastian Slama and Beatriz Olmos and Simon B. Jäger}, doi = {10.1103/PhysRevLett.134.083603}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083603}, shortjournal = {Phys. Rev. Lett.}, title = {Spin self-organization in an optical cavity facilitated by inhomogeneous broadening}, volume = {134}, year = {2025}, }
• (2025). Room-temperature optically detected magnetic resonance of telecom single-photon emitters in GaN. PRL, 134(8), 083602. (www)

  @article{ , abstract = {Solid-state defects susceptible of spin manipulation hold great promise for scalable quantum technology. To broaden their utility, operation at room temperature and emission in the telecom wavelength range are desired, eliminating cryogenic requirements and leveraging existing optical fiber infrastructure for the transmission of quantum information. To that end, we report that telecom single-photon emitters (SPEs) in gallium nitride (GaN) exhibit optically detected magnetic resonance (ODMR) at room temperature. The analysis of ODMR as a function of magnetic field orientation enables the determination of the orientation of the spin quantization axis with respect to the GaN crystalline lattice. The optical transitions dynamics are analyzed to gain further insight into the transition rates dominating ODMR. Our findings, coupled with the mature fabrication technology of GaNs, could facilitate the realization of scalable quantum technology.}, archive = {J_PRL}, author = {John J. H. Eng and Zhengzhi Jiang and Max Meunier and Abdullah Rasmita and Haoran Zhang and Yuzhe Yang and Feifei Zhou and Hongbing Cai and Zhaogang Dong and Jesús Zúñiga-Pérez and Weibo Gao}, doi = {10.1103/PhysRevLett.134.083602}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083602}, shortjournal = {Phys. Rev. Lett.}, title = {Room-temperature optically detected magnetic resonance of telecom single-photon emitters in GaN}, volume = {134}, year = {2025}, }
• (2025). Atomic-scale on-demand photon polarization manipulation with high efficiency for integrated photonic chips. PRL, 134(8), 083601. (www)

  @article{ , abstract = {In order to overcome the challenge of lacking polarization encoding in integrated quantum photonic circuits, we propose a scheme to realize arbitrary polarization manipulation of a single photon by integrating a single quantum emitter in a photonic waveguide. In our scheme, one transition path of the three-level emitter is designed to simultaneously couple with two orthogonal polarization degenerate modes in the waveguide with adjustable coupling strengths, and the other transition path of the three-level emitter is driven by an external coherent field. The proposed polarization converter has several advantages, including arbitrary polarization conversion for any input polarization, tunable working frequency, excellent antidissipation ability with high-conversion efficiency, and atomic-scale size. Our Letter provides an effective solution to enable the polarization encoding of photons that can be applied in the integrated quantum photonic circuits, and will boost quantum photonic chips.}, archive = {J_PRL}, author = {Yunning Lu and Zeyang Liao and Xue-Hua Wang}, doi = {10.1103/PhysRevLett.134.083601}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083601}, shortjournal = {Phys. Rev. Lett.}, title = {Atomic-scale on-demand photon polarization manipulation with high efficiency for integrated photonic chips}, volume = {134}, year = {2025}, }
• (2025). In situ imaging of a single-atom wave packet in continuous space. PRL, 134(8), 083403. (www)

  @article{ , abstract = {We report on the imaging of the in situ spatial distribution of deterministically prepared single-atom wave packets as they expand in a plane, finding excellent agreement with the scaling dynamics predicted by the Schrödinger equation. Our measurement provides a direct and quantitative observation of the textbook free expansion of a one-particle Gaussian wave packet, which we believe has no equivalent in the existing literature. Second, we utilize these expanding wave packets as a benchmark to develop a protocol for the controlled projection of a spatially extended wave function from continuous space onto the sites of a deep optical lattice and subsequent single-atom imaging using quantum gas microscopy techniques. By probing the square modulus of the wave function for various lattice ramp-up times, we show how to obtain a near-perfect projection onto lattice sites. Establishing this protocol represents a crucial prerequisite to the realization of a quantum gas microscope for continuum physics. The method demonstrated here for imaging a wave packet whose initial extent greatly exceeds the pinning lattice spacing, is designed to be applicable to the many-body wave function of interacting systems in continuous space, promising a direct access to their microscopic properties, including spatial correlation functions up to high order and large distances.}, archive = {J_PRL}, author = {Joris Verstraten and Kunlun Dai and Maxime Dixmerias and Bruno Peaudecerf and Tim de Jongh and Tarik Yefsah}, doi = {10.1103/PhysRevLett.134.083403}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083403}, shortjournal = {Phys. Rev. Lett.}, title = {In situ imaging of a single-atom wave packet in continuous space}, volume = {134}, year = {2025}, }
• (2025). Kolmogorov scaling in turbulent 2D bose-einstein condensates. PRL, 134(8), 083402. (www)

  @article{ , abstract = {We investigated turbulence in 2D atomic Bose-Einstein condensates (BECs) using a minimally destructive, impurity injection technique analogous to particle image velocimetry in conventional fluids. Our approach transfers small regions of the BEC into a different hyperfine state and tracks their displacement, ultimately yielding the velocity field. This allows us to quantify turbulence in the same way as is conventional in fluid dynamics in terms of velocity-velocity correlation functions, called velocity structure functions, that obey Kolmogorov scaling laws. Furthermore, the velocity increments show a clear fat-tail non-Gaussian distribution that results from intermittency corrections to the initial “K41” Kolmogorov theory. Our observations are fully consistent with the later “KO62” description. These results are validated by a 2D dissipative Gross-Pitaevskii simulation.}, archive = {J_PRL}, author = {M. Zhao and J. Tao and I. B. Spielman}, doi = {10.1103/PhysRevLett.134.083402}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083402}, shortjournal = {Phys. Rev. Lett.}, title = {Kolmogorov scaling in turbulent 2D bose-einstein condensates}, volume = {134}, year = {2025}, }
• (2025). Magneto-optical trapping of a heavy polyatomic molecule for precision measurement. PRL, 134(8), 083401. (www)

  @article{ , abstract = {We report a magneto-optical trap of strontium monohydroxide (SrOH) containing 2000(600) molecules at a temperature of 1.2(3) mK. The lifetime is 91(9) ms, which is limited by decay to optically unaddressed vibrational states. This provides the foundation for future sub-Doppler cooling and optical trapping of SrOH, a polyatomic molecule suited for precision searches for physics beyond the standard model including new CP violating particles and ultralight dark matter. We also identify important features in this system that guide cooling and trapping of complex and heavy polyatomic molecules into the ultracold regime.}, archive = {J_PRL}, author = {Zack D. Lasner and Alexander Frenett and Hiromitsu Sawaoka and Loïc Anderegg and Benjamin Augenbraun and Hana Lampson and Mingda Li and Annika Lunstad and Jack Mango and Abdullah Nasir and Tasuku Ono and Takashi Sakamoto and John M. Doyle}, doi = {10.1103/PhysRevLett.134.083401}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {083401}, shortjournal = {Phys. Rev. Lett.}, title = {Magneto-optical trapping of a heavy polyatomic molecule for precision measurement}, volume = {134}, year = {2025}, }
• (2025). Nuclear astrophysics in the storage ring: Background suppressed simultaneous measurement of (p,γ) and (p,n) reactions. PRL, 134(8), 082701. (www)

  @article{ , abstract = {We report the application of the new elimination of Rutherford elastic scattering technique for the measurement of proton-induced reaction cross sections utilizing stored ions decelerated to astrophysical energies. This approach results in a background reduction factor of about 1 order of magnitude, enabling the first measurement of a ( p , n ) cross section in a storage ring. Here, the reaction channels Xe 124 ( p , n ) and Xe 124 ( p , γ ) have been studied just above the neutron threshold energy. The new data provide valuable constraints for Hauser-Feshbach theory and extrapolation of the ( p , γ ) cross section to lower energies. Most importantly, for nuclei of limited availability, the method represents a powerful improvement to efficiently study proton-induced reactions at energies within or close to the astrophysical Gamow window, bringing many reaction measurements within reach that were previously inaccessible in the laboratory.}, archive = {J_PRL}, author = {L. Varga and J. Glorius and M. Aliotta and K. Blaum and L. Bott and C. Brandau and B. Brückner and C. G. Bruno and X. Chen and R. Chen and S. Dababneh and T. Davinson and D. Dmytriiev and S. F. Dellmann and I. Dillmann and P. Erbacher and S. Fiebiger and O. Forstner and T. Gaßner and K. Göbel and S. Goriely and C. J. Griffin and R. E. Grisenti and M. Groothuis and A. Gumberidze and G. Gyürky and M. Heil and R. Hensch and R. Hess and P.-M. Hillenbrand and P. Hillmann and O. Hinrichs and R. Joseph and B. Jurado and T. Kausch and K. Khasawneh and A. Khodaparast and T. Kisselbach and N. Klapper and C. Kozhuharov and D. Kurtulgil and G. J. Lane and C. Langer and G. Leckenby and C. Lederer-Woods and M. Lestinsky and Yu. A. Litvinov and S. Litvinov and B. Löher and E. Lorenz and B. Lorentz and P. Marini and J. Marsh and E. Menz and T. Morgenroth and T. T. Nguyen and F. Nolden and N. Petridis and U. Popp and A. Psaltis and M. Reed and R. Reifarth and M. S. Sanjari and D. Savran and M. Sguazzin and H. Simon and R. S. Sidhu and Z. Slavkovská and U. Spillmann and M. Steck and T. Stöhlker and J. Stumm and A. Surzhykov and J. Swartz and T. Szücs and A. Taremi Zadeh and B. Thomas and S. Yu. Torilov and H. Törnqvist and M. Träger and C. Trageser and S. Trotsenko and D. Vescovi and M. Volknandt and H. Weick and M. Weigand and C. Wolf and P. J. Woods and Y. M. Xing and T. Yamaguchi}, doi = {10.1103/PhysRevLett.134.082701}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082701}, shortjournal = {Phys. Rev. Lett.}, title = {Nuclear astrophysics in the storage ring: Background suppressed simultaneous measurement of (p,γ) and (p,n) reactions}, volume = {134}, year = {2025}, }
• (2025). Origin of the low-energy enhancement of the γ-ray strength function. PRL, 134(8), 082502. (www)

  @article{ , abstract = {The low-energy enhancement (LEE) in γ -ray strength functions has been experimentally identified in a large number of nuclei during the past two decades; however, the origin of the enhancement is not fully understood. Building on previous theoretical work, we investigate the LEE and its relation to the scissors mode (SM) with an independent theoretical approach. We apply a novel angular-momentum-projected shell-model method that explicitly endows degrees of freedom to describe the scissors motion. Taking the recently measured γ -ray strength functions in Neodymium isotopes as examples, we find that the LEE arises from a quasi-free scissors motion appearing only in weakly-deformed nuclei, which can be viewed as an approximate free-rotation of neutrons with respect to protons. This leads us to propose a new type of collective motion, scissors rotation , to contrast the scissors vibration widely known in well-deformed nuclei. The observed LEE is naturally interpreted as the first evidence for this collective excitation mode.}, archive = {J_PRL}, author = {Fang-Qi Chen (陈芳祁 and Y. F. Niu (牛一斐 and Yang Sun (孙扬 and Mathis Wiedeking}, doi = {10.1103/PhysRevLett.134.082502}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082502}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of the low-energy enhancement of the γ-ray strength function}, volume = {134}, year = {2025}, }
• (2025). Improved limit on neutrinoless double beta decay of mo100 from AMoRE-I. PRL, 134(8), 082501. (www)

  @article{ , abstract = {AMoRE searches for the neutrinoless double beta decay using 100 kg of enriched . Scintillating molybdate crystals coupled with a metallic magnetic calorimeter operate at milli-Kelvin temperatures to measure the energy of electrons emitted in the decay. AMoRE-I is a demonstrator for the full-scale AMoRE, operated at the Yangyang Underground Laboratory for over two years. The exposure was (or ), and the total background rate near the value was . We observed no indication of decay and report a new lower limit of the half-life of decay as at 90% confidence level. The effective Majorana mass limit range is using nuclear matrix elements estimated in the framework of different models, including the recent shell model calculations.}, archive = {J_PRL}, author = {AMoRE Collaboration and A. Agrawal and V. V. Alenkov and P. Aryal and J. Beyer and B. Bhandari and R. S. Boiko and K. Boonin and O. Buzanov and C. R. Byeon and N. Chanthima and M. K. Cheoun and J. S. Choe and Seonho Choi and S. Choudhury and J. S. Chung and F. A. Danevich and M. Djamal and D. Drung and C. Enss and A. Fleischmann and A. M. Gangapshev and L. Gastaldo and Y. M. Gavrilyuk and A. M. Gezhaev and O. Gileva and V. D. Grigorieva and V. I. Gurentsov and C. Ha and D. H. Ha and E. J. Ha and D. H. Hwang and E. J. Jeon and J. A. Jeon and H. S. Jo and J. Kaewkhao and C. S. Kang and W. G. Kang and V. V. Kazalov and S. Kempf and A. Khan and S. Khan and D. Y. Kim and G. W. Kim and H. B. Kim and Ho-Jong Kim and H. J. Kim and H. L. Kim and H. S. Kim and M. B. Kim and S. C. Kim and S. K. Kim and S. R. Kim and W. T. Kim and Y. D. Kim and Y. H. Kim and K. Kirdsiri and Y. J. Ko and V. V. Kobychev and V. Kornoukhov and V. V. Kuzminov and D. H. Kwon and C. H. Lee and DongYeup Lee and E. K. Lee and H. J. Lee and H. S. Lee and J. Lee and J. Y. Lee and K. B. Lee and M. H. Lee and M. K. Lee and S. W. Lee and Y. C. Lee and D. S. Leonard and H. S. Lim and B. Mailyan and E. P. Makarov and P. Nyanda and Y. Oh and S. L. Olsen and S. I. Panasenko and H. K. Park and H. S. Park and K. S. Park and S. Y. Park and O. G. Polischuk and H. Prihtiadi and S. Ra and S. S. Ratkevich and G. Rooh and E. Sala and M. B. Sari and J. Seo and K. M. Seo and B. Sharma and K. A. Shin and V. N. Shlegel and K. Siyeon and J. So and N. V. Sokur and J. K. Son and J. W. Song and N. Srisittipokakun and V. I. Tretyak and R. Wirawan and K. R. Woo and H. J. Yeon and Y. S. Yoon and Q. Yue}, doi = {10.1103/PhysRevLett.134.082501}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082501}, shortjournal = {Phys. Rev. Lett.}, title = {Improved limit on neutrinoless double beta decay of mo100 from AMoRE-I}, volume = {134}, year = {2025}, }
• (2025). Calibrating the medium effects of light clusters in heavy-ion collisions. PRL, 134(8), 082304. (www)

  @article{ , abstract = {We propose a Bayesian inference estimation of in-medium modification of the cluster self-energies from light nuclei multiplicities measured in selected samples of central Xe 136 , 124 + Sn 124 , 112 collisions with the INDRA apparatus. The data are interpreted with a relativistic quasiparticle cluster approach in the mean-field approximation without any prior assumption on the thermal parameters of the model. An excellent reproduction is obtained for H and He isotope multiplicities, and compatible posterior distributions are found for the unknown thermal parameters. We conclude that the cluster- σ -meson coupling is temperature dependent, becoming weaker when the temperature increases, in agreement with microscopic quantum statistical calculations. This implies a faster decrease of the light cluster abundances with temperature than previously estimated.}, archive = {J_PRL}, author = {Tiago Custódio and Alex Rebillard-Soulié and Rémi Bougault and Diego Gruyer and Francesca Gulminelli and Tuhin Malik and Helena Pais and Constança Providência}, doi = {10.1103/PhysRevLett.134.082304}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082304}, shortjournal = {Phys. Rev. Lett.}, title = {Calibrating the medium effects of light clusters in heavy-ion collisions}, volume = {134}, year = {2025}, }
• (2025). Minimizing selection bias in inclusive jets in heavy-ion collisions with energy correlators. PRL, 134(8), 082303. (www)

  @article{ , abstract = {The first-ever measurement of energy correlators within inclusive jets produced in heavy-ion collisions, revealed by the CMS Collaboration, shows a clear enhancement at large angles relative to the proton-proton (p-p) baseline. However, interpreting this enhancement is complicated due to selection bias from energy loss, which also distorts the energy correlator heavy-ion to p-p ratio in the hadronization region, hindering our understanding of parton/hadron dynamics in a colored medium. In this Letter, we introduce a new ratio of energy correlator observables that removes the leading effects of selection bias from the two-point energy correlator spectrum (E2C). pythia and herwig simulations show that the impact of selection bias in the E2C is reduced by an order of magnitude, while sensitivity to any other medium modifications is retained. This quantity can be obtained directly from the experimental measurements presented by CMS, as illustrated in an accompanying note [C. Andres and J. Holguin, arXiv:2409.07526 ].}, archive = {J_PRL}, author = {Carlota Andres and Jack Holguin and Raghav Kunnawalkam Elayavalli and Jussi Viinikainen}, doi = {10.1103/PhysRevLett.134.082303}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082303}, shortjournal = {Phys. Rev. Lett.}, title = {Minimizing selection bias in inclusive jets in heavy-ion collisions with energy correlators}, volume = {134}, year = {2025}, }
• (2025). Generalized thermodynamic relations for perfect spin hydrodynamics. PRL, 134(8), 082302. (www)

  @article{ , abstract = {Generalized thermodynamic relations are introduced into the framework of a relativistic perfect spin hydrodynamics. They allow for consistent treatment of spin degrees of freedom, including the use of spin tensors whose structure follows from microscopic calculations. The obtained results are important for establishing consistency between different formulations of spin hydrodynamics and form the basis for introducing dissipative corrections.}, archive = {J_PRL}, author = {Wojciech Florkowski and Mykhailo Hontarenko}, doi = {10.1103/PhysRevLett.134.082302}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082302}, shortjournal = {Phys. Rev. Lett.}, title = {Generalized thermodynamic relations for perfect spin hydrodynamics}, volume = {134}, year = {2025}, }
• (2025). Anisotropic flow in fixed-target Pb208+Ne20 collisions as a probe of quark-gluon plasma. PRL, 134(8), 082301. (www)

  @article{ , abstract = {The System for Measuring Overlap with Gas (SMOG2) at the LHCb detector enables the study of fixed-target ion-ion collisions at relativistic energies ( in the center of mass). With input from ab initio calculations of the structure of and , we compute hydrodynamic predictions for the anisotropic flow of and collisions to be tested with upcoming LHCb data. This will allow the detailed study of quark-gluon plasma formation as well as experimental tests of the predicted nuclear shapes. Elliptic flow ( ) in collisions is greatly enhanced compared to the baseline due to the shape of , which is deformed in a bowling-pin geometry. Owing to the large radius, this effect is seen in a broad centrality range, a unique feature of this collision configuration. Larger elliptic flow further enhances the quadrangular flow ( ) of collisions via nonlinear coupling, and impacts the sign of the kurtosis of the elliptic flow vector distribution ( ). Exploiting the shape of proves thus an ideal method to investigate the formation of quark-gluon plasma in fixed-target experiments at LHCb, and demonstrates the power of System for Measuring Overlap with Gas as a tool to image nuclear ground states.}, archive = {J_PRL}, author = {Giuliano Giacalone and Wenbin Zhao and Benjamin Bally and Shihang Shen and Thomas Duguet and Jean-Paul Ebran and Serdar Elhatisari and Mikael Frosini and Timo A. Lähde and Dean Lee and Bing-Nan Lu and Yuan-Zhuo Ma and Ulf-G. Meißner and Govert Nijs and Jacquelyn Noronha-Hostler and Christopher Plumberg and Tomás R. Rodríguez and Robert Roth and Wilke van der Schee and Björn Schenke and Chun Shen and Vittorio Somà}, doi = {10.1103/PhysRevLett.134.082301}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {082301}, shortjournal = {Phys. Rev. Lett.}, title = {Anisotropic flow in fixed-target Pb208+Ne20 collisions as a probe of quark-gluon plasma}, volume = {134}, year = {2025}, }
• (2025). First determination of the spin-parity of Ξc(3055)+,0 baryons. PRL, 134(8), 081901. (www)

  @article{ , abstract = {The Ξ b 0 ( − ) → Ξ c ( 3055 ) + ( 0 ) ( → D + ( 0 ) Λ ) π − decay chains are observed, and the spin-parity of Ξ c ( 3055 ) + ( 0 ) baryons is determined for the first time. The measurement is performed using proton-proton collision data at a center-of-mass energy of s = 13 TeV , corresponding to an integrated luminosity of 5.4 fb − 1 , recorded by the LHCb experiment between 2016 and 2018. The spin-parity of the Ξ c ( 3055 ) + ( 0 ) baryons is determined to be 3 / 2 + with a significance of more than 6.5 σ ( 3.5 σ ) compared to all other tested hypotheses. The up-down asymmetries of the Ξ b 0 ( − ) → Ξ c ( 3055 ) + ( 0 ) π − transitions are measured to be − 0.92 ± 0.10 ± 0.05 ( − 0.92 ± 0.16 ± 0.22 ), consistent with maximal parity violation, where the first uncertainty is statistical and the second is systematic. These results support the hypothesis that the Ξ c ( 3055 ) + ( 0 ) baryons correspond to the first D -wave λ -mode excitation of the Ξ c flavor triplet.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and R. Ataíde Da Silva and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and W. Baldini and L. Balzani and H. Bao and J. Baptista de Souza Leite and C. Barbero Pretel and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and J. M. Basels and S. Bashir and G. Bassi and B. Batsukh and P. B. Battista and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and N. A. Behling and S. Belin and V. Bellee and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and N. Bondar and A. Bordelius and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and M. Bovill and T. J. V. Bowcock and A. Boyer and C. Bozzi and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and A. Butkevich and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and A. C. Caillet and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and J. Castro Godinez and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and E. Chatzianagnostou and C. A. Chavez Barajas and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and X. Chiotopoulos and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and P. Collins and T. Colombo and M. Colonna and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and S. Dekkers and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and E. Epple and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and A. Fernandez Casani and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and K. L. Fischer and D. S. Fitzgerald and C. Fitzpatrick and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Führing and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and T. Q. Gao and Y. Gao and M. Garau and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and S. Ghizzo and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and L. Girardey and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and A. Gomes and S. Gomez Fernandez and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and L. Guerry and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and J. Haimberger and M. Hajheidari and G. Hallett and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and M. Hartmann and S. Hashmi and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and D. Hill and S. E. Hollitt and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and A. John Rubesh Rajan and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and J. Juan Castella and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and M. Kane and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and M. K. Kazanecki and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. Kshyvanskyi and J. Kubat and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and P. Laguarta Gonzalez and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and G. Lanfranchi and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and H. Lee and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and B. Leverington and A. Li and C. Li and H. Li and K. Li and L. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and W. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and J. Lomba Castro and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and Q. Lu and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and R. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. J. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and E. Mariani and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and L. Martel and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Santos and F. Martinez Vidal and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and J. Mazorra de Cos and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and R. A. Mohammed and R. D. Moise and S. Mokhnenko and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and Q. Niu and P. Nogarolli and P. Nogga and N. S. Nolte and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and D. Osthues and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and F. Paciolla and A. Padee and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perro and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and T. Poeschl and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and V. Pugatch and G. Punzi and S. Qasim and Q. Q. Qian and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and J. Roensch and A. Rogachev and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and M. Romero Lamas and A. Romero Vidal and G. Romolini and F. Ronchetti and T. Rong and M. Rotondo and S. R. Roy and M. S. Rudolph and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and C. Sanchez Gras and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and A. Sarnatskiy and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and F. Sborzacchi and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and Y. Sun and D. Sundfeld and W. Sutcliffe and P. N. Swallow and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and V. Valcarce Cadenas and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Vesterinen and D. Vico Benet and P. Vidrier Villalba and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and G. Vouters and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and H. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Y. W. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and C. White and M. Whitehead and E. Whiter and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. R. J. Williams and R. Williams and Z. Williams and F. F. Wilson and W. Wislicki and M. Witek and L. Witola and C. P. Wong and G. Wormser and S. A. Wotton and H. Wu and J. Wu and Y. Wu and Z. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and D. Yang and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and X. Yin and C. Y. Yu and J. Yu and X. Yuan and Y. Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and F. Zenesini and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and S. Z. Zheng and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.081901}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081901}, shortjournal = {Phys. Rev. Lett.}, title = {First determination of the spin-parity of Ξc(3055)+,0 baryons}, volume = {134}, year = {2025}, }
• (2025). Unique forbidden beta decays at zero momentum transfer. PRL, 134(8), 081805. (www)

  @article{ , abstract = {We report an exploratory study of the O ( α ) structure-dependent electromagnetic radiative corrections to unique first-forbidden nuclear beta decays. We show that the insertion of angular momentum into the nuclear matrix element by the virtual or real photon exchange opens up the decay at vanishing nuclear recoil momentum which was forbidden at tree level, leading to a dramatic change in the decay spectrum not anticipated in existing studies. We discuss its implications for precision tests on the standard model and searches for new physics.}, archive = {J_PRL}, author = {Chien-Yeah Seng and Ayala Glick-Magid and Vincenzo Cirigliano}, doi = {10.1103/PhysRevLett.134.081805}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081805}, shortjournal = {Phys. Rev. Lett.}, title = {Unique forbidden beta decays at zero momentum transfer}, volume = {134}, year = {2025}, }
• (2025). Dual-baseline search for active-to-sterile neutrino oscillations in NOvA. PRL, 134(8), 081804. (www)

  @article{ , abstract = {We report a search for neutrino oscillations to sterile neutrinos under a model with three active and one sterile neutrinos ( model). This analysis uses the NOvA detectors exposed to the NuMI beam, running in neutrino mode. The data exposure, protons on target, doubles that previously analyzed by NOvA, and the analysis is the first to use charged-current interactions in conjunction with neutral-current interactions. Neutrino samples in the near and far detectors are fitted simultaneously, enabling the search to be carried out over a range extending 2 (3) orders of magnitude above (below) . NOvA finds no evidence for active-to-sterile neutrino oscillations under the model at 90% confidence level. New limits are reported in multiple regions of parameter space, excluding some regions currently allowed by IceCube at 90% confidence level. We additionally set the most stringent limits for anomalous appearance for .}, archive = {J_PRL}, author = {NOvA Collaboration and M. A. Acero and B. Acharya and P. Adamson and N. Anfimov and A. Antoshkin and E. Arrieta-Diaz and L. Asquith and A. Aurisano and A. Back and N. Balashov and P. Baldi and B. A. Bambah and E. F. Bannister and A. Barros and A. Bat and K. Bays and R. Bernstein and T. J. C. Bezerra and V. Bhatnagar and D. Bhattarai and B. Bhuyan and J. Bian and A. C. Booth and R. Bowles and B. Brahma and C. Bromberg and N. Buchanan and A. Butkevich and S. Calvez and T. J. Carroll and E. Catano-Mur and J. P. Cesar and A. Chatla and R. Chirco and B. C. Choudhary and A. Christensen and M. F. Cicala and T. E. Coan and A. Cooleybeck and C. Cortes-Parra and D. Coveyou and L. Cremonesi and G. S. Davies and P. F. Derwent and P. Ding and Z. Djurcic and K. Dobbs and M. Dolce and D. Doyle and D. Dueñas Tonguino and E. C. Dukes and A. Dye and R. Ehrlich and E. Ewart and P. Filip and M. J. Frank and H. R. Gallagher and F. Gao and A. Giri and R. A. Gomes and M. C. Goodman and M. Groh and R. Group and A. Habig and F. Hakl and J. Hartnell and R. Hatcher and H. Hausner and M. He and K. Heller and V. Hewes and A. Himmel and T. Horoho and A. Ivanova and B. Jargowsky and J. Jarosz and M. Judah and I. Kakorin and A. Kalitkina and D. M. Kaplan and B. Kirezli-Ozdemir and J. Kleykamp and O. Klimov and L. W. Koerner and L. Kolupaeva and R. Kralik and A. Kumar and V. Kus and T. Lackey and K. Lang and J. Lesmeister and A. Lister and J. Liu and J. A. Lock and M. Lokajicek and M. MacMahon and S. Magill and W. A. Mann and M. T. Manoharan and M. Manrique Plata and M. L. Marshak and M. Martinez-Casales and V. Matveev and B. Mehta and M. D. Messier and H. Meyer and T. Miao and V. Mikola and W. H. Miller and S. Mishra and S. R. Mishra and A. Mislivec and R. Mohanta and A. Moren and A. Morozova and W. Mu and L. Mualem and M. Muether and D. Myers and D. Naples and A. Nath and S. Nelleri and J. K. Nelson and R. Nichol and E. Niner and A. Norman and A. Norrick and H. Oh and A. Olshevskiy and T. Olson and M. Ozkaynak and A. Pal and J. Paley and L. Panda and R. B. Patterson and G. Pawloski and R. Petti and R. K. Plunkett and L. R. Prais and M. Rabelhofer and A. Rafique and V. Raj and M. Rajaoalisoa and B. Ramson and B. Rebel and P. Roy and O. Samoylov and M. C. Sanchez and S. Sánchez Falero and P. Shanahan and P. Sharma and A. Sheshukov and A. Shmakov and Shivam and W. Shorrock and S. Shukla and D. K. Singha and I. Singh and P. Singh and V. Singh and E. Smith and J. Smolik and P. Snopok and N. Solomey and A. Sousa and K. Soustruznik and M. Strait and L. Suter and A. Sutton and K. Sutton and S. Swain and C. Sweeney and A. Sztuc and B. Tapia Oregui and N. Talukdar and P. Tas and T. Thakore and J. Thomas and E. Tiras and M. Titus and Y. Torun and D. Tran and J. Tripathi and J. Trokan-Tenorio and J. Urheim and P. Vahle and Z. Vallari and J. D. Villamil and K. J. Vockerodt and M. Wallbank and C. Weber and M. Wetstein and D. Whittington and D. A. Wickremasinghe and T. Wieber and J. Wolcott and M. Wrobel and S. Wu and W. Wu and Y. Xiao and B. Yaeggy and A. Yahaya and A. Yankelevich and K. Yonehara and S. Zadorozhnyy and J. Zalesak and R. Zwaska}, doi = {10.1103/PhysRevLett.134.081804}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081804}, shortjournal = {Phys. Rev. Lett.}, title = {Dual-baseline search for active-to-sterile neutrino oscillations in NOvA}, volume = {134}, year = {2025}, }
• (2025). Wess-zumino-witten interactions of axions. PRL, 134(8), 081803. (www)

  @article{ , abstract = {We present a consistent derivation of the complete Wess-Zumino-Witten interactions of axions, including the counter-term necessary to guarantee the gauge invariance of the standard model. By treating the derivative of the axion field as a background gauge field and incorporating auxiliary chiral rotation phases, we ensure consistency in the axion-interaction Lagrangian. This approach allows us to derive basis-independent physical interactions of axions with gauge bosons and vector mesons. These interactions have broad applications in axion phenomenology for both light and heavy axion particles.}, archive = {J_PRL}, author = {Yang Bai and Ting-Kuo Chen and Jia Liu and Xiaolin Ma}, doi = {10.1103/PhysRevLett.134.081803}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081803}, shortjournal = {Phys. Rev. Lett.}, title = {Wess-zumino-witten interactions of axions}, volume = {134}, year = {2025}, }
• (2025). Search for the KL→π0νν¯ decay at the J-PARC KOTO experiment. PRL, 134(8), 081802. (www)

  @article{ , abstract = {We performed a search for the decay using the data taken in 2021 at the J-PARC KOTO experiment. With newly installed counters and new analysis method, the expected background was suppressed to . With a single event sensitivity of , no events were observed in the signal region. An upper limit on the branching fraction for the decay was set to be at the 90% confidence level (C.L.), which improved the previous upper limit from KOTO by a factor of 1.4. With the same data, a search for was also performed, where is an invisible boson with a mass ranging from 1 to . For with a mass of , an upper limit on the branching fraction of was set to be at the 90% C.L.}, archive = {J_PRL}, author = {KOTO Collaboration and J. K. Ahn and M. Farrington and M. Gonzalez and N. Grethen and K. Hanai and N. Hara and H. Haraguchi and Y. B. Hsiung and T. Inagaki and M. Katayama and T. Kato and Y. Kawata and E. J. Kim and H. M. Kim and A. Kitagawa and T. K. Komatsubara and K. Kotera and S. K. Lee and X. Li and G. Y. Lim and C. Lin and Y. Luo and T. Mari and T. Matsumura and I. Morioka and H. Nanjo and H. Nishimiya and Y. Noichi and T. Nomura and K. Ono and M. Osugi and P. Paschos and J. Redeker and T. Sato and Y. Sato and T. Shibata and N. Shimizu and T. Shinkawa and K. Shiomi and R. Shiraishi and S. Suzuki and Y. Tajima and N. Taylor and Y. C. Tung and Y. W. Wah and H. Watanabe and T. Wu and T. Yamanaka and H. Y. Yoshida}, doi = {10.1103/PhysRevLett.134.081802}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081802}, shortjournal = {Phys. Rev. Lett.}, title = {Search for the KL→π0νν¯ decay at the J-PARC KOTO experiment}, volume = {134}, year = {2025}, }
• (2025). First measurement of missing energy due to nuclear effects in monoenergetic neutrino charged-current interactions. PRL, 134(8), 081801. (www)

  @article{ , abstract = {We present the first measurement of the missing energy due to nuclear effects in monoenergetic, muon neutrino charged-current interactions on carbon, originating from decay at rest ( ), performed with the J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source liquid scintillator based experiment. Toward characterizing the neutrino interaction, ostensibly or , we define the missing energy as the energy transferred to the nucleus ( ) minus the kinetic energy of the outgoing proton(s), and relate this to visible energy in the detector, . The missing energy, which is naively expected to be zero in the absence of nuclear effects (e.g., nucleon separation energy, Fermi momenta, and final-state interactions), is uniquely sensitive to many aspects of the interaction, and has previously been inaccessible with neutrinos. The shape-only, differential cross section measurement reported, based on a pure double-coincidence kaon decay-at-rest signal (621 total events), provides detailed insight into neutrino-nucleus interactions, allowing even the nuclear orbital shell of the struck nucleon to be inferred. The measurement provides an important benchmark for models and event generators at hundreds of MeV neutrino energies, characterized by the difficult-to-model transition region between neutrino-nucleus and neutrino-nucleon scattering, and relevant for applications in nuclear physics, neutrino oscillation measurements, and Type-II supernova studies.}, archive = {J_PRL}, author = {math xmlns="http://www.w3.org/1998/Math/MathML" display="inline">JSNS2 Collaboration and E. Marzec and S. Ajimura and A. Antonakis and M. Botran and M. K. Cheoun and J. H. Choi and J. W. Choi and J. Y. Choi and T. Dodo and H. Furuta and J. H. Goh and K. Haga and M. Harada and S. Hasegawa and Y. Hino and T. Hiraiwa and W. Hwang and T. Iida and E. Iwai and S. Iwata and H. I. Jang and J. S. Jang and M. C. Jang and H. K. Jeon and S. H. Jeon and K. K. Joo and D. E. Jung and S. K. Kang and Y. Kasugai and T. Kawasaki and E. J. Kim and J. Y. Kim and E. M. Kim and S. Y. Kim and W. Kim and S. B. Kim and H. Kinoshita and T. Konno and K. Kuwata and D. H. Lee and S. Lee and I. T. Lim and C. Little and T. Maruyama and S. Masuda and S. Meigo and S. Monjushiro and D. H. Moon and T. Nakano and M. Niiyama and K. Nishikawa and M. Noumachi and M. Y. Pac and B. J. Park and H. W. Park and J. B. Park and J. S. Park and R. G. Park and S. J. M. Peeters and G. Roellinghoff and C. Rott and J. W. Ryu and K. Sakai and S. Sakamoto and T. Shima and C. D. Shin and J. Spitz and I. Stancu and F. Suekane and Y. Sugaya and K. Suzuya and M. Taira and Y. Takeuchi and W. Wang and J. Waterfield and W. Wei and R. White and Y. Yamaguchi and M. Yeh and I. S. Yeo and C. Yoo and I. Yu and A. Zohaib}, doi = {10.1103/PhysRevLett.134.081801}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081801}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of missing energy due to nuclear effects in monoenergetic neutrino charged-current interactions}, volume = {134}, year = {2025}, }
• (2025). Possible implications of QCD axion dark matter constraints from helioscopes and haloscopes for the string theory landscape. PRL, 134(8), 081602. (www)

  @article{ , abstract = {Laboratory experiments have the capacity to detect the QCD axion in the next decade, and precisely measure its mass, if it composes the majority of the dark matter. In type IIB string theory on Calabi-Yau threefolds in the geometric regime, the QCD axion mass, m a , is strongly correlated with the topological Hodge number h 1 , 1 . We compute m a in a scan of 185965 compactifications of type IIB string theory on toric hypersurface Calabi-Yau threefolds. We compute the range of h 1 , 1 probed by different experiments under the condition that the QCD axion can provide the observed dark matter density with minimal fine-tuning. Taking the experiments DMRadio, ADMX, MADMAX, and BREAD as indicative on different mass ranges, the h 1 , 1 distributions peak near h 1 , 1 = 24.9 , 65.4, 196.8, and 310.9, respectively. We furthermore conclude that, without severe fine-tuning, detection of the QCD axion as dark matter at any mass disfavors 80% of models with h 1 , 1 = 491 , which is thought to have the most known Calabi-Yau threefolds. Measurement of the solar axion mass with IAXO is the dominant probe of all models with h 1 , 1 ≳ 250 . This Letter demonstrates the immense importance of axion detection in experimentally constraining the string landscape.}, archive = {J_PRL}, author = {Naomi Gendler and David J. E. Marsh}, doi = {10.1103/PhysRevLett.134.081602}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081602}, shortjournal = {Phys. Rev. Lett.}, title = {Possible implications of QCD axion dark matter constraints from helioscopes and haloscopes for the string theory landscape}, volume = {134}, year = {2025}, }
• (2025). Oscillons from Q-balls through renormalization. PRL, 134(8), 081601. (www)

  @article{ , abstract = {Using a renormalization-inspired perturbation expansion we show that oscillons in a generic field theory in ( ) dimensions arise as dressed Q-balls of a universal (up to the leading nonlinear order) complex field theory. This theory reveals a close similarity to the integrable complex sine-Gordon model, which possesses exact multi- -balls. We show that excited oscillons, with characteristic modulations of their amplitude, are two-oscillons bound states generated from a two -ball solution.}, archive = {J_PRL}, author = {F. Blaschke and T. Romańczukiewicz and K. Sławińska and A. Wereszczyński}, doi = {10.1103/PhysRevLett.134.081601}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081601}, shortjournal = {Phys. Rev. Lett.}, title = {Oscillons from Q-balls through renormalization}, volume = {134}, year = {2025}, }
• (2025). Single versus the repetitive penrose process in a kerr black hole. PRL, 134(8), 081403. (www)

  @article{ , abstract = {Extracting the rotational energy from a Kerr black hole (BH) is one of the crucial topics in relativistic astrophysics. Here, we give special attention to the Penrose ballistic process based on the fission of a massive particle into two particles and , occurring in the ergosphere of a Kerr BH. Bardeen et al. indicated that for the process to occur, some additional “hydrodynamical forces or superstrong radiation reactions” were needed. Wald and Chandrasekhar further expanded this idea. This animosity convinced Piran and collaborators to move from a simple three-body system characterizing the original Penrose process to a many-body system. This many-body approach was further largely expanded by others, some questionable in their validity. Here, we return to the simplest original Penrose process and show that the solution of the equations of motion, imposing the turning point condition on their trajectories, leads to the rotational energy extraction from the BH expected by Penrose. The efficiency of energy extraction by a single process is quantified for three different single decay processes occurring, respectively, at , and . An interesting repetitive model has been proposed by Misner et al. [ Gravitation (W. H. Freeman, San Francisco, 1973)]. Indeed, it would appear that a repetitive sequence of 246 decays of the above injection process at and the corresponding ones at and could extract 100% of the rotational energy of the BH, so violating energy conservation. The accompanying article, accounting for the existence of the BH irreducible mass, introduces a nonlinear approach that avoids violating energy conservation and leads to a new energy extraction process.}, archive = {J_PRL}, author = {Remo Ruffini and Mikalai Prakapenia and Hernando Quevedo and Shurui Zhang}, doi = {10.1103/PhysRevLett.134.081403}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081403}, shortjournal = {Phys. Rev. Lett.}, title = {Single versus the repetitive penrose process in a kerr black hole}, volume = {134}, year = {2025}, }
• (2025). Black hole spectroscopy in environments: Detectability prospects. PRL, 134(8), 081402. (www)

  @article{ , abstract = {The ringdown phase following a binary black hole coalescence is a powerful tool for measuring properties of the remnant black hole. Future gravitational wave detectors will increase the precision of these measurements and may be sensitive to the environment surrounding the black hole. This work examines how environments affect the ringdown from a binary coalescence. Our analysis shows that for astrophysical parameters and sensitivity of planned detectors, the ringdown signal is indistinguishable from its vacuum counterpart, suggesting that ringdown-only analyses can reliably extract the (redshifted) mass and spin of the remnant black hole. These conclusions include models with spectral instabilities, suggesting that these are not relevant from an observational viewpoint. Deviations from inspiral-only estimates could then enhance the characterisation of environmental effects present during the coalescence.}, archive = {J_PRL}, author = {Thomas F. M. Spieksma and Vitor Cardoso and Gregorio Carullo and Matteo Della Rocca and Francisco Duque}, doi = {10.1103/PhysRevLett.134.081402}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081402}, shortjournal = {Phys. Rev. Lett.}, title = {Black hole spectroscopy in environments: Detectability prospects}, volume = {134}, year = {2025}, }
• (2025). Instability of nonsingular black holes in nonlinear electrodynamics. PRL, 134(8), 081401. (www)

  @article{ , abstract = {We show that nonsingular black holes realized in nonlinear electrodynamics are always prone to Laplacian instability around the center because of a negative squared sound speed in the angular direction. This is the case for both electric and magnetic BHs, where the instability of one of the vector-field perturbations leads to enhancing a dynamical gravitational perturbation in the even-parity sector. Thus, the background regular metric is no longer maintained in a steady state. Our results suggest that the construction of stable, nonsingular black holes with regular centers, if they exist, requires theories beyond nonlinear electrodynamics.}, archive = {J_PRL}, author = {Antonio De Felice and Shinji Tsujikawa}, doi = {10.1103/PhysRevLett.134.081401}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081401}, shortjournal = {Phys. Rev. Lett.}, title = {Instability of nonsingular black holes in nonlinear electrodynamics}, volume = {134}, year = {2025}, }
• (2025). Binary neutron star mergers as the source of the highest energy cosmic rays. PRL, 134(8), 081003. (www)

  @article{ , abstract = {We propose that ultrahigh energy cosmic rays (UHECRs) are produced in binary neutron star (BNS) mergers. This scenario can account for the heretofore inexplicable narrow rigidity range of UHECRs because the jets of BNS mergers are generated by a gravitationally driven dynamo and thus are nearly identical due to the narrow range of BNS masses. Observed UHECRs with energies well beyond 100 EeV can be explained as r -process nuclei, without invoking an exotic source class. Evidence for this mechanism, and its prediction of coincidences between neutrinos above 10 PeV and gravitational waves, are discussed.}, archive = {J_PRL}, author = {Glennys R. Farrar}, doi = {10.1103/PhysRevLett.134.081003}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081003}, shortjournal = {Phys. Rev. Lett.}, title = {Binary neutron star mergers as the source of the highest energy cosmic rays}, volume = {134}, year = {2025}, }
• (2025). Measurement of very-high-energy diffuse gamma-ray emissions from the galactic plane with LHAASO-WCDA. PRL, 134(8), 081002. (www)

  @article{ , abstract = {The diffuse Galactic gamma-ray emission is a very important tool used to study the propagation and interaction of cosmic rays in the Milky Way. In this Letter, we report the measurements of the diffuse emission from the Galactic plane—covering Galactic longitudes from 15° to 235° and latitudes from − 5 ° to + 5 ° , in an energy range of 1 to 25 TeV—made with the Water Cherenkov Detector Array (WCDA) of the Large High Altitude Air Shower Observatory. After the sky regions of known sources are masked, the diffuse emission is detected with 24.6 σ and 9.1 σ significance in the inner Galactic plane ( 15 ° < l < 12 5 ° , | b | < 5 ° ) and outer Galactic plane ( 125 ° < l < 23 5 ° , | b | < 5 ° ), respectively. The WCDA spectra in both regions can be well described by a power-law function, with spectral indices of − 2.67 ± 0.0 5 stat in the inner region and − 2.83 ± 0.1 9 stat in the outer region, respectively. Combined with the Square Kilometer Array (KM2A) measurements at higher energies, a clear softening of the spectrum is found in the inner region, with change of spectral indices by ∼ 0.5 at a break energy around 30 TeV. The fluxes of the diffuse emission are higher by a factor of 1.5–2.7 than the model prediction assuming local cosmic ray spectra and the gas column density, which are consistent with those measured by the KM2A. Along the Galactic longitude, the spatial distribution of the diffuse emission shows deviation from that of the gas column density. The spectral shape of the diffuse emission may vary in different longitude regions. The WCDA measurements bridge the gap between the low-energy measurements by space detectors and the ultra-high-energy observations by KM2A and other experiments. These results suggest that improved modeling of the wideband diffuse emission is required.}, archive = {J_PRL}, author = {LHAASO Collaboration and Zhen Cao and F. Aharonian and Axikegu and Y. X. Bai and Y. W. Bao and D. Bastieri and X. J. Bi and Y. J. Bi and W. Bian and A. V. Bukevich and Q. Cao and W. Y. Cao and Zhe Cao and J. Chang and J. F. Chang and A. M. Chen and E. S. Chen and H. X. Chen and Liang Chen and Lin Chen and Long Chen and M. J. Chen and M. L. Chen and Q. H. Chen and S. Chen and S. H. Chen and S. Z. Chen and T. L. Chen and Y. Chen and N. Cheng and Y. D. Cheng and M. C. Chu and M. Y. Cui and S. W. Cui and X. H. Cui and Y. D. Cui and B. Z. Dai and H. L. Dai and Z. G. Dai and Danzengluobu and X. Q. Dong and K. K. Duan and J. H. Fan and Y. Z. Fan and J. Fang and J. H. Fang and K. Fang and C. F. Feng and H. Feng and L. Feng and S. H. Feng and X. T. Feng and Y. Feng and Y. L. Feng and S. Gabici and B. Gao and C. D. Gao and Q. Gao and W. Gao and W. K. Gao and M. M. Ge and T. T. Ge and L. S. Geng and G. Giacinti and G. H. Gong and Q. B. Gou and M. H. Gu and F. L. Guo and J. Guo and X. L. Guo and Y. Q. Guo and Y. Y. Guo and Y. A. Han and O. A. Hannuksela and M. Hasan and H. H. He and H. N. He and J. Y. He and Y. He and Y. K. Hor and B. W. Hou and C. Hou and X. Hou and H. B. Hu and Q. Hu and S. C. Hu and C. Huang and D. H. Huang and T. Q. Huang and W. J. Huang and X. T. Huang and X. Y. Huang and Y. Huang and Y. Y. Huang and X. L. Ji and H. Y. Jia and K. Jia and H. B. Jiang and K. Jiang and X. W. Jiang and Z. J. Jiang and M. Jin and M. M. Kang and I. Karpikov and D. Khangulyan and D. Kuleshov and K. Kurinov and B. B. Li and C. M. Li and Cheng Li and Cong Li and D. Li and F. Li and H. B. Li and H. C. Li and Jian Li and Jie Li and K. Li and S. D. Li and W. L. Li and X. R. Li and Xin Li and Y. Z. Li and Zhe Li and Zhuo Li and E. W. Liang and Y. F. Liang and S. J. Lin and B. Liu and C. Liu and D. Liu and D. B. Liu and H. Liu and H. D. Liu and J. Liu and J. L. Liu and M. Y. Liu and R. Y. Liu and S. M. Liu and W. Liu and Y. Liu and Y. N. Liu and Q. Luo and Y. Luo and H. K. Lv and B. Q. Ma and L. L. Ma and X. H. Ma and J. R. Mao and Z. Min and W. Mitthumsiri and H. J. Mu and Y. C. Nan and A. Neronov and K. C. Y. Ng and L. J. Ou and P. Pattarakijwanich and Z. Y. Pei and J. C. Qi and M. Y. Qi and B. Q. Qiao and J. J. Qin and A. Raza and D. Ruffolo and A. Sáiz and M. Saeed and D. Semikoz and L. Shao and O. Shchegolev and X. D. Sheng and F. W. Shu and H. C. Song and Yu. V. Stenkin and V. Stepanov and Y. Su and D. X. Sun and Q. N. Sun and X. N. Sun and Z. B. Sun and J. Takata and P. H. T. Tam and Q. W. Tang and R. Tang and Z. B. Tang and W. W. Tian and L. H. Wan and C. Wang and C. B. Wang and G. W. Wang and H. G. Wang and H. H. Wang and J. C. Wang and Kai Wang and L. P. Wang and L. Y. Wang and P. H. Wang and R. Wang and W. Wang and X. G. Wang and X. Y. Wang and Y. Wang and Y. D. Wang and Y. J. Wang and Z. H. Wang and Z. X. Wang and Zhen Wang and Zheng Wang and D. M. Wei and J. J. Wei and Y. J. Wei and T. Wen and C. Y. Wu and H. R. Wu and Q. W. Wu and S. Wu and X. F. Wu and Y. S. Wu and S. Q. Xi and J. Xia and G. M. Xiang and D. X. Xiao and G. Xiao and Y. L. Xin and Y. Xing and D. R. Xiong and Z. Xiong and D. L. Xu and R. F. Xu and R. X. Xu and W. L. Xu and L. Xue and D. H. Yan and J. Z. Yan and T. Yan and C. W. Yang and C. Y. Yang and F. Yang and F. F. Yang and L. L. Yang and M. J. Yang and R. Z. Yang and W. X. Yang and Y. H. Yao and Z. G. Yao and L. Q. Yin and N. Yin and X. H. You and Z. Y. You and Y. H. Yu and Q. Yuan and H. Yue and H. D. Zeng and T. X. Zeng and W. Zeng and M. Zha and B. B. Zhang and F. Zhang and H. Zhang and H. M. Zhang and H. Y. Zhang and J. L. Zhang and Li Zhang and P. F. Zhang and P. P. Zhang and R. Zhang and S. B. Zhang and S. R. Zhang and S. S. Zhang and X. Zhang and X. P. Zhang and Y. F. Zhang and Yi Zhang and Yong Zhang and B. Zhao and J. Zhao and L. Zhao and L. Z. Zhao and S. P. Zhao and X. H. Zhao and F. Zheng and W. J. Zhong and B. Zhou and H. Zhou and J. N. Zhou and M. Zhou and P. Zhou and R. Zhou and X. X. Zhou and B. Y. Zhu and C. G. Zhu and F. R. Zhu and H. Zhu and K. J. Zhu and Y. C. Zou and X. Zuo}, doi = {10.1103/PhysRevLett.134.081002}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081002}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of very-high-energy diffuse gamma-ray emissions from the galactic plane with LHAASO-WCDA}, volume = {134}, year = {2025}, }
• (2025). Constraints on axions from patchy screening of the cosmic microwave background. PRL, 134(8), 081001. (www)

  @article{ , abstract = {The resonant conversion of cosmic microwave background (CMB) photons into axions within large-scale structure induces an anisotropic spectral distortion in CMB temperature maps. Applying state-of-the-art foreground cleaning techniques to Planck CMB observations, we construct maps of axion-induced “patchy screening” of the CMB. We cross-correlate these maps with data from the unWISE galaxy survey and find no evidence of axions. We constrain the axion-photon coupling, at the 95% confidence level for axion masses in the range . These constraints are competitive with the tightest astrophysical axion limits in this mass range and are inferred from robust population-level statistics, which makes them complementary to existing searches that rely on modeling of individual systems.}, archive = {J_PRL}, author = {Samuel Goldstein and Fiona McCarthy and Cristina Mondino and J. Colin Hill and Junwu Huang and Matthew C. Johnson}, doi = {10.1103/PhysRevLett.134.081001}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {081001}, shortjournal = {Phys. Rev. Lett.}, title = {Constraints on axions from patchy screening of the cosmic microwave background}, volume = {134}, year = {2025}, }
• (2025). Communication power of a noisy qubit. PRL, 134(8), 080803. (www)

  @article{ , abstract = {A fundamental limitation of quantum communication is that a single qubit can carry at most one bit of classical information. For an important class of quantum communication channels, known as entanglement breaking, this limitation holds even if the sender and receiver share entangled particles. But does this mean that, for the purpose of communicating classical messages, a noisy entanglement-breaking qubit channel can be replaced by a noisy bit channel? Here we answer the question in the negative. We introduce a game, similar to the Monty Hall problem in classical statistics, where a sender assists a receiver in finding a valuable item (the “prize”) hidden in one of four possible boxes, while avoiding a hazardous item (the “bomb”) hidden in one of the remaining three boxes. We show that no classical strategy using a noisy bit channel can ensure that the bomb is avoided, even if the sender and receiver share arbitrary amounts of randomness. In contrast, communication of a qubit through a class of noisy entanglement-breaking channels, which we call quantum not channels, allows the players to deterministically avoid the bomb and to find the prize with a guaranteed nonzero probability. Our findings show that the communication of classical messages through a noisy entanglement-breaking qubit channel assisted by quantum entanglement cannot, in general, be simulated by communication through a noisy bit channel assisted by classical correlations.}, archive = {J_PRL}, author = {Giulio Chiribella and Saptarshi Roy and Tamal Guha and Sutapa Saha}, doi = {10.1103/PhysRevLett.134.080803}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080803}, shortjournal = {Phys. Rev. Lett.}, title = {Communication power of a noisy qubit}, volume = {134}, year = {2025}, }
• (2025). Enhancing interferometry using weak value amplification with real weak values. PRL, 134(8), 080802. (www)

  @article{ , abstract = {We introduce an ultrasensitive interferometric protocol that combines weak value amplification (WVA) with traditional interferometry. This protocol uses weak value amplification of the relative delay between two paths to enhance interferometric sensitivity. As an example, we demonstrate a proof-of-principle experiment that achieves few-attosecond timing resolution (few nanometer path length resolution) with a double-slit interferometer using only common optical components. Since our example uses only the spatial shift of double-slit interference fringes, its precision is not limited by the timing resolution of the detectors but is instead limited by the fundamental shot noise associated with classical light and the diminished technical noise. We experimentally demonstrate that the signal-to-noise ratio can be improved by one to two orders of magnitude relative to a measurement that does not use WVA. Two key conclusions are drawn: (i) Most conventional interferometric techniques primarily rely on determining the path difference (time delay or longitudinal phase), with their precision constrained by technical noise. Our protocol offers a robust solution for minimizing the technical noise in traditional interferometry, with precision in principle approaching the shot-noise limit. (ii) Although WVA has achieved significant advancements in ultrasensitive longitudinal phase measurement, its applicability is constrained by the need for broad spectral bandwidths and high-resolution spectrometers. Contrary to previous assumptions, we demonstrate that quantum-limited WVA time delay measurements are achievable with narrow band light using real weak values. Thus, the cost-effectiveness and practicality of the proposed protocol using narrow band light broaden the scope of WVA applications. This protocol holds potential for broad applications in optical metrology, quantum optics and quantum information, biomedical imaging, and interferometric telescopes for astrophysics.}, archive = {J_PRL}, author = {Jing-Hui Huang and Kyle M. Jordan and Adetunmise C. Dada and Xiang-Yun Hu and Jeff. S. Lundeen}, doi = {10.1103/PhysRevLett.134.080802}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080802}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing interferometry using weak value amplification with real weak values}, volume = {134}, year = {2025}, }
• (2025). Speeding up quantum measurement using space-time trade-off. PRL, 134(8), 080801. (www)

  @article{ , abstract = {We present a scheme for speeding up quantum measurement. The scheme builds on previous protocols that entangle the system to be measured with ancillary systems. In the idealized situation of perfect entangling operations and no decoherence, it gives an exact space-time trade-off meaning the readout speed increases linearly with the number of ancilla. We verify this scheme is robust against experimental imperfections through numerical modeling of gate noise and readout errors, and under certain circumstances our scheme can even lead to better than linear improvement in the speed of measurement with the number of systems measured. This hardware-agnostic approach is broadly applicable to a range of quantum technology platforms and offers a route to accelerate midcircuit measurement as required for effective quantum error correction.}, archive = {J_PRL}, author = {Christopher Corlett and Ieva Čepaitė and Andrew J. Daley and Cica Gustiani and Gerard Pelegrí and Jonathan D. Pritchard and Noah Linden and Paul Skrzypczyk}, doi = {10.1103/PhysRevLett.134.080801}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080801}, shortjournal = {Phys. Rev. Lett.}, title = {Speeding up quantum measurement using space-time trade-off}, volume = {134}, year = {2025}, }
• (2025). Symmetry induced enhancement in finite-time thermodynamic trade-off relations. PRL, 134(8), 080401. (www)

  @article{ , abstract = {Symmetry imposes constraints on open quantum systems, affecting the dissipative properties in nonequilibrium processes. Superradiance is a typical example in which the decay rate of the system is enhanced via a collective system-bath coupling that respects permutation symmetry. Such a model has also been applied to heat engines. However, a generic framework that addresses the impact of symmetry in finite-time thermodynamics is not well established. Here, we show a symmetry-based framework that describes the fundamental limit of collective enhancement in finite-time thermodynamics. Specifically, we derive a general upper bound on the average jump rate, which quantifies the fundamental speed set by thermodynamic speed limits and trade-off relations. We identify the symmetry condition that achieves the obtained bound, and explicitly construct an open quantum system model that goes beyond the enhancement realized by the conventional superradiance model.}, archive = {J_PRL}, author = {Ken Funo and Hiroyasu Tajima}, doi = {10.1103/PhysRevLett.134.080401}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080401}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry induced enhancement in finite-time thermodynamic trade-off relations}, volume = {134}, year = {2025}, }
• (2025). Simultaneous verification of genuine multipartite nonlocality and full network nonlocality. PRL, 134(8), 080202. (www)

  @article{ , abstract = {Genuine multipartite nonlocality and nonlocality arising in networks composed of several independent sources have been investigated separately. While some genuinely entangled states cannot be verified by violating a single Bell-type inequality, a quantum network consisting of different sources enables the certification of the nonclassicality of all sources. In this Letter, we propose the first method to verify both types of nonlocality simultaneously in a single experiment. We consider a quantum network comprising a bipartite source and a tripartite source. We demonstrate that there are quantum correlations that cannot be simulated if the tripartite source distributes biseparable systems while the bipartite source distributes even stronger-than-quantum systems. These correlations can be used to verify both the genuine multipartite nonlocality of generalized Greenberger-Horne-Zeilinger states and the full network nonlocality that is stronger than all the existing results. Experimentally, we observe both types of nonlocality in a high-fidelity photonic quantum network by violating a single network Bell inequality.}, archive = {J_PRL}, author = {Ning-Ning Wang and Xue Yang and Yan-Han Yang and Chao Zhang and Ming-Xing Luo and Bi-Heng Liu and Yun-Feng Huang and Chuan-Feng Li and Guang-Can Guo}, doi = {10.1103/PhysRevLett.134.080202}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080202}, shortjournal = {Phys. Rev. Lett.}, title = {Simultaneous verification of genuine multipartite nonlocality and full network nonlocality}, volume = {134}, year = {2025}, }
• (2025). Deterministic photonic entanglement arising from non-abelian quantum holonomy. PRL, 134(8), 080201. (www)

  @article{ , abstract = {Realizing deterministic, high-fidelity entangling interactions—of the kind that can be utilized for efficient quantum information processing—between photons remains an elusive goal. Here, we address this long-standing issue by devising a protocol for creating and manipulating highly entangled superpositions of well-controlled states of light by using an on-chip photonic system that has recently been shown to implement three-dimensional, non-Abelian quantum holonomy. Our calculations indicate that a subset of such entangled superpositions are maximally entangled, “volume-law” states, and that the underlying entanglement can be distilled and purified for applications in quantum science. Crucially, we generalize this approach to demonstrate the potentiality of deterministically entangling two arbitrarily high, -dimensional quantum systems, by formally establishing a deep connection between the matrix representations of the unitary quantum holonomy—within energy-degenerate subspaces in which the total excitation number is conserved—and the ( )-dimensional irreducible representations of the rotation operator, where and . Specifically, our protocol deterministically entangles spatially localized modes that are not only distinguishable but are also individually accessible and amenable to state preparation and measurement, and therefore, we envisage that this entangling mechanism could be utilized for deterministic quantum information processing with light.}, archive = {J_PRL}, author = {Aniruddha Bhattacharya and Chandra Raman}, doi = {10.1103/PhysRevLett.134.080201}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080201}, shortjournal = {Phys. Rev. Lett.}, title = {Deterministic photonic entanglement arising from non-abelian quantum holonomy}, volume = {134}, year = {2025}, }
• (2025). Essay: Mapping luminous and dark matter in the universe. PRL, 134(8), 080001. (www)

  @article{ , abstract = {Our standard model of the Universe predicts the distribution of dark matter to 1% at the scales needed for upcoming experiments, yet our predictions for how the luminous matter—which has interactions besides gravity—is distributed remain highly uncertain. Understanding how much gas and stars there are in the Universe and where they preferentially live is challenging, and the uncertainty affects how well we can understand the cosmological model itself. For example, it compromises our ability to tell apart different models for dark energy, the mysterious force driving the accelerated expansion of the Universe. In this Essay, I will touch upon many recent developments that suggest we will be able to overcome this limitation before data from new experiments become available. More excitingly, I will describe how our efforts to model luminous and dark matter jointly will create new possibilities for constraining the physics of supermassive black holes, galaxies, and gas over time.}, archive = {J_PRL}, author = {Nora Elisa Chisari}, doi = {10.1103/PhysRevLett.134.080001}, journal = {Physical Review Letters}, month = {2}, number = {8}, pages = {080001}, shortjournal = {Phys. Rev. Lett.}, title = {Essay: Mapping luminous and dark matter in the universe}, volume = {134}, year = {2025}, }
• (2025). Comment on “Can neural quantum states learn volume-law ground states?”. PRL, 134(7), 079701. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 079701 (2025)}, archive = {J_PRL}, author = {Zakari Denis and Alessandro Sinibaldi and Giuseppe Carleo}, doi = {10.1103/PhysRevLett.134.079701}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {079701}, shortjournal = {Phys. Rev. Lett.}, title = {Comment on “Can neural quantum states learn volume-law ground states?”}, volume = {134}, year = {2025}, }
• (2025). Attraction-enhanced emergence of friction in colloidal matter. PRL, 134(7), 078202. (www)

  @article{ , abstract = {How frictional effects emerge at the microscopic level in particulate materials remains a challenging question, particularly in systems subject to thermal fluctuations due to the transient nature of interparticle contacts. Here, we directly relate particle-level frictional arrest to local coordination in an attractive colloidal model system. We reveal that the orientational dynamics of particles slows down exponentially with increasing coordination number due to the emergence of frictional interactions, the strength of which can be tuned simply by varying the attraction strength. Using a simple computer simulation model, we uncover how the interparticle interactions govern the formation of frictional contacts between particles. Our results establish quantitative relations between friction, coordination, and interparticle interactions. This is a key step toward using interparticle friction to tune the mechanical properties of particulate materials.}, archive = {J_PRL}, author = {Berend van der Meer and Taiki Yanagishima and Roel P. A. Dullens}, doi = {10.1103/PhysRevLett.134.078202}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {078202}, shortjournal = {Phys. Rev. Lett.}, title = {Attraction-enhanced emergence of friction in colloidal matter}, volume = {134}, year = {2025}, }
• (2025). Geometrically frustrated, mechanical metamaterial membranes: Large-scale stress accumulation and size-selective assembly. PRL, 134(7), 078201. (www)

  @article{ , abstract = {We study the effect of geometric frustration on dilational mechanical metamaterial membranes. While shape frustrated elastic plates can only accommodate nonzero Gaussian curvature up to size scales that ultimately vanish with their elastic thickness, we show that frustrated metamembranes accumulate hyperbolic curvatures up to mesoscopic length scales that are ultimately independent of the size of their microscopic constituents. A continuum elastic theory and discrete numerical model describe the size-dependent shape and internal stresses of axisymmetric, trumpetlike frustrated metamembranes, revealing a nontrivial crossover to a much weaker power-law growth in elastic strain energy with size than in frustrated elastic membranes. We study a consequence of this for the self-limiting assembly thermodynamics of frustrated trumpets, showing a severalfold increase in the size range of self-limitation of metamembranes relative to elastic membranes.}, archive = {J_PRL}, author = {Michael Wang and Sourav Roy and Christian Santangelo and Gregory Grason}, doi = {10.1103/PhysRevLett.134.078201}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {078201}, shortjournal = {Phys. Rev. Lett.}, title = {Geometrically frustrated, mechanical metamaterial membranes: Large-scale stress accumulation and size-selective assembly}, volume = {134}, year = {2025}, }
• (2025). Detecting directional coupling in network dynamical systems via kalman’s observability. PRL, 134(7), 077401. (www)

  @article{ , abstract = {Detecting coupling in network dynamical systems from time series is an open problem in the physics of complex systems. In this Letter, we tackle this issue from a control-theoretic perspective. Drawing inspiration from Kalman’s notion of observability, we argue the presence of directional coupling between two units, when is detected as an internal state from the measurement of . We illustrate this approach on a series of analytically tractable systems, showcasing how it overcomes limitations of state-of-the-art methods for network inference.}, archive = {J_PRL}, author = {Rayan Succar and Maurizio Porfiri}, doi = {10.1103/PhysRevLett.134.077401}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {077401}, shortjournal = {Phys. Rev. Lett.}, title = {Detecting directional coupling in network dynamical systems via kalman’s observability}, volume = {134}, year = {2025}, }
• (2025). Large tunneling magnetoresistance in nonvolatile 2D hybrid spin filters. PRL, 134(7), 077001. (www)

  @article{ , abstract = {Ferromagnetic semiconductors offer an efficient way to achieve high spin polarization via spin filtering effect. Large tunneling magnetoresistance (TMR) can then be realized when multiple spin filters are put in series, as recently demonstrated in van der Waals 2D A-type antiferromagnets such as and CrSBr. However, the interlayer antiferromagnetic ground state of these magnets inherently results in a high resistance state at zero field, and this volatile behavior limits potential applications. Here we fabricate hybrid spin filters using 2D ferromagnetic metal and semiconductor , which are nonvolatile as two magnets are magnetically decoupled. We achieve large TMR of around 100%, with its temperature dependence well fitted by the extended Jullière model. Additionally, the devices allow spin injection tuned through bias voltage, and TMR polarity reversals are observed. Our work opens a new route to develop 2D magnetic semiconductor based spintronics.}, archive = {J_PRL}, author = {Xiaoyu Wang and Lihao Zhang and Miao He and Qi Li and Wenqin Song and Kunlin Yang and Shuxi Wang and Takashi Taniguchi and Kenji Watanabe and Lei Zhang and Wu Shi and Yingchun Cheng and Zhe Qu and Jie Pan and Zhe Wang}, doi = {10.1103/PhysRevLett.134.077001}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {077001}, shortjournal = {Phys. Rev. Lett.}, title = {Large tunneling magnetoresistance in nonvolatile 2D hybrid spin filters}, volume = {134}, year = {2025}, }
• (2025). Feshbach resonances in Exciton–Charge-carrier scattering in semiconductor bilayers. PRL, 134(7), 076903. (www)

  @article{ , abstract = {Feshbach resonances play a vital role in the success of cold atoms investigating strongly correlated physics. The recent observation of their solid-state analog in the scattering of holes and intralayer excitons in transition metal dichalcogenides [I. Schwartz et al. , Science 374 , 336 (2021) ] holds compelling promise for bringing fully controllable interactions to the field of semiconductors. Here, we demonstrate how tunneling-induced layer hybridization can lead to the emergence of two distinct classes of Feshbach resonances in atomically thin semiconductors. Based on microscopic scattering theory we show that these two types of Feshbach resonances allow us to tune interactions between electrons and both short-lived intralayer, as well as long-lived interlayer excitons. We predict the exciton-electron scattering phase shift from first principles and show that the exciton-electron coupling is fully tunable from strong to vanishing interactions. The tunability of interactions opens the avenue to explore Bose-Fermi mixtures in solid-state systems in regimes that were previously only accessible in cold atom experiments.}, archive = {J_PRL}, author = {Marcel Wagner and Rafał Ołdziejewski and Félix Rose and Verena Köder and Clemens Kuhlenkamp and Ataç İmamoğlu and Richard Schmidt}, doi = {10.1103/PhysRevLett.134.076903}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076903}, shortjournal = {Phys. Rev. Lett.}, title = {Feshbach resonances in Exciton–Charge-carrier scattering in semiconductor bilayers}, volume = {134}, year = {2025}, }
• (2025). Infrared magnetopolaritons in MoTe2 monolayers and bilayers. PRL, 134(7), 076902. (www)

  @article{ , abstract = {monolayers and bilayers are unique within the family of van der Waals materials since they pave the way toward atomically thin infrared light-matter quantum interfaces, potentially reaching the important telecommunication windows. Here, we report emergent exciton polaritons based on monolayers and bilayers in a low-temperature open microcavity in a joint experiment-theory study. Our experiments clearly evidence both the enhanced oscillator strength and enhanced luminescence of bilayers, signified by a 38% increase of the Rabi splitting and a strongly enhanced relaxation of polaritons to low-energy states. The latter is distinct from polaritons in monolayers, which feature a bottlenecklike relaxation inhibition. Both the polaritonic spin valley locking in monolayers and the spin-layer locking in bilayers are revealed via the Zeeman effect, which we map and control via the light-matter composition of our polaritonic resonances.}, archive = {J_PRL}, author = {Bo Han and Jamie M. Fitzgerald and Lukas Lackner and Roberto Rosati and Martin Esmann and Falk Eilenberger and Takashi Taniguchi and Kenji Watanabe and Marcin Syperek and Ermin Malic and Christian Schneider}, doi = {10.1103/PhysRevLett.134.076902}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076902}, shortjournal = {Phys. Rev. Lett.}, title = {Infrared magnetopolaritons in MoTe2 monolayers and bilayers}, volume = {134}, year = {2025}, }
• (2025). Evidence of athermal metastable phase in a halide perovskite: Optically tracked thermal-breach memory. PRL, 134(7), 076901. (www)

  @article{ , abstract = {Halide perovskite materials have been extensively studied in the last decade because of their impressive optoelectronic properties. However, their one characteristic that is uncommon for semiconductors is that many undergo thermally induced structural phase transitions. The transition is hysteretic, with the hysteresis window marking the boundary of the metastable phase. We have discovered that in methylammonium lead iodide, this hysteretic metastable phase is athermal, meaning it shows almost no temporal phase evolution under isothermal conditions. We also show that a large number of distinguishable metastable states can be prepared following different thermal pathways. Furthermore, under a reversible thermal perturbation, the states in the metastable phase either show return-point memory or undergo a systematic nonrecoverable phase evolution, depending on the thermal history and the sign of the temperature perturbation. Since the phase fraction can be probed with extreme sensitivity via luminescence, we have an optically retrievable memory that reliably records any breach in temperature stability. Such thermal-breach memory in athermal martensites, of which there are numerous examples, may be useful for tagging packages requiring strict temperature control during transportation or preservation.}, archive = {J_PRL}, author = {Kingshuk Mukhuti and Satyaki Kundu and Debasmita Pariari and Deepesh Kalauni and Ashutosh Mohanty and Aniket Bajaj and D. D. Sarma and Bhavtosh Bansal}, doi = {10.1103/PhysRevLett.134.076901}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076901}, shortjournal = {Phys. Rev. Lett.}, title = {Evidence of athermal metastable phase in a halide perovskite: Optically tracked thermal-breach memory}, volume = {134}, year = {2025}, }
• (2025). Ferroelectric spin-orbit valve effect. PRL, 134(7), 076801. (www)

  @article{ , abstract = {In ferroelectric (FE) semiconductors with strong spin-orbit coupling, the electron’s spin direction is locked to its momentum by an intrinsic spin-orbit field (SOF) switchable by ferroelectric polarization. This provides a promising platform for novel nonvolatile spintronic devices. Here, we propose exploiting the switchable SOF to realize a FE spin-orbit valve (FE-SOV), where two FE semiconductors are separated by a thin barrier layer. Because of the locking between the SOF and polarization direction, the conductance of the FE-SOV strongly depends on the relative orientation of polarization of the two FE semiconductors. Using a tight-binding model and density functional theory calculations for FE-SOVs based on two-dimensional FE SnTe and Bi, we demonstrate a giant FE-SOV effect that is characterized by the conductance change of several orders in magnitude. Our work enriches spin-orbit physics of ferroelectrics and proposes a new type of all-electric control of a nonvolatile spin-orbitronic device, which holds promise for future electronic and memory applications.}, archive = {J_PRL}, author = {L. L. Tao and Mingbo Dou and Xianjie Wang and E. Y. Tsymbal}, doi = {10.1103/PhysRevLett.134.076801}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076801}, shortjournal = {Phys. Rev. Lett.}, title = {Ferroelectric spin-orbit valve effect}, volume = {134}, year = {2025}, }
• (2025). Ground state of the s=1 antiferromagnetic heisenberg chain is topologically nontrivial if gapped. PRL, 134(7), 076602. (www)

  @article{ , abstract = {Under the widely accepted but unproven assumption that the one-dimensional antiferromagnetic Heisenberg model has a unique gapped ground state, we prove that the model belongs to a nontrivial symmetry-protected topological phase. In other words, we rigorously rule out the possibility that the model has a unique gapped ground state that is topologically trivial. To be precise, we assume that the models on open finite chains with a boundary magnetic field have unique ground states with a uniform gap and prove that the ground state of the infinite chain has a nontrivial topological index. This further implies the presence of a gapless edge excitation in the model on the half-infinite chain and the existence of a topological phase transition in the model that interpolates between the Heisenberg chain and the trivial model.}, archive = {J_PRL}, author = {Hal Tasaki}, doi = {10.1103/PhysRevLett.134.076602}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076602}, shortjournal = {Phys. Rev. Lett.}, title = {Ground state of the s=1 antiferromagnetic heisenberg chain is topologically nontrivial if gapped}, volume = {134}, year = {2025}, }
• (2025). Continuous transition between bosonic fractional chern insulator and superfluid. PRL, 134(7), 076601. (www)

  @article{ , abstract = {The properties of fractional Chern insulator (FCI) phases and the phase transitions between FCIs and Mott insulators in bosonic systems are well studied. The continuous transitions between FCI and superfluids (SFs), however, despite the inspiring field theoretical predictions [M. Barkeshli and J. McGreevy, Phys. Rev. B 89 , 235116 (2014) ; M. Barkeshli and J. McGreevy, Phys. Rev. B 86 , 075136 (2012) ; M. Barkeshli et al. , Phys. Rev. Lett. 115 , 026802 (2015) ; X.-Y. Song et al. , Phys. Rev. B 109 , 085143 (2024) ; and X.-Y. Song and Y.-H. Zhang, SciPost Phys. 15 , 215 (2023) ], have not been directly verified. The existing numerical results of the FCI-SF transition are either indirect or clearly first order. Here, by simply tuning the bandwidth of the Haldane honeycomb lattice model, we find direct transitions from a bosonic FCI at filling of a flat Chern band to two SF states with bosons condensed at momenta or , respectively. While the transition is first order, the transition is found to be continuous, and the bipartite entanglement entropy at the critical point with the area-law scaling is consistent with the critical theories. Through finite-size criticality analysis, the obtained critical exponents and are both compatible with those of the 3D universality class within numerical uncertainty and possibly more exotic beyond-Landau ones. This Letter thence presents a direct numerical demonstration of a continuous FCI-SF transition between a topologically ordered phase and a spontaneous continuous symmetry-breaking phase, and further indicates the zero-field bosonic FCI might be realized from a SF state by gradually flattening the dispersion of the Chern band, through the (quasi)adiabatic preparation in ultracold atom systems.}, archive = {J_PRL}, author = {Hongyu Lu and Han-Qing Wu and Bin-Bin Chen and Zi Yang Meng}, doi = {10.1103/PhysRevLett.134.076601}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076601}, shortjournal = {Phys. Rev. Lett.}, title = {Continuous transition between bosonic fractional chern insulator and superfluid}, volume = {134}, year = {2025}, }
• (2025). Paradigm for finding d-electron heavy fermions: The case of cr-doped CsFe2As2. PRL, 134(7), 076504. (www)

  @article{ , abstract = {We define a general strategy for finding new heavy-fermionic materials without rare-earth elements: doping a Hund metal with pronounced orbital-selective correlations towards half-filling. We argue that in general band structures, a possible orbital-selective Mott transition is frustrated by interorbital hopping into heavy-fermion behavior—where orbitals provide both the heavy and the light electrons—which is enhanced when approaching half-filling. This phase ultimately disappears due to magnetic correlations, as in a standard Doniach diagram. Experimentally we have hole doped , a Hund metal with 0.5 electrons/Fe away from half-filling, and obtained a heavy fermionic state with the highest Sommerfeld coefficient for Fe pnictides to date ( ), before signatures of an antiferromagnetic phase set in.}, archive = {J_PRL}, author = {Matteo Crispino and Pablo Villar Arribi and Anmol Shukla and Frédéric Hardy and Amir-Abbas Haghighirad and Thomas Wolf and Rolf Heid and Michael Merz and Christoph Meingast and Tommaso Gorni and Adolfo Avella and Luca de’ Medici}, doi = {10.1103/PhysRevLett.134.076504}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076504}, shortjournal = {Phys. Rev. Lett.}, title = {Paradigm for finding d-electron heavy fermions: The case of cr-doped CsFe2As2}, volume = {134}, year = {2025}, }
• (2025). Higher landau-level analogs and signatures of non-abelian states in twisted bilayer MoTe2. PRL, 134(7), 076503. (www)

  @article{ , abstract = {Recent experimental discovery of fractional Chern insulators at zero magnetic field in moiré superlattices has sparked intense interests in bringing Landau level physics to flat Chern bands. In twisted MoTe 2 bilayers ( tMoTe 2 ), recent theoretical and experimental studies have found three consecutive flat Chern bands at twist angle ∼ 2 ° . In this Letter, we investigate whether higher Landau level physics can be found in these consecutive Chern bands. At twist angles 2.00° and 1.89°, we identify four consecutive C = 1 bands for the K valley in tMoTe 2 . By constructing Wannier functions directly from density functional theory (DFT) calculations, a six-orbital model is developed to describe the consecutive Chern bands, with the orbitals forming a honeycomb lattice. Exact diagonalization on top of Hartree-Fock calculations are carried out with the Wannier functions. Especially, when the second moiré miniband is half-filled, signatures of non-Abelian states are found. Our Wannier-based approach in modeling moiré superlattices is faithful to DFT wave functions and can serve as benchmarks for continuum models. The possibility of realizing non-Abelian anyons at zero magnetic field also opens up a new pathway for fault-tolerant quantum information processing.}, archive = {J_PRL}, author = {Chong Wang and Xiao-Wei Zhang and Xiaoyu Liu and Jie Wang and Ting Cao and Di Xiao}, doi = {10.1103/PhysRevLett.134.076503}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076503}, shortjournal = {Phys. Rev. Lett.}, title = {Higher landau-level analogs and signatures of non-abelian states in twisted bilayer MoTe2}, volume = {134}, year = {2025}, }
• (2025). Mott transition and volume law entanglement with neural quantum states. PRL, 134(7), 076502. (www)

  @article{ , abstract = {The interplay between delocalization and repulsive interactions can cause electronic systems to undergo a Mott transition between a metal and an insulator. Here we use neural network hidden fermion determinantal states (HFDS) to uncover this transition in the disordered, fully connected Hubbard model. While dynamical mean-field theory (DMFT) provides exact solutions to physical observables of the model in the thermodynamic limit, our method allows us to directly access the wave function for finite system sizes well beyond the reach of exact diagonalization. We demonstrate how HFDS are able to obtain more accurate results in the metallic regime and in the vicinity of the transition than calculations based on a matrix product state (MPS) ansatz, for which the volume law of entanglement exhibited by the system is prohibitive. We use the HFDS method to calculate the energy and double occupancy, the quasiparticle weight and the energy gap and, importantly, the amplitudes of the wave function that provide a novel insight into this model. Our work paves the way for the study of strongly correlated electron systems with neural quantum states.}, archive = {J_PRL}, author = {Chloé Gauvin-Ndiaye and Joseph Tindall and Javier Robledo Moreno and Antoine Georges}, doi = {10.1103/PhysRevLett.134.076502}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076502}, shortjournal = {Phys. Rev. Lett.}, title = {Mott transition and volume law entanglement with neural quantum states}, volume = {134}, year = {2025}, }
• (2025). Extracting the luttinger parameter from a single wave function. PRL, 134(7), 076501. (www)

  @article{ , abstract = {The low-energy physics of Tomonaga-Luttinger liquids (TLLs) is controlled by the Luttinger parameter. We demonstrate that this parameter can be extracted from a single wave function for one-component TLLs with periodic boundary condition. This method relies on the fact that TLLs are described by conformal field theory in which crosscap states can be constructed. The overlaps between the crosscap states and the ground state as well as some excited states are proved to be universal numbers that directly reveal the Luttinger parameter. In microscopic lattice models, crosscap states are formed by putting each pair of antipodal sites into a maximally entangled state. Analytical and numerical calculations are performed in a few representative models to substantiate the conformal field theory prediction. The extracted Luttinger parameters are generally quite accurate in finite-size systems with moderate lengths, so there is no need to perform data fitting and/or finite-size scaling.}, archive = {J_PRL}, author = {Bi-Yang Tan and Yueshui Zhang and Hua-Chen Zhang and Wei Tang and Lei Wang and Hong-Hao Tu and Ying-Hai Wu}, doi = {10.1103/PhysRevLett.134.076501}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076501}, shortjournal = {Phys. Rev. Lett.}, title = {Extracting the luttinger parameter from a single wave function}, volume = {134}, year = {2025}, }
• (2025). General method to construct flat bands in two-dimensional lattices. PRL, 134(7), 076402. (www)

  @article{ , abstract = {Searching for new materials hosting flat bands is pivotal for exploring strongly correlated effects and designing sensitive quantum devices, but remains challenging. We present a general method for realizing flat bands based on mathematical optimization and symmetry analysis. The method enables the discovery of types of two-dimensional lattices that can host flat bands, in sharp contrast with flat-band lattices predicted previously besides the well-known ones. We further verify the method using first-principles calculations. Our approach provides new insights for the design of flat-band lattices, particularly when aiming to create experimentally feasible configurations.}, archive = {J_PRL}, author = {H. T. Li and T. Z. Ji and R. G. Yan and W. L. Fan and Z. X. Zhang and L. Sun and B. F. Miao and G. Chen and X. G. Wan and H. F. Ding}, doi = {10.1103/PhysRevLett.134.076402}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076402}, shortjournal = {Phys. Rev. Lett.}, title = {General method to construct flat bands in two-dimensional lattices}, volume = {134}, year = {2025}, }
• (2025). Anomalies in the electronic stopping of slow antiprotons in LiF. PRL, 134(7), 076401. (www)

  @article{ , abstract = {We present first-principles theoretical calculations for the electronic stopping power (SP) of both protons and antiprotons in LiF. Our results show the presence of the Barkas effect: a higher stopping for positively charged particles than their negatively charged antiparticles. In contrast, a previous study has predicted an anti-Barkas effect (higher stopping for negative charges) at low velocity [Qi, Bruneval and Maliyov, Phys. Rev. Lett. 128 , 043401 (2022) ]. We explain this discrepancy by showing that this anti-Barkas effect appears for highly symmetric trajectories and disappears when considering trajectories that better reproduce the experimental setup. Our low-velocity results show that the SP of both protons and antiproton vanish for velocities under 0.1 a.u.}, archive = {J_PRL}, author = {Guerda Massillon-JL and Alfredo A. Correa and Xavier Andrade and Emilio Artacho}, doi = {10.1103/PhysRevLett.134.076401}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076401}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalies in the electronic stopping of slow antiprotons in LiF}, volume = {134}, year = {2025}, }
• (2025). Spontaneous localization at a potential saddle point from edge state reconstruction in a quantum hall point contact. PRL, 134(7), 076302. (www)

  @article{ , abstract = {Quantum point contacts (QPCs) are an essential component in mesoscopic devices. Here, we study the transmission of quantum Hall edge modes through a gate-defined QPC in monolayer graphene. We observe resonant tunneling peaks and a nonlinear conductance pattern characteristic of Coulomb-blockaded localized states. The in-plane electric polarizability reveals the states are localized at a classically unstable electrostatic saddle point. We explain this unexpected finding within a self-consistent Thomas-Fermi model, finding that localization of a zero-dimensional state at the saddle point is favored whenever the applied confinement potential is sufficiently soft compared to the Coulomb energy. Our results provide a direct demonstration of Coulomb-driven reconstruction at the boundary of a quantum Hall system.}, archive = {J_PRL}, author = {Liam A. Cohen and Noah L. Samuelson and Taige Wang and Kai Klocke and Cian C. Reeves and Takashi Taniguchi and Kenji Watanabe and Sagar Vijay and Michael P. Zaletel and Andrea F. Young}, doi = {10.1103/PhysRevLett.134.076302}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076302}, shortjournal = {Phys. Rev. Lett.}, title = {Spontaneous localization at a potential saddle point from edge state reconstruction in a quantum hall point contact}, volume = {134}, year = {2025}, }
• (2025). Absence of weak localization on negative curvature surfaces. PRL, 134(7), 076301. (www)

  @article{ , abstract = {The interplay between disorder and quantum interference leads to a wide variety of physical phenomena including celebrated Anderson localization—the complete absence of diffusive transport due to quantum interference between different particle trajectories. In two dimensions, any amount of disorder is thought to induce localization of all states at long enough length scales. In this Letter, we present an argument providing a mechanism for disrupting localization: by tuning the underlying curvature of the manifold on which diffusion takes place. We show that negative curvature manifolds contain a natural infrared cutoff for the probability of self-returning paths. We calculate the Cooperon—directly related to the weak-localization corrections to the conductivity—in hyperbolic space. It is shown that negative curvature leads to a rapid growth in the number of available trajectories a particle can coherently traverse in a given time, reducing the importance of interference effects and restoring diffusive behavior even in the absence of inelastic collisions. We further argue that on certain manifolds with variable curvature the hyperbolic regions dominate due to intermittency and arrest weak localization, which may be of relevance to two-dimensional materials due to surface roughness. This result may be amenable to experimental verification through the use of quantum simulators. Finally, we use results on mixed-curvature gravity by Zel’dovich to argue that our generic result on the absence of weak localization in two dimensions also applies to surfaces of mixed curvature, which may be of relevance to realistic experiments on weakly disordered metallic films on rough substrates.}, archive = {J_PRL}, author = {Jonathan B. Curtis and Prineha Narang and Victor Galitski}, doi = {10.1103/PhysRevLett.134.076301}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076301}, shortjournal = {Phys. Rev. Lett.}, title = {Absence of weak localization on negative curvature surfaces}, volume = {134}, year = {2025}, }
• (2025). Layer-dependent charge-state lifetime of single se vacancies in WSe2. PRL, 134(7), 076201. (www)

  @article{ , abstract = {Defect engineering in two-dimensional semiconductors has been exploited to tune the optoelectronic properties and introduce new quantum states in the band gap. Chalcogen vacancies in transition metal dichalcogenides in particular have been found to strongly impact charge carrier concentration and mobility in 2D transistors as well as feature subgap emission and single-photon response. In this Letter, we investigate the layer-dependent charge-state lifetime of Se vacancies in . In one monolayer , we observe ultrafast charge transfer from the lowest unoccupied orbital of the top Se vacancy to the graphene substrate within measured via the current saturation in scanning tunneling approach curves. For Se vacancies decoupled by transition metal dichalcogenide (TMD) multilayers, we find a subexponential increase of the charge lifetime from in bilayer to a few nanoseconds in four-layer , alongside a reduction of the defect state binding energy. Additionally, we attribute the continuous suppression and energy shift of the in-gap defect state resonances at very close tip-sample distances to a current saturation effect. Our results provide a key measure of the layer-dependent charge transfer rate of chalcogen vacancies in TMDs.}, archive = {J_PRL}, author = {Laric Bobzien and Jonas Allerbeck and Nils Krane and Andres Ortega-Guerrero and Zihao Wang and Daniel E. Cintron Figueroa and Chengye Dong and Carlo A. Pignedoli and Joshua A. Robinson and Bruno Schuler}, doi = {10.1103/PhysRevLett.134.076201}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076201}, shortjournal = {Phys. Rev. Lett.}, title = {Layer-dependent charge-state lifetime of single se vacancies in WSe2}, volume = {134}, year = {2025}, }
• (2025). X-ray signature of the superionic transition in warm dense fcc water ice. PRL, 134(7), 076102. (www)

  @article{ , abstract = {The fcc superionic phase of ice is a key component of the warm dense water phase diagram. While a few x-ray diffraction studies, under dynamic and static compressions, have reported the stability of the fcc structure, the transition to the superionic state has not been investigated in detail. Here, a remarkable thermal volume expansion is disclosed, which is interpreted as being directly related to the superionic transition. This could be achieved by implementing a heating capsule geometry within the laser-heated diamond anvil cell. Fcc ice is recovered metastable at ambient temperature, allowing us to observe that superionicity in the fcc phase emerges at a slightly lower temperature than for the bcc–fcc structural transition. The crossover in volume thermal expansion at the superionic transition agrees with recent ab initio calculations; however, its magnitude is larger than predicted.}, archive = {J_PRL}, author = {Alexis Forestier and Gunnar Weck and Frédéric Datchi and Sandra Ninet and Gaston Garbarino and Mohamed Mezouar and Paul Loubeyre}, doi = {10.1103/PhysRevLett.134.076102}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076102}, shortjournal = {Phys. Rev. Lett.}, title = {X-ray signature of the superionic transition in warm dense fcc water ice}, volume = {134}, year = {2025}, }
• (2025). Switching two-dimensional sliding ferroelectrics by mechanical bending. PRL, 134(7), 076101. (www)

  @article{ , abstract = {Two-dimensional van der Waals materials, possessing a unique stacking degree of freedom, offer an alternative strategy for modulating their properties through interlayer sliding. Controlling the stacking order is crucial for tuning material properties and developing slidetronics-based devices. Here, using machine-learning potentials, we propose a mechanical bending approach to manipulate stacking orders and related properties in sliding ferroelectric h-BN, 3R- MoS 2 , and nonferroelectric bilayer graphene. Our simulations predict the formation of irreversible kinks in bent bilayers, deviating from the expected arclike deformation. This kink formation arises from the interplay between bending energy and interlayer stacking energy. Notably, the bending-induced kink contains a ferroelectric topological domain wall that reverses the polarization of sliding ferroelectrics, a mechanism distinct from the conventional flexoelectric effect. This work proposes an exciting mechanical bending approach to dynamically manipulate the stacking order and associated optical, topological, ferroelectric, and magnetic properties in van der Waals layered materials.}, archive = {J_PRL}, author = {Ri He and Hua Wang and Fenglin Deng and Yuxiang Gao and Bingwen Zhang and Yubai Shi and Run-Wei Li and Zhicheng Zhong}, doi = {10.1103/PhysRevLett.134.076101}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076101}, shortjournal = {Phys. Rev. Lett.}, title = {Switching two-dimensional sliding ferroelectrics by mechanical bending}, volume = {134}, year = {2025}, }
• (2025). Theory of pressure dependence of superconductivity in bilayer nickelate La3Ni2O7. PRL, 134(7), 076001. (www)

  @article{ , abstract = {A recent experiment showed the superconducting transition temperature in the Ruddlesden-Popper bilayer La 3 Ni 2 O 7 decreases monotonically with increasing pressure above 14 GPa. In order to unravel the underlying mechanism for this unusual dependence, we performed theoretical investigations by combining the density functional theory (DFT) and the unbiased functional renormalization group (FRG). Our DFT calculations show that the Fermi pockets are essentially unchanged with increasing pressure (above 14 GPa), but the bandwidth is enlarged, and particularly the interlayer hopping integral between the nickel 3 d 3 z 2 − r 2 orbitals is enhanced. From the DFT band structure, we construct the bilayer tight-binding model in terms of the nickel 3 d 3 z 2 − r 2 and 3 d x 2 − y 2 orbitals. On this basis, we investigate the superconductivity induced by correlation effects by FRG calculations. We find consistently s ± -wave pairing triggered by spin fluctuations, but the latter are weakened by pressure and lead to a decreasing transition temperature versus pressure, in qualitative agreement with the experiment. We emphasize that the itinerancy of the d orbitals is important and captured naturally in our FRG calculations, and we argue that the unusual pressure dependence would be unnatural, if not impossible, in the otherwise local-moment picture of the nickel d orbitals. This sheds light on the pertinent microscopic description, and more importantly the mechanism, of superconductivity in La 3 Ni 2 O 7 .}, archive = {J_PRL}, author = {Kai-Yue Jiang and Yu-Han Cao and Qing-Geng Yang and Hong-Yan Lu and Qiang-Hua Wang}, doi = {10.1103/PhysRevLett.134.076001}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {076001}, shortjournal = {Phys. Rev. Lett.}, title = {Theory of pressure dependence of superconductivity in bilayer nickelate La3Ni2O7}, volume = {134}, year = {2025}, }
• (2025). Ultrafast spin rotation of relativistic lepton beams via terahertz wave in a dielectric-lined waveguide. PRL, 134(7), 075001. (www)

  @article{ , abstract = {Spin rotation is central for the spin manipulation of lepton beams which, in turn, plays an important role in investigation of the properties of spin-polarized lepton beams and the examination of spin-dependent interactions. However, realization of compact and ultrafast spin rotation of lepton beams, between longitudinal and transverse polarizations, still faces significant challenges. Here, we put forward a novel method for ultrafast (picosecond timescale) spin rotation of a relativistic lepton beam via employing a moderate-intensity terahertz (THz) wave in a dielectric-lined waveguide (DLW). The lepton beam undergoes spin precession induced by the THz magnetic field. We find that optimizing the lepton velocity and THz phase velocity in the DLW can mitigate the impact of transverse Lorentz forces on the lepton beam and increase the precession frequency, thereby maintaining the beam quality and enhancing the efficiency of transverse-to-longitudinal spin rotation. The final polarization degree of the lepton beam exceeds 98%, and the energy spread can be improved significantly. Flexibility in adjusting the electromagnetic modes within the DLW adds further potential for spin manipulation and holds promise for advancing the development of spin-polarized particle beams, which has broad applications in materials science and atomic, nuclear, and high-energy physics.}, archive = {J_PRL}, author = {Zhong-Peng Li and Yu Wang and Ting Sun and Feng Wan and Yousef I. Salamin and Mamutjan Ababekri and Qian Zhao and Kun Xue and Ye Tian and Wen-Qing Wei and Jian-Xing Li}, doi = {10.1103/PhysRevLett.134.075001}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {075001}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrafast spin rotation of relativistic lepton beams via terahertz wave in a dielectric-lined waveguide}, volume = {134}, year = {2025}, }
• (2025). Effective transport by 2D turbulence: Vortex-gas theory vs scale-invariant inverse cascade. PRL, 134(7), 074101. (www)

  @article{ , abstract = {The scale-invariant inverse energy cascade is a hallmark of 2D turbulence, with its theoretical energy spectrum observed in both direct numerical simulations (DNS) and laboratory experiments. Under this scale-invariance assumption, the effective diffusivity of a 2D turbulent flow is dimensionally controlled by the energy flux and the friction coefficient only. Surprisingly, however, we show that such scaling predictions are invalidated by numerical solutions of the 2D Navier-Stokes equation forced at intermediate wave number and damped by weak linear or quadratic drag. We derive alternate scaling-laws for the effective diffusivity based on the emergence of intense, isolated vortices causing spatially inhomogeneous frictional dissipation localized within the small vortex cores. The predictions quantitatively match DNS data. This study points to a universal large-scale organization of 2D turbulent flows in physical space, bridging standard 2D Navier-Stokes turbulence with large-scale geophysical turbulence.}, archive = {J_PRL}, author = {Julie Meunier and Basile Gallet}, doi = {10.1103/PhysRevLett.134.074101}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {074101}, shortjournal = {Phys. Rev. Lett.}, title = {Effective transport by 2D turbulence: Vortex-gas theory vs scale-invariant inverse cascade}, volume = {134}, year = {2025}, }
• (2025). Contact angle measurements of the apparent line tension are spurious. PRL, 134(7), 074001. (www)

  @article{ , abstract = {Phenomena in diverse contexts such as wetting, biological assembly, and manufacturing are attributed to the three-phase line tension. However, decades of line tension estimates based on contact angles of droplets controversially span 6 orders of magnitude, raising the question of which measurements are authoritative. Here, we show with experiments and calculations that contact angles fail to estimate line tension regardless of length scale, technique, and measurement quality. Line tension measurements based on contact angles are driven by two distinct and spurious mechanisms: body forces under ideal conditions, and data scatter under noisy conditions.}, archive = {J_PRL}, author = {Beng Hau Tan and Hongjie An}, doi = {10.1103/PhysRevLett.134.074001}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {074001}, shortjournal = {Phys. Rev. Lett.}, title = {Contact angle measurements of the apparent line tension are spurious}, volume = {134}, year = {2025}, }
• (2025). Spatiotemporal steering of nondiffracting wave packets. PRL, 134(7), 073803. (www)

  @article{ , abstract = {We study the dynamics of space-time nondiffracting wave packets, commonly known as light bullets, in a spatiotemporally varying medium. We show that by spatiotemporal refraction, a monochromatic focused beam can be converted to a light bullet that propagates at a given velocity. By further designing the index profile of the spatiotemporal boundary, the group velocity and the propagation direction of the light bullet can be engineered in a programmable way. All effects mentioned above cannot be achieved by spatial or temporal boundaries, and are only possible with spatiotemporal boundaries. These findings provide unique ways to engineer the dynamics of electromagnetic wave packets in space-time. Such wave packets with engineered space-time trajectory may find potential applications in the spatiotemporal control of material properties or particles, or for use as a way to emulate relativistic physics in the laboratory.}, archive = {J_PRL}, author = {Haiwen Wang and Cheng Guo and Shanhui Fan}, doi = {10.1103/PhysRevLett.134.073803}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073803}, shortjournal = {Phys. Rev. Lett.}, title = {Spatiotemporal steering of nondiffracting wave packets}, volume = {134}, year = {2025}, }
• (2025). Vortex interference enables optimal 3D interferometric nanoscopy. PRL, 134(7), 073802. (www)

  @article{ , abstract = {Super-resolution imaging methods that combine interferometric axial (z) analysis with single-molecule localization microscopy (iSMLM) have achieved ultrahigh 3D precision and contributed to the elucidation of important biological ultrastructures. However, their dependence on imaging multiple phase-shifted output channels necessitates complex instrumentation and operation. To solve this problem, we develop an interferometric superresolution microscope capable of optimal direct axial nanoscopy, termed VILM (Vortex Interference Localization Microscopy). Using a pair of vortex phase plates with opposite orientation for each dual-opposed objective lens, the detection point-spread functions (PSFs) adopt a bilobed profile whose rotation encodes the axial position. Thus, direct 3D single-molecule coordinate determination can be achieved with a single output image. By reducing the number of output channels to as few as one and utilizing a simple beam splitter, the imaging system is significantly streamlined, while the optimal iSMLM imaging performance is retained, with axial precision 2 times better than the lateral. The capability of VILM is demonstrated by resolving the architecture of microtubules and probing the organization of tyrosine-phosphorylated signaling proteins in integrin-based cell adhesions.}, archive = {J_PRL}, author = {Wei Wang and Zengxin Huang and Yilin Wang and Hangfeng Li and Pakorn Kanchanawong}, doi = {10.1103/PhysRevLett.134.073802}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073802}, shortjournal = {Phys. Rev. Lett.}, title = {Vortex interference enables optimal 3D interferometric nanoscopy}, volume = {134}, year = {2025}, }
• (2025). Topological pumping of multifrequency solitons. PRL, 134(7), 073801. (www)

  @article{ , abstract = {We report on the topological pumping of quadratic optical solitons, observed through their quantized transport in a dynamic optical potential. A distinctive feature of this system is that the two fields with different frequencies, which together form the quadratic soliton, evolve in separate yet topologically equivalent dynamic optical potentials. Pumping in this system exhibits several notable differences from pumping in cubic media. While Chern indices characterizing quantized transport for uncoupled fundamental and second harmonic waves are nonzero, small-amplitude solitons with narrow spectra do not move, thus revealing a nontopological phase. As the nonlinearity increases, the system undergoes a sharp transition, depending on the velocity of one of the sublattices forming dynamical potential, into the phase where the quantized transport of quadratic solitons governed by nonzero Chern numbers is observed. The power level at which this transition occurs increases with increase of pumping velocity, and the transition is observed even in the regime when the adiabatic approximation no longer applies. Unlike in cubic media, in a quadratic medium neither breakup of topological pumping nor fractional pumping at high power levels are observed.}, archive = {J_PRL}, author = {Yaroslav V. Kartashov and Fangwei Ye and Vladimir V. Konotop}, doi = {10.1103/PhysRevLett.134.073801}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073801}, shortjournal = {Phys. Rev. Lett.}, title = {Topological pumping of multifrequency solitons}, volume = {134}, year = {2025}, }
• (2025). Controlling the dynamics of atomic correlations via the coupling to a dissipative cavity. PRL, 134(7), 073604. (www)

  @article{ , abstract = {We analyze the relaxation dynamics in an open system, composed by a quantum gas of bosons in a lattice interacting via both contact and global interactions. We report the onset of periodic oscillations of the atomic coherences exhibiting hallmarks of synchronization after a quantum quench. The dynamical behavior exhibits the many-body collapse and revival of atomic coherences and emerges from the interplay of the quantum dissipative nature of the cavity field and the presence of a (approximate) strong symmetry in the dissipative system. We further show that the approximate symmetry can dynamically self-organize. We argue that the approximate symmetry can be tailored to obtain long-lived coherences. These insights provide a general recipe to engineer the dynamics of globally interacting systems.}, archive = {J_PRL}, author = {Catalin-Mihai Halati and Ameneh Sheikhan and Giovanna Morigi and Corinna Kollath}, doi = {10.1103/PhysRevLett.134.073604}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073604}, shortjournal = {Phys. Rev. Lett.}, title = {Controlling the dynamics of atomic correlations via the coupling to a dissipative cavity}, volume = {134}, year = {2025}, }
• (2025). Non-gaussian generalized two-mode squeezing: Applications to two-ensemble spin squeezing and beyond. PRL, 134(7), 073603. (www)

  @article{ , abstract = {Bosonic two-mode squeezed states are paradigmatic entangled Gaussian states that have wide utility in quantum information and metrology. Here, we show that the basic structure of these states can be generalized to arbitrary bipartite quantum systems in a manner that allows simultaneous, Heisenberg-limited estimation of two independent parameters for finite-dimensional systems. Further, we show that these general states can always be stabilized by a relatively simple Markovian dissipative process. In the specific case where the two subsystems are ensembles of two-level atoms or spins, our generalized states define a notion of two-mode spin squeezing that is valid beyond the Gaussian limit and that enables true multiparameter estimation. We discuss how generalized Ramsey measurements allow one to reach the two-parameter quantum Cramér-Rao bound, and how the dissipative preparation scheme is compatible with current experiments.}, archive = {J_PRL}, author = {Mikhail Mamaev and Martin Koppenhöfer and Andrew Pocklington and Aashish A. Clerk}, doi = {10.1103/PhysRevLett.134.073603}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073603}, shortjournal = {Phys. Rev. Lett.}, title = {Non-gaussian generalized two-mode squeezing: Applications to two-ensemble spin squeezing and beyond}, volume = {134}, year = {2025}, }
• (2025). Motional sideband asymmetry of a solid-state mechanical resonator at room temperature. PRL, 134(7), 073602. (www)

  @article{ , abstract = {The motional sideband asymmetry of a mechanical oscillator interacting with a laser field can be observed when approaching the quantum ground state, where the zero-point energy of the mechanical oscillator becomes a sizable contribution to its motion. In the context of quantum optomechanics, it allows, in principle, calibration-free inference of the thermal equilibrium of a macroscopic mechanical resonator with its optical bath. At room temperature, this phenomenon has been observed in pioneering experiments using levitated nanoparticles. Measuring this effect with solid-state mechanical resonators has been compounded by thermal intermodulation noise, mirror frequency noise and low quantum cooperativity. Here, we sideband-cool a membrane-in-the-middle system close to the quantum ground state from room temperature and observe motional sideband asymmetry in a dual-homodyne measurement. Sideband thermometry yields a minimum phonon occupancy of n ¯ eff = 9.5 . Our work provides insights into nonlinear optomechanical dynamics at room temperature and facilitates accessible optomechanical quantum technologies without the need for complex feedback control and cryogenic cooling.}, archive = {J_PRL}, author = {Yi Xia and Guanhao Huang and Alberto Beccari and Alessio Zicoschi and Amirali Arabmoheghi and Nils J. Engelsen and Tobias J. Kippenberg}, doi = {10.1103/PhysRevLett.134.073602}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073602}, shortjournal = {Phys. Rev. Lett.}, title = {Motional sideband asymmetry of a solid-state mechanical resonator at room temperature}, volume = {134}, year = {2025}, }
• (2025). Enhanced laser cooling of a mechanical resonator via zero-photon detection. PRL, 134(7), 073601. (www)

  @article{ , abstract = {Throughout quantum science and technology, measurement is used as a powerful resource for nonlinear operations and quantum state engineering. In particular, single-photon detection is commonly employed for quantum-information applications and tests of fundamental physics. By contrast, and perhaps counterintuitively, measurement of the absence of photons also provides useful information, and offers significant potential for a wide range of new experimental directions. Here, we propose and experimentally demonstrate cooling of a mechanical resonator below its laser-cooled mechanical occupation via zero-photon detection on the anti-Stokes scattered optical field and verify this cooling through heterodyne measurements. Our measurements are well captured by a stochastic master equation and the techniques introduced here open new avenues for cooling, quantum thermodynamics, quantum state engineering, and quantum measurement and control.}, archive = {J_PRL}, author = {Evan A. Cryer-Jenkins and Kyle D. Major and Jack Clarke and Georg Enzian and Magdalena Szczykulska and Jinglei Zhang and Arjun Gupta and Anthony C. Leung and Harsh Rathee and Andreas Ø. Svela and Anthony K. C. Tan and Almut Beige and Klaus Mølmer and Michael R. Vanner}, doi = {10.1103/PhysRevLett.134.073601}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073601}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced laser cooling of a mechanical resonator via zero-photon detection}, volume = {134}, year = {2025}, }
• (2025). Attosecond clocking and control of strong field quantum trajectories. PRL, 134(7), 073201. (www)

  @article{ , abstract = {We introduce a quantum trajectory selector method capable of resolving individual quantum trajectories responsible for strong-field phenomena in real time, revealing the dependence of the electron dynamics on the ionization time. Using an attosecond extreme ultraviolet pulse train, we select the moment of ionization and measure the rates of rescattered electron emission and double ionization driven by a phase locked near IR (1.77 or ) field. We show that there is an intensity-dependent shift in the ionization time associated with double ionization, and we clock this shift as it varies by 250 as. The quantum trajectory selector provides a new attosecond paradigm for expanding our understanding of recollision-driven physics.}, archive = {J_PRL}, author = {Andrew J. Piper and Qiaoyi Liu and Abraham Camacho Garibay and Dietrich Kiesewetter and Vyacheslav Leshchenko and Jens E. Bækhøj and Pierre Agostini and Kenneth J. Schafer and Louis F. DiMauro and Yaguo Tang}, doi = {10.1103/PhysRevLett.134.073201}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073201}, shortjournal = {Phys. Rev. Lett.}, title = {Attosecond clocking and control of strong field quantum trajectories}, volume = {134}, year = {2025}, }
• (2025). Photon many-body dispersion: Exchange-correlation functional for strongly coupled light-matter systems. PRL, 134(7), 073002. (www)

  @article{ , abstract = {We introduce an electron-photon exchange-correlation functional for quantum electrodynamical density-functional theory (QEDFT). The approach, photon MBD (pMBD), is inspired by the many-body dispersion (MBD) method for weak intermolecular interactions, which is generalized to include both electronic and photonic (electromagnetic) degrees of freedom on the same footing. We demonstrate that pMBD accurately captures effects that arise in the context of strong light-matter interactions, such as anisotropic electron-photon interactions, beyond single-photon effects, and cavity-modulated van der Waals interactions. Moreover, we show that pMBD is computationally efficient and allows simulations of large complex systems coupled to optical cavities.}, archive = {J_PRL}, author = {Cankut Tasci and Leonardo A. Cunha and Johannes Flick}, doi = {10.1103/PhysRevLett.134.073002}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073002}, shortjournal = {Phys. Rev. Lett.}, title = {Photon many-body dispersion: Exchange-correlation functional for strongly coupled light-matter systems}, volume = {134}, year = {2025}, }
• (2025). Diffractive imaging of transient electronic coherences in molecules with electron vortices. PRL, 134(7), 073001. (www)

  @article{ , abstract = {Direct imaging of transient electronic coherences in molecules has been challenging, with the potential to control electron motions and influence reaction outcomes. We propose a novel time-resolved vortex electron diffraction technique to spatially resolve transient electronic coherences in isolated molecules. By analyzing helical dichroism diffraction signals, the contribution of electronic populations cancels out, isolating the purely electronic coherence signals. This allows direct monitoring of the time evolution and decoherence of transient electronic coherences in molecules.}, archive = {J_PRL}, author = {Haowei Wu and Haiwang Yong}, doi = {10.1103/PhysRevLett.134.073001}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {073001}, shortjournal = {Phys. Rev. Lett.}, title = {Diffractive imaging of transient electronic coherences in molecules with electron vortices}, volume = {134}, year = {2025}, }
• (2025). Light Λ hypernuclei studied with chiral hyperon-nucleon and hyperon-nucleon-nucleon forces. PRL, 134(7), 072502. (www)

  @article{ , abstract = {A study of light Λ hypernuclei in chiral effective field theory is presented. For the first time, chiral Λ NN and Σ NN three-body forces are included consistently. The calculations are performed within the no-core shell model. Results for the separation energies of the hypernuclei H Λ 3 , H Λ 4 / He Λ 4 , He Λ 5 , and Li Λ 7 are given. It is found that the experimental values can be fairly well reproduced once hyperon-nucleon-nucleon three-body forces are taken into account.}, archive = {J_PRL}, author = {Hoai Le and Johann Haidenbauer and Ulf-G. Meißner and Andreas Nogga}, doi = {10.1103/PhysRevLett.134.072502}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {072502}, shortjournal = {Phys. Rev. Lett.}, title = {Light Λ hypernuclei studied with chiral hyperon-nucleon and hyperon-nucleon-nucleon forces}, volume = {134}, year = {2025}, }
• (2025). First measurement of the neutron-emission probability with a surrogate reaction in inverse kinematics at a heavy-ion storage ring. PRL, 134(7), 072501. (www)

  @article{ , abstract = {Neutron-induced reaction cross sections of short-lived nuclei are imperative to understand the origin of heavy elements in stellar nucleosynthesis and for societal applications, but their measurement is extremely complicated due to the radioactivity of the targets involved. One way of overcoming this issue is to combine surrogate reactions with the unique possibilities offered by heavy-ion storage rings. In this work, we describe the first surrogate-reaction experiment in inverse kinematics, which we successfully conducted at the Experimental Storage Ring (ESR) of the GSI/FAIR facility, using the Pb 208 ( p , p ′ ) reaction as a surrogate for neutron capture on Pb 207 . Thanks to the outstanding detection efficiencies possible at the ESR, we were able to measure for the first time the neutron-emission probability as a function of the excitation energy of Pb 208 . We have used this probability to select different descriptions of the γ -ray strength function and nuclear level density, and provide reliable results for the neutron-induced radiative capture cross section of Pb 207 at energies for which no experimental data exist.}, archive = {J_PRL}, author = {M. Sguazzin and B. Jurado and J. Pibernat and J. A. Swartz and M. Grieser and J. Glorius and Yu. A. Litvinov and J. Adamczewski-Musch and P. Alfaurt and P. Ascher and L. Audouin and C. Berthelot and B. Blank and K. Blaum and B. Brückner and S. Dellmann and I. Dillmann and C. Domingo-Pardo and M. Dupuis and P. Erbacher and M. Flayol and O. Forstner and D. Freire-Fernández and M. Gerbaux and J. Giovinazzo and S. Grévy and C. J. Griffin and A. Gumberidze and S. Heil and A. Heinz and R. Hess and D. Kurtulgil and N. Kurz and G. Leckenby and S. Litvinov and B. Lorentz and V. Méot and J. Michaud and S. Pérard and N. Petridis and U. Popp and D. Ramos and R. Reifarth and M. Roche and M. S. Sanjari and R. S. Sidhu and U. Spillmann and M. Steck and Th. Stöhlker and B. Thomas and L. Thulliez and M. Versteegen and B. Włoch}, doi = {10.1103/PhysRevLett.134.072501}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {072501}, shortjournal = {Phys. Rev. Lett.}, title = {First measurement of the neutron-emission probability with a surrogate reaction in inverse kinematics at a heavy-ion storage ring}, volume = {134}, year = {2025}, }
• (2025). Lattice QCD calculation of the subtraction function in forward compton amplitude. PRL, 134(7), 071903. (www)

  @article{ , abstract = {The subtraction function plays a pivotal role in calculations involving the forward Compton amplitude, which is crucial for predicting the Lamb shift in muonic atoms, as well as the proton-neutron mass difference. In this Letter, we present a lattice QCD calculation of the subtraction function using two domain wall fermion gauge ensembles near the physical pion mass. We utilize a recently proposed subtraction point, demonstrating its advantage in mitigating statistical and systematic uncertainties by eliminating the need for ground-state subtraction. Our results reveal significant contributions from intermediate states to the subtraction function. Incorporating these contributions, we compute the proton, neutron, and nucleon isovector subtraction functions at photon momentum transfer . For the proton subtraction function, we compare our lattice results with chiral perturbation theory prediction at low and with the results from the perturbative operator-product expansion at high . Finally, using these subtraction functions as input, we determine their contribution to two-photon exchange effects in the Lamb shift and isovector nucleon electromagnetic self-energy.}, archive = {J_PRL}, author = {Yang Fu and Xu Feng and Lu-Chang Jin and Chuan Liu and Shi-Da Wen}, doi = {10.1103/PhysRevLett.134.071903}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071903}, shortjournal = {Phys. Rev. Lett.}, title = {Lattice QCD calculation of the subtraction function in forward compton amplitude}, volume = {134}, year = {2025}, }
• (2025). Resummation of threshold double logarithms in hadroproduction of heavy quarkonium. PRL, 134(7), 071902. (www)

  @article{ , abstract = {We resum threshold double logarithms that appear in inclusive production of heavy quarkonium. This resolves the catastrophic failure of fixed-order perturbation theory where quarkonium cross sections at large transverse momentum can turn negative due to large radiative corrections. We find that resummation is imperative for describing measured prompt production rates of at large transverse momentum.}, archive = {J_PRL}, author = {Hee Sok Chung and U-Rae Kim and Jungil Lee}, doi = {10.1103/PhysRevLett.134.071902}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071902}, shortjournal = {Phys. Rev. Lett.}, title = {Resummation of threshold double logarithms in hadroproduction of heavy quarkonium}, volume = {134}, year = {2025}, }
• (2025). Transverse force distributions in the proton from lattice QCD. PRL, 134(7), 071901. (www)

  @article{ , abstract = {Single-spin asymmetries observed in polarized deep-inelastic scattering are important probes of hadron structure. The Sivers asymmetry has been the focus of much attention in QCD phenomenology and is yet to be understood at the quark level. In this Letter, we present a lattice QCD calculation of the spatial distribution of a color-Lorentz force acting on the struck quark in a proton. We determine a spin-independent confining force, as well as spin-dependent force distributions with local forces on the order of . These distributions offer a complementary picture of the Sivers asymmetry in transversely polarized deep-inelastic scattering.}, archive = {J_PRL}, author = {QCDSF Collaboration and J. A. Crawford and K. U. Can and R. Horsley and P. E. L Rakow and G. Schierholz and H. Stüben and R. D. Young and J. M. Zanotti}, doi = {10.1103/PhysRevLett.134.071901}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071901}, shortjournal = {Phys. Rev. Lett.}, title = {Transverse force distributions in the proton from lattice QCD}, volume = {134}, year = {2025}, }
• (2025). Search for highly ionizing particles in pp collisions during LHC run 2 using the full MoEDAL detector. PRL, 134(7), 071802. (www)

  @article{ , abstract = {This search for magnetic monopoles (MMs) and high electric charge objects (HECOs) with spins 0, and 1, uses for the first time the full MoEDAL detector, exposed to proton-proton collisions at 13 TeV. The results are interpreted in terms of Drell-Yan and photon-fusion pair production. Mass limits on direct production of MMs of up to 10 Dirac magnetic charges and HECOs with electric charge in the range to , were achieved. The charge limits placed on MM and HECO production are currently the strongest in the world. MoEDAL is the only LHC experiment capable of being directly calibrated for highly ionizing particles using heavy ions and with a detector system dedicated to definitively measuring magnetic charge.}, archive = {J_PRL}, author = {MoEDAL Collaboration and B. Acharya and J. Alexandre and P. Benes and B. Bergmann and S. Bertolucci and A. Bevan and R. Brancaccio and H. Branzas and P. Burian and M. Campbell and S. Cecchini and Y. M. Cho and M. de Montigny and A. De Roeck and J. R. Ellis and M. Fairbairn and D. Felea and M. Frank and J. Hays and A. M. Hirt and D. L.-J. Ho and P. Q. Hung and J. Janecek and M. Kalliokoski and D. H. Lacarrère and C. Leroy and G. Levi and A. Margiotta and R. Maselek and A. Maulik and N. Mauri and N. E. Mavromatos and M. Mieskolainen and L. Millward and V. A. Mitsou and A. Mukhopadhyay and E. Musumeci and I. Ostrovskiy and P.-P. Ouimet and J. Papavassiliou and L. Patrizii and G. E. Păvălaş and J. L. Pinfold and L. A. Popa and V. Popa and M. Pozzato and S. Pospisil and A. Rajantie and R. Ruiz de Austri and Z. Sahnoun and M. Sakellariadou and K. Sakurai and S. Sarkar and G. Semenoff and A. Shaa and G. Sirri and K. Sliwa and R. Soluk and M. Spurio and M. Staelens and M. Suk and M. Tenti and V. Togo and J. A. Tuszyński and A. Upreti and V. Vento and O. Vives}, doi = {10.1103/PhysRevLett.134.071802}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071802}, shortjournal = {Phys. Rev. Lett.}, title = {Search for highly ionizing particles in pp collisions during LHC run 2 using the full MoEDAL detector}, volume = {134}, year = {2025}, }
• (2025). Search for reactor-produced millicharged particles with skipper-CCDs at the CONNIE and atucha-II experiments. PRL, 134(7), 071801. (www)

  @article{ , abstract = {Millicharged particles, proposed by various extensions of the standard model, can be created in pairs by high-energy photons within nuclear reactors and can interact electromagnetically with electrons in matter. Recently, the existence of a plasmon peak in the interaction cross section with silicon in the eV range was highlighted as a promising approach to enhance low-energy sensitivities. The CONNIE and Atucha-II reactor neutrino experiments utilize Skipper-CCD sensors, which enable the detection of interactions in the eV range. We present world-leading limits on the charge of millicharged particles within a mass range spanning 6 orders of magnitude, derived through a comprehensive analysis and the combination of data from both experiments.}, archive = {J_PRL}, author = {CONNIE and Atucha-II Collaborations and Alexis A. Aguilar-Arevalo and Juan Carlos D’Olivo and Youssef Sarkis and Nicolas Avalos and Xavier Bertou and Pablo Bellino and Carla Bonifazi and Ana Botti and Gustavo Cancelo and Juan Estrada and Richard Ford and Kevin Kuk and Andrew Lathrop and Javier Tiffenberg and Mariano Cababié and Brenda A. Cervantes-Vergara and Claudio Chavez and Fernando Chierchie and David Delgado and Eliana Depaoli and João dos Anjos and Herman P. Lima, Jr and Guillermo Fernandez Moroni and Aldo R. Fernandes Neto and Ben Kilminster and Patrick Lemos and Katherine Maslova and Irina Nasteva and Ana Carolina Oliveira and Pedro Ventura and Martin Makler and Agustina Magnoni and Franciole Marinho and Jorge Molina and Diego Stalder and Santiago Perez and Dario Rodrigues and Laura Paulucci and Ivan Sidelnik and Miguel Sofo Haro}, doi = {10.1103/PhysRevLett.134.071801}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for reactor-produced millicharged particles with skipper-CCDs at the CONNIE and atucha-II experiments}, volume = {134}, year = {2025}, }
• (2025). Boundary carrollian conformal field theories and open null strings. PRL, 134(7), 071604. (www)

  @article{ , abstract = {We consider Carrollian conformal field theories in two dimensions and construct the boundary Carrollian conformal algebra (BCCA), opening up innumerable possibilities for further studies, given the growing relevance of Carrollian symmetries. We prove that the BCCA emerges by contracting a single copy of the Virasoro algebra. As an application, we construct, for the first time, open null strings and show that, for Dirichlet boundary conditions, we recover the BCCA as the algebra of constraints. We finally reconstruct our string results by taking the null limit of tensile open strings.}, archive = {J_PRL}, author = {Arjun Bagchi and Pronoy Chakraborty and Shankhadeep Chakrabortty and Stefan Fredenhagen and Daniel Grumiller and Priyadarshini Pandit}, doi = {10.1103/PhysRevLett.134.071604}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071604}, shortjournal = {Phys. Rev. Lett.}, title = {Boundary carrollian conformal field theories and open null strings}, volume = {134}, year = {2025}, }
• (2025). N=8 supergravity from positivity. PRL, 134(7), 071603. (www)

  @article{ , abstract = {The duality between color and kinematics brings many simplifications to the construction of scattering amplitudes. Here, we show that satisfaction of the tree-level Bern-Carrasco-Johansson relations can dramatically simplify loop computations even when the loop-level relations are not explicitly satisfied. We introduce an agglomerative algorithm, color-dual cut tiling, that builds the entire integrand from the simplest on-shell conditions applied to a seed of off-shell integrand information. Specifically, we demonstrate that for two-to-two scattering at three loops in the maximally supersymmetric gauge theory there is sufficient information contained in planar cuts—completely determined by positivity constraints—to generate all of the nonplanar sector. We further make use of the generalized double copy to generate a representation of maximally supersymmetric gravity as a functional of the planar SYM input. We close with comments on generalizations and possible applications of the approach.}, archive = {J_PRL}, author = {John Joseph M. Carrasco and Alex Edison and Nia Robles Del Pino and Suna Zekioğlu}, doi = {10.1103/PhysRevLett.134.071603}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071603}, shortjournal = {Phys. Rev. Lett.}, title = {N=8 supergravity from positivity}, volume = {134}, year = {2025}, }
• (2025). All planar two-loop amplitudes in maximally supersymmetric yang-mills theory. PRL, 134(7), 071602. (www)

  @article{ , abstract = {We calculate the general planar dual-conformally invariant double-pentagon and pentabox integrals in four dimensions. Concretely, we derive onefold integral representations for these elliptic integrals over polylogarithms of weight three. These integral representations allow us to determine the respective symbols using consistency conditions alone. Together with the previously calculated double-box integral, these integrals suffice to express all two-loop planar scattering amplitudes in maximally supersymmetric Yang-Mills theory in four dimensions—which we thus calculate for any number of particles and any helicity configuration.}, archive = {J_PRL}, author = {Anne Spiering and Matthias Wilhelm and Chi Zhang (张驰}, doi = {10.1103/PhysRevLett.134.071602}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071602}, shortjournal = {Phys. Rev. Lett.}, title = {All planar two-loop amplitudes in maximally supersymmetric yang-mills theory}, volume = {134}, year = {2025}, }
• (2025). Supersymmetric localization and nonconformal n=2 supersymmetric yang-mills theories in the perturbative regime. PRL, 134(7), 071601. (www)

  @article{ , abstract = {We examine the relation between supersymmetric localization on and standard QFT results for nonconformal theories in flat space. Specifically, we consider BPS circular Wilson loops in four-dimensional supersonic Yang-Mills theories with massless hypermultiplets in an arbitrary representation such that the function is nonvanishing. On , localization maps this observable into an interacting matrix model. Despite broken conformal symmetry at the quantum level, we show that within a specific regime of validity the matrix model predictions are consistent with perturbation theory in flat space up to order . At this order, the reorganization of Feynman diagrams based on the matrix model potential, which has been widely tested in conformal models, also applies in nonconformal setups and is realized, in perturbative field theory, through highly nontrivial interference mechanisms.}, archive = {J_PRL}, author = {Marco Billò and Luca Griguolo and Alessandro Testa}, doi = {10.1103/PhysRevLett.134.071601}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071601}, shortjournal = {Phys. Rev. Lett.}, title = {Supersymmetric localization and nonconformal n=2 supersymmetric yang-mills theories in the perturbative regime}, volume = {134}, year = {2025}, }
• (2025). Minimum neutron star mass in neutrino-driven supernova explosions. PRL, 134(7), 071403. (www)

  @article{ , abstract = {Supernova theory has struggled to explain the lightest known neutron star candidate with an accurate mass determination, the companion in the eccentric compact binary system . To improve the theoretical lower limit for neutron star birth masses, we perform 3D supernova simulations for five stellar models close to the minimum mass for iron core collapse. We obtain a record-low neutron star mass of and a substantial kick of . Given residual uncertainties in stellar evolution, a neutron star origin for the object remains plausible.}, archive = {J_PRL}, author = {Bernhard Müller and Alexander Heger and Jade Powell}, doi = {10.1103/PhysRevLett.134.071403}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071403}, shortjournal = {Phys. Rev. Lett.}, title = {Minimum neutron star mass in neutrino-driven supernova explosions}, volume = {134}, year = {2025}, }
• (2025). Impact of bulk viscosity on the postmerger gravitational-wave signal from merging neutron stars. PRL, 134(7), 071402. (www)

  @article{ , abstract = {In the violent postmerger of binary neutron-star mergers strong oscillations are present that impact the emitted gravitational-wave (GW) signal. The frequencies, temperatures, and densities involved in these oscillations allow for violations of the chemical equilibrium promoted by weak interactions, thus leading to a nonzero bulk viscosity that can impact dynamics and GW signals. We present the first simulations of binary neutron-star mergers employing the self-consistent and second-order formulation of the equations of relativistic hydrodynamics for dissipative fluids proposed by Müller, Israel, and Stewart. With the spirit of obtaining a first assessment of the impact of bulk viscosity on the structure and radiative efficiency of the merger remnant we adopt a simplified but realistic approach for the viscosity, which we assume to be determined by direct and modified Urca reactions and hence to vary within the stars. At the same time, to compensate for the lack of a precise knowledge about the strength of bulk viscosity, we explore the possible behaviors by considering three different scenarios of low, medium, and high bulk viscosity. In this way, we find that large values of the bulk viscosities damp the collision-and-bounce oscillations that characterize the dynamics of the stellar cores right after the merger. At the same time, large viscosities tend to preserve the deformations in the remnant, thus leading to a comparatively more efficient GW emission and to changes in the postmerger spectrum that can be up to 100 Hz in the case of the most extreme configurations. Overall, our self-consistent results indicate that bulk viscosity increases the energy radiated in GWs soon after the merger by in the (realistic) scenario of small viscosity, and by in the (unrealistic) scenario of large viscosity.}, archive = {J_PRL}, author = {Michail Chabanov and Luciano Rezzolla}, doi = {10.1103/PhysRevLett.134.071402}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071402}, shortjournal = {Phys. Rev. Lett.}, title = {Impact of bulk viscosity on the postmerger gravitational-wave signal from merging neutron stars}, volume = {134}, year = {2025}, }
• (2025). Magnetic-induced force noise in LISA pathfinder free-falling test masses. PRL, 134(7), 071401. (www)

  @article{ , abstract = {LISA Pathfinder was a mission designed to test key technologies required for gravitational wave detection in space. Magnetically driven forces play a key role in the instrument sensitivity in the low-frequency regime, which corresponds to the measurement band of interest for future space-borne gravitational wave observatories. Magnetically induced forces couple to the test mass motion, introducing a contribution to the relative acceleration noise between the free-falling test masses. In this Letter we present the first complete estimate of this term of the instrument performance model. Our results set the magnetic-induced acceleration noise during the February 2017 noise run of at 1 mHz and at 0.1 mHz. We also discuss how the nonstationarities of the interplanetary magnetic field can affect these values during extreme space weather conditions.}, archive = {J_PRL}, author = {M. Armano and H. Audley and J. Baird and P. Binetruy and M. Born and D. Bortoluzzi and E. Castelli and A. Cavalleri and A. Cesarini and A. M. Cruise and K. Danzmann and M. de Deus Silva and I. Diepholz and G. Dixon and R. Dolesi and L. Ferraioli and V. Ferroni and E. D. Fitzsimons and M. Freschi and L. Gesa and D. Giardini and F. Gibert and R. Giusteri and C. Grimani and J. Grzymisch and I. Harrison and M-S Hartig and G. Heinzel and M. Hewitson and D. Hollington and D. Hoyland and M. Hueller and H. Inchauspé and O. Jennrich and P. Jetzer and N. Karnesis and B. Kaune and N. Korsakova and C. J. Killow and L. Liu and J. A. Lobo and J. P. López-Zaragoza and R. Maarschalkerweerd and D. Mance and V. Martín and L. Martin-Polo and F. Martin-Porqueras and J. Martino and P. W. McNamara and J. Mendes and L. Mendes and N. Meshksar and M. Nofrarias and S. Paczkowski and M. Perreur-Lloyd and A. Petiteau and P. Pivato and E. Plagnol and J. Ramos-Castro and J. Reiche and F. Rivas and D. I. Robertson and G. Russano and L. Sala and D. Serrano and J. Slutsky and C. F. Sopuerta and T. Sumner and D. Texier and J. I. Thorpe and D. Vetrugno and S. Vitale and G. Wanner and H. Ward and P. J. Wass and W. J. Weber and L. Wissel and A. Wittchen and P. Zweifel}, doi = {10.1103/PhysRevLett.134.071401}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071401}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic-induced force noise in LISA pathfinder free-falling test masses}, volume = {134}, year = {2025}, }
• (2025). Search for MeV-scale axionlike particles and dark photons with PandaX-4T. PRL, 134(7), 071004. (www)

  @article{ , abstract = {Axionlike particles (ALPs) and dark photons (DPs) are viable dark matter particle candidates. We have searched for possible ALP/DP signals in the PandaX-4T liquid xenon detector using of data. A binned likelihood fit is constructed to search for possible mono-energetic peaks induced by the absorption processes between ALPs/DPs and atomic electrons of xenon. A detailed temporal model of decays associated with xenon isotopes is introduced to constrain the number of background events. No signal excess over background expectations is observed, and we have established the most stringent exclusion limits for most ALP/DP masses across the range of to . The improvement is particularly significant within the mass range of , with the average factor of 3.5 compared to previous results.}, archive = {J_PRL}, author = {PandaX Collaboration and Tao Li and Zihao Bo and Wei Chen and Xun Chen and Yunhua Chen and Zhaokan Cheng and Xiangyi Cui and Yingjie Fan and Deqing Fang and Zhixing Gao and Lisheng Geng and Karl Giboni and Xunan Guo and Xuyuan Guo and Zichao Guo and Chencheng Han and Ke Han and Changda He and Jinrong He and Di Huang and Houqi Huang and Junting Huang and Ruquan Hou and Yu Hou and Xiangdong Ji and Xiangpan Ji and Yonglin Ju and Chenxiang Li and Jiafu Li and Mingchuan Li and Shuaijie Li and Zhiyuan Li and Qing Lin and Jianglai Liu and Congcong Lu and Xiaoying Lu and Lingyin Luo and Yunyang Luo and Wenbo Ma and Yugang Ma and Yajun Mao and Yue Meng and Xuyang Ning and Binyu Pang and Ningchun Qi and Zhicheng Qian and Xiangxiang Ren and Dong Shan and Xiaofeng Shang and Xiyuan Shao and Guofang Shen and Manbin Shen and Wenliang Sun and Yi Tao and Anqing Wang and Guanbo Wang and Hao Wang and Jiamin Wang and Lei Wang and Meng Wang and Qiuhong Wang and Shaobo Wang and Siguang Wang and Wei Wang and Xiuli Wang and Xu Wang and Zhou Wang and Yuehuan Wei and Weihao Wu and Yuan Wu and Mengjiao Xiao and Xiang Xiao and Kaizhi Xiong and Yifan Xu and Shunyu Yao and Binbin Yan and Xiyu Yan and Yong Yang and Peihua Ye and Chunxu Yu and Ying Yuan and Zhe Yuan and Youhui Yun and Xinning Zeng and Minzhen Zhang and Peng Zhang and Shibo Zhang and Shu Zhang and Tao Zhang and Wei Zhang and Yang Zhang and Yingxin Zhang and Yuanyuan Zhang and Li Zhao and Jifang Zhou and Jiaxu Zhou and Jiayi Zhou and Ning Zhou and Xiaopeng Zhou and Yubo Zhou and Zhizhen Zhou}, doi = {10.1103/PhysRevLett.134.071004}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071004}, shortjournal = {Phys. Rev. Lett.}, title = {Search for MeV-scale axionlike particles and dark photons with PandaX-4T}, volume = {134}, year = {2025}, }
• (2025). Sensitivity of JWST to eV-scale decaying axion dark matter. PRL, 134(7), 071003. (www)

  @article{ , abstract = {The recently launched James Webb Space Telescope can resolve eV-scale emission lines arising from dark matter decay. We forecast the end-of-mission sensitivity to the decay of axions, a leading dark matter candidate, in the Milky Way using the blank-sky observations expected during standard operations. Searching for unassociated emission lines will constrain axions in the mass range 0.18 to 2.6 eV with axion-photon couplings g a γ γ ≳ 5.5 × 10 − 12 GeV − 1 . In particular, these results will constrain nucleophobic QCD axions to masses ≲ 0.2 eV .}, archive = {J_PRL}, author = {Sandip Roy and Carlos Blanco and Christopher Dessert and Anirudh Prabhu and Tea Temim}, doi = {10.1103/PhysRevLett.134.071003}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071003}, shortjournal = {Phys. Rev. Lett.}, title = {Sensitivity of JWST to eV-scale decaying axion dark matter}, volume = {134}, year = {2025}, }
• (2025). Hunting dark matter lines in the infrared background with the james webb space telescope. PRL, 134(7), 071002. (www)

  @article{ , abstract = {Dark matter particles with a mass around 1 eV can decay into near-infrared photons. Utilizing available public blank sky observations from the NIRSpec IFU on the James Webb Space Telescope (JWST), we search for a narrow emission line due to decaying dark matter and derive leading constraints in the mass range 0.8–3 eV on the decay rate to photons, and more specifically, on the axion-photon coupling for the case of axionlike particles. We exclude τ < 3.5 × 10 26 s at m DM ≃ 0.8 eV and, in the case of axions, g a γ γ > 1.3 × 10 − 11 GeV − 1 for m a ≃ 2.2 eV . Our results do not rely on dedicated observations, rather we use blank sky observations intended for sky subtraction, and thus our reach may be automatically strengthened as JWST continues to observe.}, archive = {J_PRL}, author = {Ryan Janish and Elena Pinetti}, doi = {10.1103/PhysRevLett.134.071002}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071002}, shortjournal = {Phys. Rev. Lett.}, title = {Hunting dark matter lines in the infrared background with the james webb space telescope}, volume = {134}, year = {2025}, }
• (2025). Plasmon-enhanced direct-detection method for boosted sub-MeV dark matter. PRL, 134(7), 071001. (www)

  @article{ , abstract = {A plasmon, a collective mode of electronic excitation in solid-state detectors, provides a novel way to detect light dark matter (DM). In this work, we present the conditions of DM to produce a plasmon resonance, requiring relativistic velocities for light DM, and generalize the collective excitation framework to account for relativistic DM. As a demonstration, we consider the cosmic ray boosted DM and find that the plasmon resonance can be significantly enhanced in the scenario with a light mediator. Utilizing the first data from the SENSEI experiment with the skipper CCDs at SNOLAB, we obtain a new strong limit on the sub-MeV DM-electron scattering cross section.}, archive = {J_PRL}, author = {Zheng-Liang Liang and Liangliang Su and Lei Wu and Bin Zhu}, doi = {10.1103/PhysRevLett.134.071001}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {071001}, shortjournal = {Phys. Rev. Lett.}, title = {Plasmon-enhanced direct-detection method for boosted sub-MeV dark matter}, volume = {134}, year = {2025}, }
• (2025). Optical quantum memory on macroscopic coherence. PRL, 134(7), 070803. (www)

  @article{ , abstract = {We propose a quantum memory based on the precreated long-lived macroscopic quantum coherence. It is shown that the proposed approach provides new physical properties and methods for retrieval of the signal light fields and improvement of the basic parameters of quantum memory. We demonstrate how the precreated coherence can enable quantum storage with low quantum noise and programmable and on demand retrieval of signal light fields in atomic ensembles with natural inhomogeneous broadening. The feasibility of implementing this proposal in various crystals doped with rare earth ions, as well as in atomic gases with a Raman transition indicates, a new way for the development of optical quantum memory.}, archive = {J_PRL}, author = {S. A. Moiseev and K. I. Gerasimov and M. M. Minnegaliev and E. S. Moiseev}, doi = {10.1103/PhysRevLett.134.070803}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070803}, shortjournal = {Phys. Rev. Lett.}, title = {Optical quantum memory on macroscopic coherence}, volume = {134}, year = {2025}, }
• (2025). Optimal control in large open quantum systems: The case of transmon readout and reset. PRL, 134(7), 070802. (www)

  @article{ , abstract = {We present a framework that combines the adjoint-state method together with reverse-time backpropagation to solve prohibitively large open-system quantum control problems. Our approach enables the optimization of arbitrary cost functions with fully general controls applied on large open quantum systems described by a Lindblad master equation. It is scalable, computationally efficient, and has a low-memory footprint. We apply this framework to optimize two inherently dissipative operations in superconducting qubits which lag behind in terms of fidelity and duration compared to other unitary operations: the dispersive readout and all-microwave reset of a transmon qubit. Our results show that while standard pulses for dispersive readout are nearly optimal, adding a transmon drive during the protocol can yield improvements in fidelity and duration. We further demonstrate a improvement in reset fidelity and duration through pulse shaping, indicating significant potential for enhancement in reset protocols. Our approach can readily be applied to optimize quantum controls in a vast range of applications such as reservoir engineering, autonomous quantum error correction, and leakage-reduction units.}, archive = {J_PRL}, author = {Ronan Gautier and Élie Genois and Alexandre Blais}, doi = {10.1103/PhysRevLett.134.070802}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070802}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal control in large open quantum systems: The case of transmon readout and reset}, volume = {134}, year = {2025}, }
• (2025). Realization of a crosstalk-free two-ion node for long-distance quantum networking. PRL, 134(7), 070801. (www)

  @article{ , abstract = {Trapped atomic ions constitute one of the leading physical platforms for building the quantum repeater nodes to realize large-scale quantum networks. In a long-distance trapped-ion quantum network, it is essential to have crosstalk-free dual-type qubits: one type, called the communication qubit, to establish an entangling interface with telecom photons; and the other type, called the memory qubit, to store quantum information immune from photon scattering under entangling attempts. Here, we report the first experimental implementation of a telecom-compatible and crosstalk-free quantum network node based on two trapped Ca + 40 ions. The memory qubit is encoded on a long-lived metastable level to avoid crosstalk with the communication qubit encoded in another subspace of the same ion species, and a quantum wavelength conversion module is employed to generate heralded ion-photon entanglement over a 12 km fiber. Our work therefore constitutes an important step toward the realization of quantum repeaters and long-distance quantum networks.}, archive = {J_PRL}, author = {P.-C. Lai and Y. Wang and J.-X. Shi and Z.-B. Cui and Z.-Q. Wang and S. Zhang and P.-Y. Liu and Z.-C. Tian and Y.-D. Sun and X.-Y. Chang and B.-X. Qi and Y.-Y. Huang and Z.-C. Zhou and Y.-K. Wu and Y. Xu and Y.-F. Pu and L.-M. Duan}, doi = {10.1103/PhysRevLett.134.070801}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070801}, shortjournal = {Phys. Rev. Lett.}, title = {Realization of a crosstalk-free two-ion node for long-distance quantum networking}, volume = {134}, year = {2025}, }
• (2025). Gate-based quantum simulation of gaussian bosonic circuits on exponentially many modes. PRL, 134(7), 070604. (www)

  @article{ , abstract = {We introduce a framework for simulating, on an ( )-qubit quantum computer, the action of a Gaussian bosonic (GB) circuit on a state over modes. Specifically, we encode the initial bosonic state’s expectation values over quadrature operators (and their covariance matrix) as an input qubit state. This is then evolved by a quantum circuit that effectively implements the symplectic propagators induced by the GB gates. We find families of GB circuits and initial states leading to efficient quantum simulations. For this purpose, we introduce a dictionary that maps between GB and qubit gates such that particle- (non-particle-) preserving GB gates lead to real- (imaginary-) time evolutions at the qubit level. For the special case of particle-preserving circuits, we present a bounded-error-quantum-polynomial time (BQP)-complete GB decision problem, indicating that GB evolutions of Gaussian states on exponentially many modes are as powerful as universal quantum computers. We also perform numerical simulations of an interferometer on modes, illustrating the power of our framework.}, archive = {J_PRL}, author = {Alice Barthe and M. Cerezo and Andrew T. Sornborger and Martín Larocca and Diego García-Martín}, doi = {10.1103/PhysRevLett.134.070604}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070604}, shortjournal = {Phys. Rev. Lett.}, title = {Gate-based quantum simulation of gaussian bosonic circuits on exponentially many modes}, volume = {134}, year = {2025}, }
• (2025). Demonstrating experimentally the encoding and dynamics of an error-correctable logical qubit on a hyperfine-coupled nuclear spin qudit. PRL, 134(7), 070603. (www)

  @article{ , abstract = {The realization of effective quantum error correction protocols remains a central challenge in the development of scalable quantum computers. Employing high-dimensional quantum systems (qudits) can offer more hardware-efficient protocols than qubit-based approaches. Using electron-nuclear double resonance, we implement a logical qubit encoded on the four states of a I = 3 / 2 nuclear spin hyperfine-coupled to an S = 1 / 2 electron spin qubit; the encoding protects against the dominant decoherence mechanism in such systems, i.e., fluctuations of the quantizing magnetic field. We explore the dynamics of the encoded state both under a controlled application of the fluctuation and under natural decoherence processes. Our results confirm the potential of these proposals for practical, implementable, fault-tolerant quantum memories.}, archive = {J_PRL}, author = {Sumin Lim and Mikhail V. Vaganov and Junjie Liu and Arzhang Ardavan}, doi = {10.1103/PhysRevLett.134.070603}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070603}, shortjournal = {Phys. Rev. Lett.}, title = {Demonstrating experimentally the encoding and dynamics of an error-correctable logical qubit on a hyperfine-coupled nuclear spin qudit}, volume = {134}, year = {2025}, }
• (2025). Time-efficient logical operations on quantum low-density parity check codes. PRL, 134(7), 070602. (www)

  @article{ , abstract = {We propose schemes capable of measuring an arbitrary set of commutative logical Pauli operators in time independent of the number of operators. The only condition is commutativity, a fundamental requirement for simultaneous measurements in quantum mechanics. Quantum low-density parity check (qLDPC) codes show great promise for realizing fault-tolerant quantum computing. They are particularly significant for early fault-tolerant technologies as they can encode many logical qubits using relatively few physical qubits. By achieving simultaneous measurements of logical operators, our approaches enable fully parallelized quantum computing, thus minimizing computation time. Our schemes are applicable to any qLDPC codes and maintain the low density of parity checks while measuring multiple logical operators simultaneously. These results enhance the feasibility of applying early fault-tolerant technologies to practical problems.}, archive = {J_PRL}, author = {Guo Zhang and Ying Li}, doi = {10.1103/PhysRevLett.134.070602}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070602}, shortjournal = {Phys. Rev. Lett.}, title = {Time-efficient logical operations on quantum low-density parity check codes}, volume = {134}, year = {2025}, }
• (2025). Synthetic multidimensional aharonov-bohm cages in fock state lattices. PRL, 134(7), 070601. (www)

  @article{ , abstract = {Fock-state lattices, composed of photon number states with infinite Hilbert space, have emerged as a promising platform for simulating high-dimensional physics due to their potential to extend into arbitrarily high dimensions. Here, we demonstrate the construction of multidimensional Fock-state lattices using superconducting quantum circuits. By controlling artificial gauge fields within their internal structures, we investigate flux-induced extreme localization dynamics, such as Aharonov-Bohm caging, extending from 2D to 3D. We also explore the coherent interference of quantum superposition states, achieving extreme localization within specific subspaces assisted by quantum entanglement. Our findings pave the way for manipulating the behavior of a broad class of quantum states in higher-dimensional systems.}, archive = {J_PRL}, author = {Jiajian Zhang and Wenhui Huang and Ji Chu and Jiawei Qiu and Xuandong Sun and Ziyu Tao and Jiawei Zhang and Libo Zhang and Yuxuan Zhou and Yuanzhen Chen and Yang Liu and Song Liu and Youpeng Zhong and Jian-Jian Miao and Jingjing Niu and Dapeng Yu}, doi = {10.1103/PhysRevLett.134.070601}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070601}, shortjournal = {Phys. Rev. Lett.}, title = {Synthetic multidimensional aharonov-bohm cages in fock state lattices}, volume = {134}, year = {2025}, }
• (2025). Stability of mixed-state quantum phases via finite markov length. PRL, 134(7), 070403. (www)

  @article{ , abstract = {For quantum phases of Hamiltonian ground states, the energy gap plays a central role in ensuring the stability of the phase as long as the gap remains finite. We propose Markov length, the length scale at which the quantum conditional mutual information (CMI) decays exponentially, as an equally essential quantity characterizing mixed-state phases and transitions. For a state evolving under a local Lindbladian, we argue that if its Markov length remains finite along the evolution, then it remains in the same phase, meaning there exists another quasilocal Lindbladian evolution that can reverse the former one. We apply this diagnostic to toric code subject to decoherence and show that the Markov length is finite everywhere except at its decodability transition, at which it diverges. CMI in this case can be mapped to the free energy cost of point defects in the random bond Ising model. This implies that the mixed-state phase transition coincides with the decodability transition and also suggests a quasilocal decoding channel.}, archive = {J_PRL}, author = {Shengqi Sang and Timothy H. Hsieh}, doi = {10.1103/PhysRevLett.134.070403}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070403}, shortjournal = {Phys. Rev. Lett.}, title = {Stability of mixed-state quantum phases via finite markov length}, volume = {134}, year = {2025}, }
• (2025). Long-range interacting systems are locally noninteracting. PRL, 134(7), 070402. (www)

  @article{ , abstract = {Enhanced experimental capabilities to control nonlocal and power-law decaying interactions are currently fueling intense research in the domain of quantum many-body physics. Compared to their counterparts with short-ranged interactions, long-range interacting systems display novel physics, such as nonlinear light cones for the propagation of information or inequivalent thermodynamic ensembles. In this work, we consider generic long-range open quantum systems in arbitrary dimensions and focus on the so-called strong long-range regime. We prove that in the thermodynamic limit local properties, captured by reduced quantum states, are described by an emergent noninteracting theory. Here, the dynamics factorizes and the individual constituents of the system evolve independently such that no correlations are generated over time. In this sense, long-range interacting systems are locally noninteracting. This has significant implications for their relaxation behavior, for instance, in relation to the emergence of long-lived quasistationary states or to the absence of thermalization.}, archive = {J_PRL}, author = {Robert Mattes and Igor Lesanovsky and Federico Carollo}, doi = {10.1103/PhysRevLett.134.070402}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070402}, shortjournal = {Phys. Rev. Lett.}, title = {Long-range interacting systems are locally noninteracting}, volume = {134}, year = {2025}, }
• (2025). Efficiently cooling quantum systems with finite resources: Insights from thermodynamic geometry. PRL, 134(7), 070401. (www)

  @article{ , abstract = {Landauer’s limit on heat dissipation during information erasure is critical as devices shrink, requiring optimal pure-state preparation to minimize errors. However, Nernst’s third law states this demands infinite resources in energy, time, or control complexity. We address the challenge of cooling quantum systems with finite resources. Using Markovian collision models, we explore resource trade-offs and present efficient cooling protocols (that are optimal for qubits) for coherent and incoherent control. Leveraging thermodynamic length, we derive bounds on heat dissipation for swap-based strategies and discuss the limitations of preparing pure states efficiently.}, archive = {J_PRL}, author = {Philip Taranto and Patryk Lipka-Bartosik and Nayeli A. Rodríguez-Briones and Martí Perarnau-Llobet and Nicolai Friis and Marcus Huber and Pharnam Bakhshinezhad}, doi = {10.1103/PhysRevLett.134.070401}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070401}, shortjournal = {Phys. Rev. Lett.}, title = {Efficiently cooling quantum systems with finite resources: Insights from thermodynamic geometry}, volume = {134}, year = {2025}, }
• (2025). Experimental quantum advantage in the odd-cycle game. PRL, 134(7), 070201. (www)

  @article{ , abstract = {We report the first experimental demonstration of the odd-cycle game. We entangle two atoms separated by ∼ 2 m , and the players use them to win the odd-cycle game with a probability ∼ 26 σ above that allowed by the best classical strategy. The experiment implements the optimal quantum strategy, is free of loopholes, and achieves 97.8(3)% of the theoretical limit to the quantum winning probability. We perform the associated Bell test and measure a nonlocal content of 0.54(2)—the largest value for physically separate devices, free of the detection loophole, ever observed.}, archive = {J_PRL}, author = {P. Drmota and D. Main and E. M. Ainley and A. Agrawal and G. Araneda and D. P. Nadlinger and B. C. Nichol and R. Srinivas and A. Cabello and D. M. Lucas}, doi = {10.1103/PhysRevLett.134.070201}, journal = {Physical Review Letters}, month = {2}, number = {7}, pages = {070201}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental quantum advantage in the odd-cycle game}, volume = {134}, year = {2025}, }
• (2025). Erratum: Noninductively driven tokamak plasmas at near-unity toroidal beta [Phys. rev. lett. 119, 035001 (2017)]. PRL, 134(6), 069901. (www)

  @article{ , abstract = {Phys. Rev. Lett. 134, 069901 (2025)}, archive = {J_PRL}, author = {D. J. Schlossberg and G. M. Bodner and M. W. Bongard and M. G. Burke and R. J. Fonck and J. M. Perry and J. A. Reusch}, doi = {10.1103/PhysRevLett.134.069901}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {069901}, shortjournal = {Phys. Rev. Lett.}, title = {Erratum: Noninductively driven tokamak plasmas at near-unity toroidal beta [Phys. rev. lett. 119, 035001 (2017)]}, volume = {134}, year = {2025}, }
• (2025). Excitation-inhibition balance controls information encoding in neural populations. PRL, 134(6), 068403. (www)

  @article{ , abstract = {Understanding how the complex connectivity structure of the brain shapes its information-processing capabilities is a long-standing question. By focusing on a paradigmatic architecture, we study how the neural activity of excitatory and inhibitory populations encodes information on external signals. We show that at long times information is maximized at the edge of stability, where inhibition balances excitation, both in linear and nonlinear regimes. In the presence of multiple external signals, this maximum corresponds to the entropy of the input dynamics. By analyzing the case of a prolonged stimulus, we find that stronger inhibition is instead needed to maximize the instantaneous sensitivity, revealing an intrinsic tradeoff between short-time responses and long-time accuracy. In agreement with recent experimental findings, our results pave the way for a deeper information-theoretic understanding of how the balance between excitation and inhibition controls optimal information-processing in neural populations.}, archive = {J_PRL}, author = {Giacomo Barzon and Daniel Maria Busiello and Giorgio Nicoletti}, doi = {10.1103/PhysRevLett.134.068403}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {068403}, shortjournal = {Phys. Rev. Lett.}, title = {Excitation-inhibition balance controls information encoding in neural populations}, volume = {134}, year = {2025}, }
• (2025). Nonequilibrium transitions in a template copying ensemble. PRL, 134(6), 068402. (www)

  @article{ , abstract = {The fuel-driven process of replication in living systems generates distributions of copied entities with varying degrees of copying accuracy. Here we introduce a thermodynamically consistent ensemble for investigating universal population features of template copying systems. In the context of copolymer copying, coarse-graining over molecular details, we establish a phase diagram of copying accuracy. We discover sharp non-equilibrium transitions between populations of random and accurate copies. Maintaining a population of accurate copies requires a minimum energy expenditure that depends on the configurational entropy of copolymer sequences.}, archive = {J_PRL}, author = {Arthur Genthon and Carl D. Modes and Frank Jülicher and Stephan W. Grill}, doi = {10.1103/PhysRevLett.134.068402}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {068402}, shortjournal = {Phys. Rev. Lett.}, title = {Nonequilibrium transitions in a template copying ensemble}, volume = {134}, year = {2025}, }
• (2025). Contractility-driven cell motility against a viscoelastic resistance. PRL, 134(6), 068401. (www)

  @article{ , abstract = {We study a model of contraction-based cell motility inside a microchannel to investigate the regulation of cell polarization and motion by the mechanical resistance of the environment. A positive feedback between the asymmetry of the acto-myosin cortex density and cell motion gives rise to spontaneous symmetry breaking and motility beyond a threshold contractility that depends on the resistance of extracellular medium. In highly viscous environments, we predict bistability under moderate contractility, so that symmetry breaking needs to be activated. In viscoelastic environments, we find the possibility for periodic oscillations in cortex density polarization and velocity. At the boundary between viscous and viscoelastic environments, the cell may cross, bounce back, or become trapped, depending on the viscoelastic relaxation time. These results are summarized in phase diagrams obtained by combining linear stability analysis and numerical simulations.}, archive = {J_PRL}, author = {Tapas Singha and Pierre Sens}, doi = {10.1103/PhysRevLett.134.068401}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {068401}, shortjournal = {Phys. Rev. Lett.}, title = {Contractility-driven cell motility against a viscoelastic resistance}, volume = {134}, year = {2025}, }
• (2025). Phase separation, capillarity, and odd-surface flows in chiral active matter. PRL, 134(6), 068301. (www)

  @article{ , abstract = {Active phase separations evade canonical thermodynamic descriptions and have thus challenged our understanding of coexistence and interfacial phenomena. Considerable progress has been made towards a nonequilibrium theoretical description of these traditionally thermodynamic concepts. Spatial parity symmetry is conspicuously assumed in much of this progress, despite the ubiquity of chirality in experimentally realized systems. In this Letter, we derive a theory for the phase coexistence and interfacial fluctuations of a system that microscopically violates spatial parity. We find suppression of the phase separation as chirality is increased as well as the development of steady-state currents tangential to the interface dividing the phases. These odd flows are irrelevant to stationary interfacial properties, with stability, capillary fluctuations, and surface area minimization determined entirely by the capillary surface tension. Using large-scale Brownian dynamics simulations, we find excellent agreement with our theoretical scaling predictions.}, archive = {J_PRL}, author = {Luke Langford and Ahmad K. Omar}, doi = {10.1103/PhysRevLett.134.068301}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {068301}, shortjournal = {Phys. Rev. Lett.}, title = {Phase separation, capillarity, and odd-surface flows in chiral active matter}, volume = {134}, year = {2025}, }
• (2025). Extending rytov approximation to vector waves for tomography of anisotropic materials. PRL, 134(6), 068101. (www)

  @article{ , abstract = {Liquid crystal phases exhibit distinctive properties due to their unique molecular ordering, making them central to materials science and soft matter physics. Their orientational ordering induces birefringence, which can be detected by optical microscopy. However, the analysis of 3D orientation, material distribution, and anisotropy from scattered light poses significant challenges due to the vector nature of the light-matter interaction. In this study, we formulate a scattering theory based on the Rytov approximation, commonly employed in scalar wave tomography, tailored to accommodate vector waves by modifying the scattering matrix. Using this formulation, we reveal the intricate 3D structure of liquid crystals with multiple topological defects. Specifically, we visualize the 3D structures of topological defects that were indistinguishable using conventional 2D imaging methods.}, archive = {J_PRL}, author = {ChulMin Oh and Herve Hugonnet and Juheon Lee and YongKeun Park}, doi = {10.1103/PhysRevLett.134.068101}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {068101}, shortjournal = {Phys. Rev. Lett.}, title = {Extending rytov approximation to vector waves for tomography of anisotropic materials}, volume = {134}, year = {2025}, }
• (2025). Exact solution of bipartite fluctuations in one-dimensional fermions. PRL, 134(6), 067101. (www)

  @article{ , abstract = {Emergence of hydrodynamics in quantum many-body systems has recently garnered growing interest. The recent experiment of ultracold atoms [J. F. Wienand et al. , Nat. Phys. 20 , 1732 (2024) ] studied emergent hydrodynamics in hard-core bosons using a bipartite fluctuation, which quantifies how the particle number fluctuates in a subsystem. In this Letter, we theoretically study the variance of a bipartite fluctuation in one-dimensional noninteracting fermionic dynamics starting from an alternating state, deriving the exact solution of the variance and its asymptotic linear growth law for the long-time dynamics. To compare the theoretical prediction with the experiment, we generalize our exact solution by incorporating the incompleteness of the initial alternating state, deriving the general linear growth law analytically. We find that it shows good agreement with the experimentally observed variance growth without any fitting parameters. Furthermore, we estimate a timescale for the local equilibration using our exact solution, finding that the timescale is independent of the initial incompleteness. To investigate the interaction effect, we implement numerical studies for the variance growth in interacting fermions, which has yet to be explored experimentally. As a result, we find that the presence of interactions breaks the linear variance growth derived in the noninteracting fermions. Our exact solutions and numerical findings here lay a foundation for growing bipartite fluctuations in quantum many-body dynamics.}, archive = {J_PRL}, author = {Kazuya Fujimoto and Tomohiro Sasamoto}, doi = {10.1103/PhysRevLett.134.067101}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {067101}, shortjournal = {Phys. Rev. Lett.}, title = {Exact solution of bipartite fluctuations in one-dimensional fermions}, volume = {134}, year = {2025}, }
• (2025). Multiplet supercurrents in a josephson circuit. PRL, 134(6), 067001. (www)

  @article{ , abstract = {Multiterminal Josephson circuits have been proposed as a promising platform to host synthetic topological phases of matter, Floquet states, and multiplet supercurrents that are mediated by pairs of Cooper pairs. Here, we explore a Josephson circuit in which three superconducting electrodes are connected through Josephson junctions to a common superconducting island. We demonstrate the dynamic generation of the multiplet supercurrents, which are found to be robust to elevated temperatures and are confirmed by exhibiting the expected Shapiro step quantization under a microwave drive. We also find an unexpected novel supercurrent, which couples a pair of contacts that are both voltage-biased with respect to the common superconducting island. We show that this supercurrent also results from synchronization of the phase dynamics of the device, opening pathways to study the interplay of nonlinear, quantum, and topological physics.}, archive = {J_PRL}, author = {Ethan G. Arnault and John Chiles and Trevyn F. Q. Larson and Chun-Chia Chen and Lingfei Zhao and Kenji Watanabe and Takashi Taniguchi and François Amet and Gleb Finkelstein}, doi = {10.1103/PhysRevLett.134.067001}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {067001}, shortjournal = {Phys. Rev. Lett.}, title = {Multiplet supercurrents in a josephson circuit}, volume = {134}, year = {2025}, }
• (2025). Room-temperature amplified spontaneous emission in two-dimensional WS2 beyond exciton mott transition. PRL, 134(6), 066904. (www)

  @article{ , abstract = {The highly excited electron-hole plasma (EHP) phase is a natural platform for studying amplified spontaneous emission (ASE), yet research into the many-body physics of EHP and ASE in two-dimensional (2D) semiconductors remains limited. Here, we report the first observation of ASE from EHP in 2D semiconductors, evidenced by an unusually sharp enhancement of emissions in suspended bilayer at a threshold power, confirming the transient differential transmission measurements under continuous wave excitations. We modeled the optical dielectric response of varying densities of excited carriers and accurately reproduced the observed emission features across different electron-hole phases from bilayer over a simple Fabry-Pérot cavity. This, together with spatially resolved emissions, confirmed that ASE stems from the degenerate EHP. Our analysis highlights the crucial role of many-body interactions in achieving ASE in 2D EHP. This Letter provides a new insight into the rich physics in EHP and expands the potential for developing advanced 2D semiconductor based optoelectronic devices.}, archive = {J_PRL}, author = {Yan Xu and Yihan Xiang and Meng Shi and Baoxing Zhai and Wei Dai and Ti Wang and Xiaoze Liu and Yiling Yu and Jun He}, doi = {10.1103/PhysRevLett.134.066904}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066904}, shortjournal = {Phys. Rev. Lett.}, title = {Room-temperature amplified spontaneous emission in two-dimensional WS2 beyond exciton mott transition}, volume = {134}, year = {2025}, }
• (2025). Distinct optical excitation mechanisms of a coherent magnon in a van der waals antiferromagnet. PRL, 134(6), 066903. (www)

  @article{ , abstract = {The control of antiferromagnets with ultrashort optical pulses has emerged as a prominent field of research. Tailored laser excitation can launch coherent spin waves at terahertz frequencies, yet a comprehensive description of their generation mechanisms is still lacking despite extensive efforts. Using terahertz emission spectroscopy, we investigate the generation of a coherent magnon mode in the van der Waals antiferromagnet NiPS 3 under a range of photoexcitation conditions. By tuning the pump photon energy from transparency to resonant with a d − d transition, we reveal a striking change in the coherent magnon’s dependence on the pump polarization, indicating two distinct excitation mechanisms. Our findings provide a strategy for the manipulation of magnetic modes via photoexcitation around subgap electronic states.}, archive = {J_PRL}, author = {Clifford J. Allington and Carina A. Belvin and Urban F. P. Seifert and Mengxing Ye and Tommy Tai and Edoardo Baldini and Suhan Son and Junghyun Kim and Jaena Park and Je-Geun Park and Leon Balents and Nuh Gedik}, doi = {10.1103/PhysRevLett.134.066903}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066903}, shortjournal = {Phys. Rev. Lett.}, title = {Distinct optical excitation mechanisms of a coherent magnon in a van der waals antiferromagnet}, volume = {134}, year = {2025}, }
• (2025). Tunable spatiotemporal orders in driven insulators. PRL, 134(6), 066902. (www)

  @article{ , abstract = {We show that driving optical phonons above a threshold fluence induces spatiotemporal orders, where material properties oscillate at an incommensurate wave vector in space and at half the drive frequency in time. The order is robust against temperature on timescales much larger than the lifetime of the excited modes and can be accompanied by a static modulation. We make predictions for time-resolved diffraction and provide estimates for candidate materials. Our results show the possibility of using THz waves in solids to realize tunable incommensurate orders on the nanoscale.}, archive = {J_PRL}, author = {Daniel Kaplan and Pavel A. Volkov and Ahana Chakraborty and Zekun Zhuang and Premala Chandra}, doi = {10.1103/PhysRevLett.134.066902}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066902}, shortjournal = {Phys. Rev. Lett.}, title = {Tunable spatiotemporal orders in driven insulators}, volume = {134}, year = {2025}, }
• (2025). Optical absorption in indirect semiconductor to semimetal PtSe2 arises from direct transitions. PRL, 134(6), 066901. (www)

  @article{ , abstract = {is a van der Waals material transitioning from an indirect band gap semiconductor to a semimetal with increasing thickness. Its absorption threshold has been conjectured to originate from interband indirect transitions. By quantitative comparison between broadband (0.8–3.0 eV) optical absorption of high-quality exfoliated crystals and DFT ab initio simulations, we prove instead that the optical absorption arises only from direct transitions. This understanding allows us to shed light on the semiconductor-to-semimetal transition in an emblematic strongly thickness-dependent 2D material, and to explore the effect of stacking and excitons on the optical absorption.}, archive = {J_PRL}, author = {Marin Tharrault and Sabrine Ayari and Mehdi Arfaoui and Eva Desgué and Romaric Le Goff and Pascal Morfin and José Palomo and Michael Rosticher and Sihem Jaziri and Bernard Plaçais and Pierre Legagneux and Francesca Carosella and Christophe Voisin and Robson Ferreira and Emmanuel Baudin}, doi = {10.1103/PhysRevLett.134.066901}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066901}, shortjournal = {Phys. Rev. Lett.}, title = {Optical absorption in indirect semiconductor to semimetal PtSe2 arises from direct transitions}, volume = {134}, year = {2025}, }
• (2025). Mechanism of type-II multiferroicity in pure and al-doped CuFeO2. PRL, 134(6), 066801. (www)

  @article{ , abstract = {Type-II multiferroicity, where electric polarization is induced by specific spin patterns, is crucial in fundamental physics and advanced spintronics. However, the spin model and magnetoelectric coupling mechanisms in prototypical type-II multiferroic CuFeO 2 and Al-doped CuFeO 2 remain unclear. Here, by considering both spin and alloy degrees of freedom, we develop a magnetic cluster expansion method, which considers all symmetry allowed interactions. Applying such method, we not only obtain realistic spin model that can correctly reproduce observations for both CuFeO 2 and CuFe 1 − x Al x O 2 , but also revisit well-known theories of the original spin-current (SC) model and p − d hybridization model. Specifically, we find that (i) a previously overlooked biquadratic interaction is critical to reproduce the ↑ ↑ ↓ ↓ ground state and excited states of CuFeO 2 ; (ii) the combination of absent biquadratic interaction and increased magnetic frustration around Al dopants stabilizes the proper screw state; and (iii) it is the generalized spin-current (GSC) model that can correctly characterize the multiferroicity of CuFeO 2 . These findings have broader implications for understanding novel magnetoelectric couplings in, e.g., monolayer multiferroic NiI 2 .}, archive = {J_PRL}, author = {Weiqin Zhu and Panshuo Wang and Haoran Zhu and Haiyan Zhu and Xueyang Li and Jun Zhao and Changsong Xu and Hongjun Xiang}, doi = {10.1103/PhysRevLett.134.066801}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066801}, shortjournal = {Phys. Rev. Lett.}, title = {Mechanism of type-II multiferroicity in pure and al-doped CuFeO2}, volume = {134}, year = {2025}, }
• (2025). Large spin-orbit torque in a-plane α−Fe2O3/Pt bilayers. PRL, 134(6), 066701. (www)

  @article{ , abstract = {Realization of efficient spin-orbit torque switching of the Néel vector in insulating antiferromagnets is a challenge, often complicated by spurious effects. Quantifying the spin-orbit torques in antiferromagnet or heavy metal heterostructures is an important first step toward this goal. Here, we employ magneto-optic techniques to study dampinglike spin-orbit torque (DL-SOT) in -plane (hematite) with a Pt spin-orbit overlayer. We find that the DL-SOT efficiency is 2 orders of magnitude larger than reported in - and -plane hematite/Pt using harmonic Hall techniques. The large magnitude of DL-SOT is supported by direct imaging of current-induced motion of antiferromagnetic domains that happens at moderate current densities. Our study introduces a new method for quantifying spin-orbit torque in antiferromagnets with a small canted moment and identifies -plane as a promising candidate to realize efficient SOT switching.}, archive = {J_PRL}, author = {Igor Lyalin and Hantao Zhang and Justin Michel and Daniel Russell and Fengyuan Yang and Ran Cheng and Roland K. Kawakami}, doi = {10.1103/PhysRevLett.134.066701}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066701}, shortjournal = {Phys. Rev. Lett.}, title = {Large spin-orbit torque in a-plane α−Fe2O3/Pt bilayers}, volume = {134}, year = {2025}, }
• (2025). Observation of temperature-independent anomalous hall effect in thin bismuth from near absolute zero to 300 k temperature. PRL, 134(6), 066603. (www)

  @article{ , abstract = {We report our discovery of a temperature-independent anomalous Hall effect (AHE) from 15 mK to 300 K temperature occurring in a pure bismuth transport device whose average thickness is 68 nm. This surprising behavior is accompanied with an expected temperature-dependent longitudinal resistance consistent with semimetallic bismuth. However, it surprisingly showed no hint of a magnetoresistance for magnetic fields between ± 30 T . Even though bismuth is a diamagnetic material that a priori does not break time-reversal symmetry, our analysis of the reconstructed conductivities points toward the AHE to be of the intrinsic type that does not emanate from magnetic impurities. Finally, as pure bismuth has been shown numerically to host a Berry curvature at its surface that breaks inversion symmetry, we propose it as a possible explanation for the temperature-independent AHE observed here.}, archive = {J_PRL}, author = {Oulin Yu and F. Boivin and A. Silberztein and G. Gervais}, doi = {10.1103/PhysRevLett.134.066603}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066603}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of temperature-independent anomalous hall effect in thin bismuth from near absolute zero to 300 k temperature}, volume = {134}, year = {2025}, }
• (2025). Topological exciton density wave in monolayer WSe2. PRL, 134(6), 066602. (www)

  @article{ , abstract = {Based on the first-principles calculations coupled with the Bethe-Salpeter equation, the topological exciton density wave is investigated in two-dimensional monolayer . We find that the topological excitonic insulator phase can exist in monolayer , and it is robust against in-plane strain. In this system, the energy minimum of exciton bands is shifted to a finite in-plane momentum, forming a Fulde-Ferrell-Larkin-Ovchinnikov-like state. Using the Gross-Pitaevskii equations, stripe-patterned exciton density waves with a nonzero velocity emerge in monolayer . Our findings pave a new way for exploring the interplay between electron correlation and nontrivial topology.}, archive = {J_PRL}, author = {Shan Dong and Yingda Chen and Hongwei Qu and Wen-Kai Lou and Kai Chang}, doi = {10.1103/PhysRevLett.134.066602}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066602}, shortjournal = {Phys. Rev. Lett.}, title = {Topological exciton density wave in monolayer WSe2}, volume = {134}, year = {2025}, }
• (2025). Multiple chern bands in twisted MoTe2 and possible non-abelian states. PRL, 134(6), 066601. (www)

  @article{ , abstract = {We investigate the moiré band structures and a possible even-denominator fractional quantum Hall state in small angle twisted bilayer , using combined large-scale local basis density functional theory calculation and continuum model exact diagonalization. Via large-scale first-principles calculations at , we find a sequence of (Chern number in the K valley) moiré Chern bands in analogy to Landau levels. By constructing the continuum model with multiple Chern bands, we undertake a band-projected exact diagonalization using an unscreened Coulomb repulsion to identify possible non-Abelian states near twist angle at the half filling of second moiré band.}, archive = {J_PRL}, author = {Cheng Xu and Ning Mao and Tiansheng Zeng and Yang Zhang}, doi = {10.1103/PhysRevLett.134.066601}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066601}, shortjournal = {Phys. Rev. Lett.}, title = {Multiple chern bands in twisted MoTe2 and possible non-abelian states}, volume = {134}, year = {2025}, }
• (2025). Magnetic phase diagram of the three-dimensional doped hubbard model. PRL, 134(6), 066502. (www)

  @article{ , abstract = {We establish the phase diagram of the Hubbard model on a cubic lattice for a wide range of temperatures, dopings, and interaction strengths, considering both commensurate and incommensurate magnetic orders. We use the dynamical mean-field theory together with an efficient method to compute the free energy which enable the determination of the correct ordering vectors. Besides an antiferromagnetic state close to half filling, we identify a number of different magnetic spiral phases with ordering vectors , and , as well as a region with close competition between them, hinting at spatial phase separation or at the onset of a stripe phase. Additionally, we extensively study several thermodynamic properties with direct relevance to cold-atom experiments: the entropy, energy, and double occupancy.}, archive = {J_PRL}, author = {Liam Rampon and Fedor Šimkovic, IV and Michel Ferrero}, doi = {10.1103/PhysRevLett.134.066502}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066502}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic phase diagram of the three-dimensional doped hubbard model}, volume = {134}, year = {2025}, }
• (2025). Strain-induced enhancement of the charge density wave in the kagome metal ScV6Sn6. PRL, 134(6), 066501. (www)

  @article{ , abstract = {The kagome geometry is an example of a frustrated configuration in which rich physics takes place, including the emergence of superconductivity and charge density wave (CDW). Among the kagome metals, hosts an unconventional CDW, with its electronic order showing a different periodicity from the leading lattice instability. In this material, a CDW-softened flat phonon band has a second-order collapse at the same time that the first-order transition occurs. This phonon band originates from the out-of-plane vibrations of the Sc and Sn atoms, and it is at the base of the electron-phonon-coupling driven CDW phase of . Here we use uniaxial strain to tune the frequency of the CDW amplitude mode, which originates from the collapse of the flat phonon band, tracking its evolution via time-resolved optical spectroscopy and first-principles calculations. Our findings emphasize the capability to induce an enhancement of the unconventional CDW properties in kagome metal through control of strain.}, archive = {J_PRL}, author = {Manuel Tuniz and Armando Consiglio and Ganesh Pokharel and Fulvio Parmigiani and Titus Neupert and Ronny Thomale and Sandeep Kumar Chaluvadi and Pasquale Orgiani and Giorgio Sangiovanni and Stephen D. Wilson and Ivana Vobornik and Federico Salvador and Federico Cilento and Domenico Di Sante and Federico Mazzola}, doi = {10.1103/PhysRevLett.134.066501}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066501}, shortjournal = {Phys. Rev. Lett.}, title = {Strain-induced enhancement of the charge density wave in the kagome metal ScV6Sn6}, volume = {134}, year = {2025}, }
• (2025). Spectroscopic evidence for possible quantum spin liquid behavior in a two-dimensional mott insulator. PRL, 134(6), 066402. (www)

  @article{ , abstract = {Mott insulators with localized magnetic moments will exhibit a quantum spin liquid state when the quantum fluctuations are strong enough to suppress the ordering of the spins. Such an entangled state will give rise to collective excitations, in which spin and charge information are carried separately. Our angle-resolved photoemission spectroscopy measurements on single-layer show a flat band around the zone center and a gap opening of about 200 meV in the low temperature, indicating 2D Mott insulating nature in the system. This flat band is dispersionless in momentum space but shows anomalously broad width around the zone center and the spectral weight decays rapidly as momentum increases. The observation is described as a spectral continuum from electron fractionalization, corroborated by a low energy effective model. The intensity of the flat band is reduced by surface doping with magnetic adatoms and the gap is closing, a result from the interaction between spin impurities coupled with spinons and the chargons, which gives rise to a charge redistribution. Doping with nonmagnetic impurities behaves differently as the chemical potential shift dominates. These findings provide insight into the quantum spin liquid states of strongly correlated electrons on 2D triangular lattices.}, archive = {J_PRL}, author = {Haiyang Chen and Fo-Hong Wang and Qiang Gao and Xue-Jian Gao and Zhenhua Chen and Yaobo Huang and Kam Tuen Law and Xiao Yan Xu and Peng Chen}, doi = {10.1103/PhysRevLett.134.066402}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066402}, shortjournal = {Phys. Rev. Lett.}, title = {Spectroscopic evidence for possible quantum spin liquid behavior in a two-dimensional mott insulator}, volume = {134}, year = {2025}, }
• (2025). Revisiting the formulation of charged defect in solids. PRL, 134(6), 066401. (www)

  @article{ , abstract = {Defect physics is at the heart of microelectronics. By keeping track of the reference energy in total energy calculations, we explicitly show that the “potential alignment” correction vanishes, and the classic Makov-Payne correction yields accurate results. From linear response theory, we further formulate an accurate expression for the quadrupole correction. Application to numerous defects including anisotropic material yields accurate formation energies in small supercells, and the historically slow convergence of the 2 + diamond vacancy is shown to be a result of slow varying gap levels of the defect leading to a size-dependent dielectric constant.}, archive = {J_PRL}, author = {Hanzhi Shang and Zeyu Jiang and Yiyang Sun and D. West and Shengbai Zhang}, doi = {10.1103/PhysRevLett.134.066401}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066401}, shortjournal = {Phys. Rev. Lett.}, title = {Revisiting the formulation of charged defect in solids}, volume = {134}, year = {2025}, }
• (2025). Anderson transition at complex energies in one-dimensional parity-time-symmetric disordered systems. PRL, 134(6), 066301. (www)

  @article{ , abstract = {The presence of disorder can severely impede wave transport, resulting in the famous Anderson localization. Previous theoretical studies found that Anderson transition can exist in one-dimensional (1D) non-Hermitian disordered rings with chiral hopping, defying the scaling theory of localization for Hermitian systems. In these systems, localized (extended) modes are associated with real (complex) energies. Here, we report that Anderson localized modes with complex energies can also exist in such systems. The emergence of the complex-energy localized modes (CELMs) directly ties to the properties of the corresponding pristine non-Hermitian system. Specifically, the density of states of the complex spectrum under the periodic boundary condition and the non-Bloch parity-time transition of the open-boundary chain both play critical roles in the emergence of the CELMs. The coexistence of extended modes, real-energy localized modes (RELMs), and CELMs should be a generic phenomenon for 1D non-Hermitian disordered systems under class AI. Our work shows that the interplay between Anderson mechanism and non-Hermitian physics enriches the properties of disordered media and opens new possibilities for controlling wave transport.}, archive = {J_PRL}, author = {Wei Wang and Xulong Wang and Guancong Ma}, doi = {10.1103/PhysRevLett.134.066301}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066301}, shortjournal = {Phys. Rev. Lett.}, title = {Anderson transition at complex energies in one-dimensional parity-time-symmetric disordered systems}, volume = {134}, year = {2025}, }
• (2025). Striped twisted state in the orientational epitaxy on quasicrystals. PRL, 134(6), 066202. (www)

  @article{ , abstract = {The optimal “twisted” geometry of a crystalline layer on a crystal has long been known, but that on a quasicrystal is still unknown and open. We predict analytically that the layer equilibrium configuration will generally exhibit a nonzero misfit angle. The theory perfectly agrees with numerical optimization of a colloid monolayer on a quasiperiodic decagonal optical lattice. Strikingly different from crystal-on-crystal epitaxy, the structure of the novel emerging twisted state exhibits an unexpected stripe pattern. Its high anisotropy should reflect on the tribomechanical properties of this unconventional interface.}, archive = {J_PRL}, author = {Nicola Manini and Mario Forzanini and Sebastiano Pagano and Marco Bellagente and Martino Colombo and Dario Bertazioli and Tommaso Salvalaggio and Andrea Vanossi and Davide Vanossi and Emanuele Panizon and Erio Tosatti and Giuseppe E. Santoro}, doi = {10.1103/PhysRevLett.134.066202}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066202}, shortjournal = {Phys. Rev. Lett.}, title = {Striped twisted state in the orientational epitaxy on quasicrystals}, volume = {134}, year = {2025}, }
• (2025). Theory of electro-ionic perturbations at supported electrocatalyst nanoparticles. PRL, 134(6), 066201. (www)

  @article{ , abstract = {Nanoscopic heterogeneities in composition and structure are quintessential for the properties of electrocatalyst materials. Here, we present a semiclassical model to study the electrochemical properties of supported electrocatalyst nanoparticles (NP). The model captures the correlated electronic and ionic equilibration across NP, support, and electrolyte. It reveals peculiar trends in surface charging of the supported NP, validated by comparison with first-principles calculations. Support-induced perturbations in electronic and ionic charge densities at the NP’s active surface manifest as distinct potentials of zero local electronic and ionic charges that could differ by more than 0.5 V in the studied system.}, archive = {J_PRL}, author = {Yufan Zhang and Tobias Binninger and Jun Huang and Michael H. Eikerling}, doi = {10.1103/PhysRevLett.134.066201}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066201}, shortjournal = {Phys. Rev. Lett.}, title = {Theory of electro-ionic perturbations at supported electrocatalyst nanoparticles}, volume = {134}, year = {2025}, }
• (2025). Unveiling resilient superconducting fluctuations in atomically thin NbSe2 through higgs mode spectroscopy. PRL, 134(6), 066002. (www)

  @article{ , abstract = {We report a combined electrical transport and optical study of the superconductivity in atomically thin . When subjected to an out-of-plane magnetic field, an anomalous metallic state emerges, characterized by a finite longitudinal resistance and a vanishing Hall resistance, suggesting the presence of particle-hole symmetry. We establish a superconducting Higgs mode in atomically thin samples, which reveals enduring superconducting fluctuations that withstand unexpectedly high reduced magnetic fields. These findings provide evidence of robust locally paired electrons in the anomalous metallic state, affirming its bosonic nature.}, archive = {J_PRL}, author = {Yu Du and Gan Liu and Wei Ruan and Zhi Fang and Kenji Watanabe and Takashi Taniguchi and Ronghua Liu and Jian-Xin Li and Xiaoxiang Xi}, doi = {10.1103/PhysRevLett.134.066002}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066002}, shortjournal = {Phys. Rev. Lett.}, title = {Unveiling resilient superconducting fluctuations in atomically thin NbSe2 through higgs mode spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Thermal properties of the Superconductor–Quantum hall interface. PRL, 134(6), 066001. (www)

  @article{ , abstract = {An important route of engineering topological states and excitations is to combine superconductors (SC) with the quantum Hall (QH) effect, and over the past decade, significant progress has been made in this direction. While typical measurements of these states focus on electronic properties, little attention has been paid to the accompanying thermal responses. Here, we examine the thermal properties of the interface between type-II superconducting electrodes and graphene in the QH regime. We use the thermal noise measurement to probe the local electron temperature of the superconductor next to the biased interface. Surprisingly, the measured temperature rise indicates that the superconductor provides a significant thermal conductivity, which is linear in temperature. This suggests electronic heat transport and may be unexpected, because the number of the quasiparticles in the superconductor should be exponentially suppressed. Instead, we attribute the measured electronic heat conductivity to the overlap of the normal states in the vortex cores.}, archive = {J_PRL}, author = {Lingfei Zhao and Trevyn F. Q. Larson and Zubair Iftikhar and John Chiles and Kenji Watanabe and Takashi Taniguchi and François Amet and Gleb Finkelstein}, doi = {10.1103/PhysRevLett.134.066001}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {066001}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal properties of the Superconductor–Quantum hall interface}, volume = {134}, year = {2025}, }
• (2025). Water nanofilms facilitate ice crystal growth across droplets. PRL, 134(6), 064001. (www)

  @article{ , abstract = {A novel mechanism that underlies the peculiar cascading freezing of multiple supercooled droplets on surfaces is reported. The initial ice crystal growth in large droplets is communicated via connected water nanofilms to smaller droplets. Using high-speed imaging, we show that the presence of a water nanofilm with thickness higher than a critical value around 4.5 nm facilitates a freezing front propagation from one droplet to its neighbors on a hydrophilic surface. The freezing propagation rate through water nanofilms is approximately 40% of the recalescence front growth rate within a droplet, both of which are well described by kinetic crystal growth theory.}, archive = {J_PRL}, author = {Shaojie Hu and Ningning Zhao and Chao Zhang and Fuxiang Li and Renpeng Chen and Dani Or}, doi = {10.1103/PhysRevLett.134.064001}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {064001}, shortjournal = {Phys. Rev. Lett.}, title = {Water nanofilms facilitate ice crystal growth across droplets}, volume = {134}, year = {2025}, }
• (2025). Bulk-hole correspondence and inner robust boundary modes in singular flatband lattices. PRL, 134(6), 063803. (www)

  @article{ , abstract = {Topological entities based on bulk-boundary correspondence are ubiquitous, from conventional to higher-order topological insulators, where the protected states are typically localized at the outer boundaries (edges or corners). A less explored scenario involves protected states that are localized at the inner boundaries, sharing the same energy as the bulk states. Here, we propose and demonstrate what we refer to as the “bulk-hole correspondence’’—a relation between the inner robust boundary modes (RBMs) and the existence of multiple “holes” in singular flatband lattices, mediated by the immovable discontinuity of the bulk Bloch wave functions. We find that the number of independent flatband states always equals the sum of the number of independent compact localized states and the number of nontrivial inner RBMs, as captured by the Betti number that also counts the hole number from topological data analysis. This correspondence is universal for singular flatband lattices, regardless of the lattice shape and the hole shape. Using laser-written kagome lattices as a platform, we experimentally observe such inner RBMs, demonstrating their real-space topological nature and robustness. Our results may extend to other singular flatband systems beyond photonics, including non-Euclidean lattices, providing a new approach for understanding nontrivial flatband states and topology in hole-bearing lattice systems.}, archive = {J_PRL}, author = {Limin Song and Shenyi Gao and Shiqi Xia and Yongsheng Liang and Liqin Tang and Daohong Song and Daniel Leykam and Zhigang Chen}, doi = {10.1103/PhysRevLett.134.063803}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063803}, shortjournal = {Phys. Rev. Lett.}, title = {Bulk-hole correspondence and inner robust boundary modes in singular flatband lattices}, volume = {134}, year = {2025}, }
• (2025). Fully programmable spatial photonic ising machine by focal plane division. PRL, 134(6), 063802. (www)

  @article{ , abstract = {Ising machines are an emerging class of hardware that promises ultrafast and energy-efficient solutions to -hard combinatorial optimization problems. Spatial photonic Ising machines (SPIMs) exploit optical computing in free space to accelerate the computation, showcasing parallelism, scalability, and low power consumption. However, current SPIMs can implement only a restricted class of problems. This partial programmability is a critical limitation that hampers their benchmark. Achieving full programmability of the device while preserving its scalability is an open challenge. Here, we report a fully programmable SPIM achieved through a novel operation method based on the division of the focal plane. In our scheme, a general Ising problem is decomposed into a set of Mattis Hamiltonians, whose energies are simultaneously computed optically by measuring the intensity on different regions of the camera sensor. Exploiting this concept, we experimentally demonstrate the computation with high success probability of ground-state solutions of up to 32-spin Ising models on unweighted maximum cut graphs with and without ferromagnetic bias. Simulations of the hardware prove a favorable scaling of the accuracy with the number of spin. Our fully programmable SPIM enables the implementation of many quadratic unconstrained binary optimization problems, further establishing SPIMs as a leading paradigm in non–von Neumann hardware.}, archive = {J_PRL}, author = {Daniele Veraldi and Davide Pierangeli and Silvia Gentilini and Marcello Calvanese Strinati and Jason Sakellariou and James S. Cummins and Airat Kamaletdinov and Marvin Syed and Richard Zhipeng Wang and Natalia G. Berloff and Dimitrios Karanikolopoulos and Pavlos G. Savvidis and Claudio Conti}, doi = {10.1103/PhysRevLett.134.063802}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063802}, shortjournal = {Phys. Rev. Lett.}, title = {Fully programmable spatial photonic ising machine by focal plane division}, volume = {134}, year = {2025}, }
• (2025). Nonuniform wave momentum band gap in biaxial anisotropic photonic time crystals. PRL, 134(6), 063801. (www)

  @article{ , abstract = {Photonic time crystals (PTCs) host momentum band gaps, enabling intriguing nonresonant light amplification in propagating waves, but opening substantial band gaps demands refractive index changes too extreme for conventional nonlinear optics. Here, we introduce momentum band gaps for nonuniform waves, including evanescent and ghost types, by extending PTCs to biaxial anisotropic photonic time crystals that periodically alternate between uniform biaxial anisotropy and isotropic media over time. We show that ghost waves, unlike evanescent waves, sustain only momentum band gaps, opening wide band gaps at even the smallest modulation depths. Moreover, we demonstrate momentum band-gap effects on nonuniform waves that can be amplified or, through decaying modes, selectively attenuated. We find that ghost wave momentum band gaps uniquely boost refracted over reflected waves under one-way incidence, in stark contrast to the balanced amplification seen in both propagating and evanescent waves. Our approach expands time-varying metamaterials by integrating wave characteristics, bridging the gap between conventional nonlinear optics and PTC momentum band gaps, and shedding new light on extreme manipulation of surface polaritons.}, archive = {J_PRL}, author = {Junhua Dong and Sihao Zhang and Huan He and Huanan Li and Jingjun Xu}, doi = {10.1103/PhysRevLett.134.063801}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063801}, shortjournal = {Phys. Rev. Lett.}, title = {Nonuniform wave momentum band gap in biaxial anisotropic photonic time crystals}, volume = {134}, year = {2025}, }
• (2025). Floquet engineering the quantum rabi model in the ultrastrong coupling regime. PRL, 134(6), 063602. (www)

  @article{ , abstract = {We study the quantum Rabi model for a two-level system coupled to a quantized cavity mode under periodic modulation of the cavity-dipole coupling in the ultrastrong coupling regime, leading to rich Floquet states. Exploiting the quantum vacuum, we show how purely mechanical driving can produce real photons, depending on the strength and frequency of the periodic coupling rate. This scheme is promising for the coherent manipulation of hybrid quantum systems and quantum vacuum effects, with potential applications for quantum state engineering, quantum information processing, and the study of nonequilibrium quantum phenomena.}, archive = {J_PRL}, author = {Kamran Akbari and Franco Nori and Stephen Hughes}, doi = {10.1103/PhysRevLett.134.063602}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063602}, shortjournal = {Phys. Rev. Lett.}, title = {Floquet engineering the quantum rabi model in the ultrastrong coupling regime}, volume = {134}, year = {2025}, }
• (2025). Observation of collapse and revival in a superconducting atomic frequency comb. PRL, 134(6), 063601. (www)

  @article{ , abstract = {Recent advancements in superconducting circuits have enabled the experimental study of collective behavior of precisely controlled intermediate-scale ensembles of qubits. In this work, we demonstrate an atomic frequency comb formed by individual artificial atoms strongly coupled to a single resonator mode. We observe periodic microwave pulses that originate from a single coherent excitation dynamically interacting with the multiqubit ensemble. We show that this revival dynamics emerges as a consequence of the constructive and periodic rephasing of the five superconducting qubits forming the vacuum Rabi split comb. In the future, similar devices could be used as a memory with in situ tunable storage time or as an on-chip periodic pulse generator with nonclassical photon statistics.}, archive = {J_PRL}, author = {E. S. Redchenko and M. Zens and M. Žemlička and M. Peruzzo and F. Hassani and R. Sett and P. Zieliński and H. S. Dhar and D. O. Krimer and S. Rotter and J. M. Fink}, doi = {10.1103/PhysRevLett.134.063601}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of collapse and revival in a superconducting atomic frequency comb}, volume = {134}, year = {2025}, }
• (2025). Neutral sulfur atom formation in decay of deep core holes in SF6. PRL, 134(6), 063003. (www)

  @article{ , abstract = {Dissociation upon sulfur -shell excitation or ionization of is studied by sulfur -shell emission spectroscopy using synchrotron radiation and multiconfiguration Dirac-Hartree-Fock calculations of emission energies and transition rates. The decay path involves in particular Auger emission with the ejection of one or more electrons, leading to singly or multiply charged intermediate states. Nevertheless, the results of the study show that the observed photon emission at 151–152 eV following excitation at 2485–2489 eV originates dominantly from transitions in neutral sulfur. This clearly indicates that the central atom retains its electrons in a dissociation process where all fluorine atoms detach before the S decay.}, archive = {J_PRL}, author = {Oksana Travnikova and Florian Trinter and Marcus Agåker and Giorgio Visentin and Joakim Andersson and Ludvig Kjellsson and Iyas Ismail and Nicolas Velasquez and Dimitris Koulentianos and Manuel Harder and Zhong Yin and Johan Söderström and Tatiana Marchenko and Renaud Guillemin and O. Dennis McGinnis and Hans Ågren and Stephan Fritzsche and Marc Simon and Jan-Erik Rubensson and Joseph Nordgren}, doi = {10.1103/PhysRevLett.134.063003}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063003}, shortjournal = {Phys. Rev. Lett.}, title = {Neutral sulfur atom formation in decay of deep core holes in SF6}, volume = {134}, year = {2025}, }
• (2025). Probing new bosons and nuclear structure with ytterbium isotope shifts. PRL, 134(6), 063002. (www)

  @article{ , abstract = {In this Letter, we present mass-ratio measurements on highly charged Yb 42 + ions with a precision of 4 × 10 − 12 and isotope-shift measurements on Yb + on the S 2 1 / 2 → D 5 / 2 2 and S 2 1 / 2 → F 7 / 2 2 transitions with a precision of 4 × 10 − 9 for the isotopes Yb 168 , 170 , 172 , 174 , 176 . We present a new method that allows us to extract higher-order changes in the nuclear charge distribution along the Yb isotope chain, benchmarking ab initio nuclear structure calculations. Additionally, we perform a King plot analysis to set bounds on a fifth force in the keV / c 2 to MeV / c 2 range coupling to electrons and neutrons.}, archive = {J_PRL}, author = {Menno Door and Chih-Han Yeh and Matthias Heinz and Fiona Kirk and Chunhai Lyu and Takayuki Miyagi and Julian C. Berengut and Jacek Bieroń and Klaus Blaum and Laura S. Dreissen and Sergey Eliseev and Pavel Filianin and Melina Filzinger and Elina Fuchs and Henning A. Fürst and Gediminas Gaigalas and Zoltán Harman and Jost Herkenhoff and Nils Huntemann and Christoph H. Keitel and Kathrin Kromer and Daniel Lange and Alexander Rischka and Christoph Schweiger and Achim Schwenk and Noritaka Shimizu and Tanja E. Mehlstäubler}, doi = {10.1103/PhysRevLett.134.063002}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063002}, shortjournal = {Phys. Rev. Lett.}, title = {Probing new bosons and nuclear structure with ytterbium isotope shifts}, volume = {134}, year = {2025}, }
• (2025). Convergent close-coupling approach to electron impact dissociation of the polyatomic molecule h3+ and its isotopologues. PRL, 134(6), 063001. (www)

  @article{ , abstract = {Cross sections for electron impact dissociative excitation and ionization in scattering on vibrationally excited levels of the ground electronic state of H 3 + and its isotopologues are reported in the energy range of 8 to 1000 eV. Calculations have been performed using a newly developed version of the molecular convergent close-coupling code. Cross sections for total dissociative excitation, ionization yielding atomic fragments such as D + , and the total inelastic cross section are presented. Good agreement with available experiments has been demonstrated.}, archive = {J_PRL}, author = {Reese K. Horton and Michael V. Pak and Igor Bray and Dmitry V. Fursa}, doi = {10.1103/PhysRevLett.134.063001}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {063001}, shortjournal = {Phys. Rev. Lett.}, title = {Convergent close-coupling approach to electron impact dissociation of the polyatomic molecule h3+ and its isotopologues}, volume = {134}, year = {2025}, }
• (2025). Direct mass measurements of neutron-rich zinc and gallium isotopes: An investigation of the formation of the first r-process peak. PRL, 134(6), 062701. (www)

  @article{ , abstract = {The prediction of isotopic abundances resulting from the rapid neutron capture process ( r process) requires high-precision mass measurements. Using TITAN’s on-line time-of-flight spectrometer, first time mass measurements are performed for Zn 83 and Ga 86 . These measurements reduced uncertainties, and are used to calculate isotopic abundances near the first r -process abundance peak using astrophysical conditions present during a binary neutron star (BNS) merger. Good agreement in abundance across a range of trajectories is found when comparing to several metal-poor stars while also strongly deviating from the solar r -process pattern. These findings point to a high degree of sensitivity to the electron fraction of a BNS merger on the final elemental abundance pattern for certain elements near the first r -process peak while others display universality. We find that small changes in electron fraction can produce distinct abundance patterns that match those of metal-poor stars with different classifications.}, archive = {J_PRL}, author = {Andrew Jacobs and Stylianos Nikas and John Ash and Behnam Ashrafkhani and Ivana Belosovic and Julian Bergmann and Callum Brown and Jaime Cardona and Eleanor Dunling and Timo Dickel and Luca Egoriti and Gabriella Gelinas and Zach Hockenbery and Sakshi Kakkar and Brian Kootte and Ali Mollaebrahimi and Eleni Marina Lykiardopoulou and Tobias Murböck and Stefan Paul and Wolfgang R. Plaß and William S. Porter and Moritz Pascal Reiter and Alex Ridley and Jon Ringuette and Christoph Scheidenberger and Rane Simpson and Coulter Walls and Yilin Wang and Jens Dilling and Ania Kwiatkowski}, doi = {10.1103/PhysRevLett.134.062701}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {062701}, shortjournal = {Phys. Rev. Lett.}, title = {Direct mass measurements of neutron-rich zinc and gallium isotopes: An investigation of the formation of the first r-process peak}, volume = {134}, year = {2025}, }
• (2025). Deformation and collectivity in doubly magic pb208. PRL, 134(6), 062502. (www)

  @article{ , abstract = {Lead-208 is the heaviest known doubly magic nucleus and its structure is therefore of special interest. Despite this magicity, which acts to provide a strong restorative force toward sphericity, it is known to exhibit both strong octupole correlations and some of the strongest quadrupole collectivity observed in doubly magic systems. In this Letter, we employ state-of-the-art experimental equipment to conclusively demonstrate, through four Coulomb-excitation measurements, the presence of a large, negative, spectroscopic quadrupole moment for both the vibrational octupole and quadrupole state, indicative of a preference for prolate deformation of the states. The observed quadrupole moment is discussed in the context of the expected splitting of the two-phonon states, due to the coupling of the quadrupole and octupole motion. These results are compared with theoretical values from three different methods, which are unable to reproduce both the sign and magnitude of this deformation. Thus, in spite of its well-studied nature, remains a puzzle for our understanding of nuclear structure.}, archive = {J_PRL}, author = {J. Henderson and J. Heery and M. Rocchini and M. Siciliano and N. Sensharma and A. D. Ayangeakaa and R. V. F. Janssens and T. M. Kowalewski and Abhishek and P. D. Stevenson and E. Yüksel and B. A. Brown and T. R. Rodriguez and L. M. Robledo and C. Y. Wu and S. Kisyov and C. Müller-Gatermann and V. Bildstein and L. Canete and C. M. Campbell and S. Carmichael and M. P. Carpenter and W. N. Catford and P. Copp and C. Cousins and M. Devlin and D. T. Doherty and P. E. Garrett and U. Garg and L. P. Gaffney and K. Hadynska-Klek and D. J. Hartley and S. F. Hicks and H. Jayatissa and S. R. Johnson and D. Kalaydjieva and F. Kondev and D. Lascar and T. Lauritsen and G. Lotay and N. Marchini and M. Matejska-Minda and S. Nandi and A. Nannini and C. O’Shea and S. Pascu and C. J. Paxman and A. Perkoff and E. E. Peters and Zs. Podolyák and A. Radich and R. Rathod and B. J. Reed and P. H. Regan and W. Reviol and E. Rubino and R. Russell and D. Seweryniak and J. R. Vanhoy and G. L. Wilson and K. Wrzosek-Lipska and S. W. Yates and I. Zanon}, doi = {10.1103/PhysRevLett.134.062502}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {062502}, shortjournal = {Phys. Rev. Lett.}, title = {Deformation and collectivity in doubly magic pb208}, volume = {134}, year = {2025}, }
• (2025). Fragmentation of the giant pairing vibration in c14 induced by many-body processes. PRL, 134(6), 062501. (www)

  @article{ , abstract = {We present a theoretical framework for treating the full excitation spectrum of J π = 0 + pair addition modes, including the well-known low-lying and bound pairing vibrations on par with the predicted high-lying pairing vibrations, often called giant pairing vibrations. Our formalism includes the coupling to low-energy collective quadrupolar modes of the core, in such a way that both single-particle self-energy effects and the pairing interaction induced by phonon exchange are accounted for. The coupling with the continuum plays an important role and is also taken into account. The theory is applied to the case of the excitation spectrum of C 14 , recently populated by two-neutron transfer reactions.}, archive = {J_PRL}, author = {F. Barranco and G. Potel and E. Vigezzi}, doi = {10.1103/PhysRevLett.134.062501}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {062501}, shortjournal = {Phys. Rev. Lett.}, title = {Fragmentation of the giant pairing vibration in c14 induced by many-body processes}, volume = {134}, year = {2025}, }
• (2025). Jet definition and transverse-Momentum–Dependent factorization in semi-inclusive deep-inelastic scattering. PRL, 134(6), 061903. (www)

  @article{ , abstract = {Using the color dipole picture of deep inelastic scattering (DIS) and the color glass condensate effective theory, we study semi-inclusive jet production in DIS at small x in the limit where the photon virtuality Q 2 is much larger than the transverse momentum squared P ⊥ 2 of the produced jet. In this limit, the cross section is dominated by aligned jet configurations, that is, quark–antiquark pairs in which one of the fermions—the would-be struck quark in the Breit frame—carries most of the longitudinal momentum of the virtual photon. We show that physically meaningful jet definitions in DIS are such that the effective axis of the jet sourced by the struck quark is controlled by its virtuality rather than by its transverse momentum. For such jet definitions, we show that the next-to-leading order cross section admits factorization in terms of the (sea) quark transverse momentum dependent distribution, which in turn satisfies a universal Dokshitzer-Gribov-Lipatov-Altarelli-Parisi and Sudakov evolution.}, archive = {J_PRL}, author = {Paul Caucal and Edmond Iancu and A. H. Mueller and Feng Yuan}, doi = {10.1103/PhysRevLett.134.061903}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061903}, shortjournal = {Phys. Rev. Lett.}, title = {Jet definition and transverse-Momentum–Dependent factorization in semi-inclusive deep-inelastic scattering}, volume = {134}, year = {2025}, }
• (2025). Complete dispersive evaluation of the hadronic light-by-light contribution to muon g−2. PRL, 134(6), 061902. (www)

  @article{ , abstract = {Hadronic light-by-light (HLbL) scattering defines one of the critical contributions in the Standard Model prediction of the anomalous magnetic moment of the muon. In this Letter, we present a complete evaluation using a dispersive formalism, in which the HLbL tensor is reconstructed from its discontinuities, expressed in terms of simpler hadronic matrix elements that can be extracted from experiment. Profiting from recent developments in the determination of axial-vector transition form factors, short-distance constraints for the HLbL tensor, and the vector–vector–axial-vector correlator, we obtain a μ HLbL = 101.9 ( 7.9 ) × 10 − 11 , which meets the precision requirements set by the final result of the Fermilab experiment.}, archive = {J_PRL}, author = {Martin Hoferichter and Peter Stoffer and Maximilian Zillinger}, doi = {10.1103/PhysRevLett.134.061902}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061902}, shortjournal = {Phys. Rev. Lett.}, title = {Complete dispersive evaluation of the hadronic light-by-light contribution to muon g−2}, volume = {134}, year = {2025}, }
• (2025). Factorization restoration through glauber gluons. PRL, 134(6), 061901. (www)

  @article{ , abstract = {We analyze the low-energy dynamics of gap-between-jets cross sections at hadron colliders, for which phase factors in the hard amplitudes spoil collinear cancellations and lead to double (“super-leading”) logarithmic behavior. Based on a method-of-regions analysis, we identify three-loop contributions from perturbative active-active Glauber-gluon exchanges with the right structure to render the cross section consistent with PDF factorization below the gap veto scale. The Glauber contributions we identify are unambiguously defined without regulators beyond dimensional regularization.}, archive = {J_PRL}, author = {Thomas Becher and Patrick Hager and Sebastian Jaskiewicz and Matthias Neubert and Dominik Schwienbacher}, doi = {10.1103/PhysRevLett.134.061901}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061901}, shortjournal = {Phys. Rev. Lett.}, title = {Factorization restoration through glauber gluons}, volume = {134}, year = {2025}, }
• (2025). Search for magnetic monopole pair production in ultraperipheral Pb+Pb collisions at sNN=5.36 TeV with the ATLAS detector at the LHC. PRL, 134(6), 061803. (www)

  @article{ , abstract = {This Letter presents a search for highly ionizing magnetic monopoles in 262 μ b − 1 of ultraperipheral Pb + Pb collision data at s NN = 5.36 TeV collected by the ATLAS detector at the LHC. A new methodology that exploits the properties of clusters of hits reconstructed in the innermost silicon detector layers is introduced to study highly ionizing particles in heavy-ion data. No significant excess above the background, which is estimated using a data-driven technique, is observed. Using a nonperturbative semiclassical model, upper limits at 95% confidence level are set on the cross section for pair production of monopoles with a single Dirac magnetic charge in the mass range of 20–150 GeV. Depending on the model, monopoles with a single Dirac magnetic charge and mass below 80–120 GeV are excluded.}, archive = {J_PRL}, author = {ATLAS Collaboration and G. Aad and E. Aakvaag and B. Abbott and S. Abdelhameed and K. Abeling and N. J. Abicht and S. H. Abidi and M. Aboelela and A. Aboulhorma and H. Abramowicz and H. Abreu and Y. Abulaiti and B. S. Acharya and A. Ackermann and C. Adam Bourdarios and L. Adamczyk and S. V. Addepalli and M. J. Addison and J. Adelman and A. Adiguzel and T. Adye and A. A. Affolder and Y. Afik and M. N. Agaras and A. Aggarwal and C. Agheorghiesei and F. Ahmadov and S. Ahuja and X. Ai and G. Aielli and A. Aikot and M. Ait Tamlihat and B. Aitbenchikh and M. Akbiyik and T. P. A. Åkesson and A. V. Akimov and D. Akiyama and N. N. Akolkar and S. Aktas and K. Al Khoury and G. L. Alberghi and J. Albert and P. Albicocco and G. L. Albouy and S. Alderweireldt and Z. L. Alegria and M. Aleksa and I. N. Aleksandrov and C. Alexa and T. Alexopoulos and F. Alfonsi and M. Algren and M. Alhroob and B. Ali and H. M. J. Ali and S. Ali and S. W. Alibocus and M. Aliev and G. Alimonti and W. Alkakhi and C. Allaire and B. M. M. Allbrooke and J. S. Allen and J. F. Allen and C. A. Allendes Flores and P. P. Allport and A. Aloisio and F. Alonso and C. Alpigiani and Z. M. K. Alsolami and M. Alvarez Estevez and A. Alvarez Fernandez and M. Alves Cardoso and M. G. Alviggi and M. Aly and Y. Amaral Coutinho and A. Ambler and C. Amelung and M. Amerl and C. G. Ames and D. Amidei and B. Amini and K. J. Amirie and S. P. Amor Dos Santos and K. R. Amos and D. Amperiadou and S. An and V. Ananiev and C. Anastopoulos and T. Andeen and J. K. Anders and A. C. Anderson and S. Y. Andrean and A. Andreazza and S. Angelidakis and A. Angerami and A. V. Anisenkov and A. Annovi and C. Antel and E. Antipov and M. Antonelli and F. Anulli and M. Aoki and T. Aoki and M. A. Aparo and L. Aperio Bella and C. Appelt and A. Apyan and S. J. Arbiol Val and C. Arcangeletti and A. T. H. Arce and J-F. Arguin and S. Argyropoulos and J.-H. Arling and O. Arnaez and H. Arnold and G. Artoni and H. Asada and K. Asai and S. Asai and N. A. Asbah and R. A. Ashby Pickering and K. Assamagan and R. Astalos and K. S. V. Astrand and S. Atashi and R. J. Atkin and M. Atkinson and H. Atmani and P. A. Atmasiddha and K. Augsten and A. D. Auriol and V. A. Austrup and G. Avolio and K. Axiotis and G. Azuelos and D. Babal and H. Bachacou and K. Bachas and A. Bachiu and E. Bachmann and A. Badea and T. M. Baer and P. Bagnaia and M. Bahmani and D. Bahner and K. Bai and J. T. Baines and L. Baines and O. K. Baker and E. Bakos and D. Bakshi Gupta and L. E. Balabram Filho and V. Balakrishnan and R. Balasubramanian and E. M. Baldin and P. Balek and E. Ballabene and F. Balli and L. M. Baltes and W. K. Balunas and J. Balz and I. Bamwidhi and E. Banas and M. Bandieramonte and A. Bandyopadhyay and S. Bansal and L. Barak and M. Barakat and E. L. Barberio and D. Barberis and M. Barbero and M. Z. Barel and T. Barillari and M-S. Barisits and T. Barklow and P. Baron and D. A. Baron Moreno and A. Baroncelli and A. J. Barr and J. D. Barr and F. Barreiro and J. Barreiro Guimarães da Costa and M. G. Barros Teixeira and S. Barsov and F. Bartels and R. Bartoldus and A. E. Barton and P. Bartos and A. Basan and M. Baselga and A. Bassalat and M. J. Basso and S. Bataju and R. Bate and R. L. Bates and S. Batlamous and B. Batool and M. Battaglia and D. Battulga and M. Bauce and M. Bauer and P. Bauer and L. T. Bazzano Hurrell and J. B. Beacham and T. Beau and J. Y. Beaucamp and P. H. Beauchemin and P. Bechtle and H. P. Beck and K. Becker and A. J. Beddall and V. A. Bednyakov and C. P. Bee and L. J. Beemster and T. A. Beermann and M. Begalli and M. Begel and A. Behera and J. K. Behr and J. F. Beirer and F. Beisiegel and M. Belfkir and G. Bella and L. Bellagamba and A. Bellerive and P. Bellos and K. Beloborodov and D. Benchekroun and F. Bendebba and Y. Benhammou and K. C. Benkendorfer and L. Beresford and M. Beretta and E. Bergeaas Kuutmann and N. Berger and B. Bergmann and J. Beringer and G. Bernardi and C. Bernius and F. U. Bernlochner and F. Bernon and A. Berrocal Guardia and T. Berry and P. Berta and A. Berthold and S. Bethke and A. Betti and A. J. Bevan and N. K. Bhalla and S. Bhatta and D. S. Bhattacharya and P. Bhattarai and Z. M. Bhatti and K. D. Bhide and V. S. Bhopatkar and R. M. Bianchi and G. Bianco and O. Biebel and R. Bielski and M. Biglietti and C. S. Billingsley and Y. Bimgdi and M. Bindi and A. Bingham and A. Bingul and C. Bini and G. A. Bird and M. Birman and M. Biros and S. Biryukov and T. Bisanz and E. Bisceglie and J. P. Biswal and D. Biswas and I. Bloch and A. Blue and U. Blumenschein and J. Blumenthal and V. S. Bobrovnikov and M. Boehler and B. Boehm and D. Bogavac and A. G. Bogdanchikov and L. S. Boggia and C. Bohm and V. Boisvert and P. Bokan and T. Bold and M. Bomben and M. Bona and M. Boonekamp and A. G. Borbély and I. S. Bordulev and G. Borissov and D. Bortoletto and D. Boscherini and M. Bosman and K. Bouaouda and N. Bouchhar and L. Boudet and J. Boudreau and E. V. Bouhova-Thacker and D. Boumediene and R. Bouquet and A. Boveia and J. Boyd and D. Boye and I. R. Boyko and L. Bozianu and J. Bracinik and N. Brahimi and G. Brandt and O. Brandt and F. Braren and B. Brau and J. E. Brau and R. Brener and L. Brenner and R. Brenner and S. Bressler and G. Brianti and D. Britton and D. Britzger and I. Brock and R. Brock and G. Brooijmans and A. J. Brooks and E. M. Brooks and E. Brost and L. M. Brown and L. E. Bruce and T. L. Bruckler and P. A. Bruckman de Renstrom and B. Brüers and A. Bruni and G. Bruni and D. Brunner and M. Bruschi and N. Bruscino and T. Buanes and Q. Buat and D. Buchin and A. G. Buckley and O. Bulekov and B. A. Bullard and S. Burdin and C. D. Burgard and A. M. Burger and B. Burghgrave and O. Burlayenko and J. Burleson and J. T. P. Burr and J. C. Burzynski and E. L. Busch and V. Büscher and P. J. Bussey and J. M. Butler and C. M. Buttar and J. M. Butterworth and W. Buttinger and C. J. Buxo Vazquez and A. R. Buzykaev and S. Cabrera Urbán and L. Cadamuro and D. Caforio and H. Cai and Y. Cai and V. M. M. Cairo and O. Cakir and N. Calace and P. Calafiura and G. Calderini and P. Calfayan and G. Callea and L. P. Caloba and D. Calvet and S. Calvet and M. Calvetti and R. Camacho Toro and S. Camarda and D. Camarero Munoz and P. Camarri and M. T. Camerlingo and D. Cameron and C. Camincher and M. Campanelli and A. Camplani and V. Canale and A. C. Canbay and E. Canonero and J. Cantero and Y. Cao and F. Capocasa and M. Capua and A. Carbone and R. Cardarelli and J. C. J. Cardenas and G. Carducci and T. Carli and G. Carlino and J. I. Carlotto and B. T. Carlson and E. M. Carlson and J. Carmignani and L. Carminati and A. Carnelli and M. Carnesale and S. Caron and E. Carquin and I. B. Carr and S. Carrá and G. Carratta and A. M. Carroll and M. P. Casado and M. Caspar and F. L. Castillo and L. Castillo Garcia and V. Castillo Gimenez and N. F. Castro and A. Catinaccio and J. R. Catmore and T. Cavaliere and V. Cavaliere and L. J. Caviedes Betancourt and Y. C. Cekmecelioglu and E. Celebi and S. Cella and V. Cepaitis and K. Cerny and A. S. Cerqueira and A. Cerri and L. Cerrito and F. Cerutti and B. Cervato and A. Cervelli and G. Cesarini and S. A. Cetin and D. Chakraborty and J. Chan and W. Y. Chan and J. D. Chapman and E. Chapon and B. Chargeishvili and D. G. Charlton and M. Chatterjee and C. Chauhan and Y. Che and S. Chekanov and S. V. Chekulaev and G. A. Chelkov and A. Chen and B. Chen and H. Chen and J. Chen and M. Chen and S. Chen and S. J. Chen and X. Chen and Y. Chen and C. L. Cheng and H. C. Cheng and S. Cheong and A. Cheplakov and E. Cheremushkina and E. Cherepanova and R. Cherkaoui El Moursli and E. Cheu and K. Cheung and L. Chevalier and V. Chiarella and G. Chiarelli and N. Chiedde and G. Chiodini and A. S. Chisholm and A. Chitan and M. Chitishvili and M. V. Chizhov and K. Choi and Y. Chou and E. Y. S. Chow and K. L. Chu and M. C. Chu and X. Chu and Z. Chubinidze and J. Chudoba and J. J. Chwastowski and D. Cieri and K. M. Ciesla and V. Cindro and A. Ciocio and F. Cirotto and Z. H. Citron and M. Citterio and D. A. Ciubotaru and A. Clark and P. J. Clark and N. Clarke Hall and C. Clarry and J. M. Clavijo Columbie and S. E. Clawson and C. Clement and Y. Coadou and M. Cobal and A. Coccaro and R. F. Coelho Barrue and R. Coelho Lopes De Sa and S. Coelli and L. S. Colangeli and B. Cole and J. Collot and P. Conde Muiño and M. P. Connell and S. H. Connell and E. I. Conroy and F. Conventi and H. G. Cooke and A. M. Cooper-Sarkar and F. A. Corchia and A. Cordeiro Oudot Choi and L. D. Corpe and M. Corradi and F. Corriveau and A. Cortes-Gonzalez and M. J. Costa and F. Costanza and D. Costanzo and B. M. Cote and J. Couthures and G. Cowan and K. Cranmer and L. Cremer and D. Cremonini and S. Crépé-Renaudin and F. Crescioli and M. Cristinziani and M. Cristoforetti and V. Croft and J. E. Crosby and G. Crosetti and A. Cueto and H. Cui and Z. Cui and W. R. Cunningham and F. Curcio and J. R. Curran and P. Czodrowski and M. J. Da Cunha Sargedas De Sousa and J. V. Da Fonseca Pinto and C. Da Via and W. Dabrowski and T. Dado and S. Dahbi and T. Dai and D. Dal Santo and C. Dallapiccola and M. Dam and G. D’amen and V. D’Amico and J. Damp and J. R. Dandoy and D. Dannheim and M. Danninger and V. Dao and G. Darbo and S. J. Das and F. Dattola and S. D’Auria and A. D’Avanzo and C. David and T. Davidek and I. Dawson and H. A. Day-hall and K. De and R. De Asmundis and N. De Biase and S. De Castro and N. De Groot and P. de Jong and H. De la Torre and A. De Maria and A. De Salvo and U. De Sanctis and F. De Santis and A. De Santo and J. B. De Vivie De Regie and J. Debevc and D. V. Dedovich and J. Degens and A. M. Deiana and F. Del Corso and J. Del Peso and L. Delagrange and F. Deliot and C. M. Delitzsch and M. Della Pietra and D. Della Volpe and A. Dell’Acqua and L. Dell’Asta and M. Delmastro and C. C. Delogu and P. A. Delsart and S. Demers and M. Demichev and S. P. Denisov and L. D’Eramo and D. Derendarz and F. Derue and P. Dervan and K. Desch and C. Deutsch and F. A. Di Bello and A. Di Ciaccio and L. Di Ciaccio and A. Di Domenico and C. Di Donato and A. Di Girolamo and G. Di Gregorio and A. Di Luca and B. Di Micco and R. Di Nardo and K. F. Di Petrillo and M. Diamantopoulou and F. A. Dias and T. Dias Do Vale and M. A. Diaz and A. R. Didenko and M. Didenko and E. B. Diehl and S. Díez Cornell and C. Diez Pardos and C. Dimitriadi and A. Dimitrievska and J. Dingfelder and T. Dingley and I-M. Dinu and S. J. Dittmeier and F. Dittus and M. Divisek and B. Dixit and F. Djama and T. Djobava and C. Doglioni and A. Dohnalova and J. Dolejsi and Z. Dolezal and K. Domijan and K. M. Dona and M. Donadelli and B. Dong and J. Donini and A. D’Onofrio and M. D’Onofrio and J. Dopke and A. Doria and N. Dos Santos Fernandes and P. Dougan and M. T. Dova and A. T. Doyle and M. A. Draguet and M. P. Drescher and E. Dreyer and I. Drivas-koulouris and M. Drnevich and M. Drozdova and D. Du and T. A. du Pree and F. Dubinin and M. Dubovsky and E. Duchovni and G. Duckeck and O. A. Ducu and D. Duda and A. Dudarev and E. R. Duden and M. D’uffizi and L. Duflot and M. Dührssen and I. Duminica and A. E. Dumitriu and M. Dunford and S. Dungs and K. Dunne and A. Duperrin and H. Duran Yildiz and M. Düren and A. Durglishvili and D. Duvnjak and B. L. Dwyer and G. I. Dyckes and M. Dyndal and B. S. Dziedzic and Z. O. Earnshaw and G. H. Eberwein and B. Eckerova and S. Eggebrecht and E. Egidio Purcino De Souza and L. F. Ehrke and G. Eigen and K. Einsweiler and T. Ekelof and P. A. Ekman and S. El Farkh and Y. El Ghazali and H. El Jarrari and A. El Moussaouy and V. Ellajosyula and M. Ellert and F. Ellinghaus and N. Ellis and J. Elmsheuser and M. Elsawy and M. Elsing and D. Emeliyanov and Y. Enari and I. Ene and S. Epari and P. A. Erland and D. Ernani Martins Neto and M. Errenst and M. Escalier and C. Escobar and E. Etzion and G. Evans and H. Evans and L. S. Evans and A. Ezhilov and S. Ezzarqtouni and F. Fabbri and L. Fabbri and G. Facini and V. Fadeyev and R. M. Fakhrutdinov and D. Fakoudis and S. Falciano and L. F. Falda Ulhoa Coelho and F. Fallavollita and G. Falsetti and J. Faltova and C. Fan and K. Y. Fan and Y. Fan and Y. Fang and M. Fanti and M. Faraj and Z. Farazpay and A. Farbin and A. Farilla and T. Farooque and S. M. Farrington and F. Fassi and D. Fassouliotis and M. Faucci Giannelli and W. J. Fawcett and L. Fayard and P. Federic and P. Federicova and O. L. Fedin and M. Feickert and L. Feligioni and D. E. Fellers and C. Feng and Z. Feng and M. J. Fenton and L. Ferencz and R. A. M. Ferguson and S. I. Fernandez Luengo and P. Fernandez Martinez and M. J. V. Fernoux and J. Ferrando and A. Ferrari and P. Ferrari and R. Ferrari and D. Ferrere and C. Ferretti and D. Fiacco and F. Fiedler and P. Fiedler and S. Filimonov and A. Filipčič and E. K. Filmer and F. Filthaut and M. C. N. Fiolhais and L. Fiorini and W. C. Fisher and T. Fitschen and P. M. Fitzhugh and I. Fleck and P. Fleischmann and T. Flick and M. Flores and L. R. Flores Castillo and L. Flores Sanz De Acedo and F. M. Follega and N. Fomin and J. H. Foo and A. Formica and A. C. Forti and E. Fortin and A. W. Fortman and M. G. Foti and L. Fountas and D. Fournier and H. Fox and P. Francavilla and S. Francescato and S. Franchellucci and M. Franchini and S. Franchino and D. Francis and L. Franco and V. Franco Lima and L. Franconi and M. Franklin and G. Frattari and Y. Y. Frid and J. Friend and N. Fritzsche and A. Froch and D. Froidevaux and J. A. Frost and Y. Fu and S. Fuenzalida Garrido and M. Fujimoto and K. Y. Fung and E. Furtado De Simas Filho and M. Furukawa and J. Fuster and A. Gaa and A. Gabrielli and P. Gadow and G. Gagliardi and L. G. Gagnon and S. Gaid and S. Galantzan and J. Gallagher and E. J. Gallas and B. J. Gallop and K. K. Gan and S. Ganguly and Y. Gao and F. M. Garay Walls and B. Garcia and C. García and A. Garcia Alonso and A. G. Garcia Caffaro and J. E. García Navarro and M. Garcia-Sciveres and G. L. Gardner and R. W. Gardner and N. Garelli and D. Garg and R. B. Garg and J. M. Gargan and C. A. Garner and C. M. Garvey and V. K. Gassmann and G. Gaudio and V. Gautam and P. Gauzzi and J. Gavranovic and I. L. Gavrilenko and A. Gavrilyuk and C. Gay and G. Gaycken and E. N. Gazis and A. A. Geanta and C. M. Gee and A. Gekow and C. Gemme and M. H. Genest and A. D. Gentry and S. George and W. F. George and T. Geralis and P. Gessinger-Befurt and M. E. Geyik and M. Ghani and K. Ghorbanian and A. Ghosal and A. Ghosh and B. Giacobbe and S. Giagu and T. Giani and A. Giannini and S. M. Gibson and M. Gignac and D. T. Gil and A. K. Gilbert and B. J. Gilbert and D. Gillberg and G. Gilles and L. Ginabat and D. M. Gingrich and M. P. Giordani and P. F. Giraud and G. Giugliarelli and D. Giugni and F. Giuli and I. Gkialas and L. K. Gladilin and C. Glasman and G. R. Gledhill and G. Glemža and M. Glisic and I. Gnesi and Y. Go and M. Goblirsch-Kolb and B. Gocke and D. Godin and B. Gokturk and S. Goldfarb and T. Golling and M. G. D. Gololo and D. Golubkov and J. P. Gombas and A. Gomes and G. Gomes Da Silva and A. J. Gomez Delegido and R. Gonçalo and L. Gonella and A. Gongadze and F. Gonnella and J. L. Gonski and R. Y. González Andana and S. González de la Hoz and R. Gonzalez Lopez and C. Gonzalez Renteria and M. V. Gonzalez Rodrigues and R. Gonzalez Suarez and S. Gonzalez-Sevilla and L. Goossens and B. Gorini and E. Gorini and A. Gorišek and T. C. Gosart and A. T. Goshaw and M. I. Gostkin and S. Goswami and C. A. Gottardo and S. A. Gotz and M. Gouighri and V. Goumarre and A. G. Goussiou and N. Govender and R. P. Grabarczyk and I. Grabowska-Bold and K. Graham and E. Gramstad and S. Grancagnolo and C. M. Grant and P. M. Gravila and F. G. Gravili and H. M. Gray and M. Greco and M. J. Green and C. Grefe and A. S. Grefsrud and I. M. Gregor and K. T. Greif and P. Grenier and S. G. Grewe and A. A. Grillo and K. Grimm and S. Grinstein and J.-F. Grivaz and E. Gross and J. Grosse-Knetter and L. Guan and J. G. R. Guerrero Rojas and G. Guerrieri and R. Gugel and J. A. M. Guhit and A. Guida and E. Guilloton and S. Guindon and F. Guo and J. Guo and L. Guo and Y. Guo and A. Gupta and R. Gupta and S. Gurbuz and S. S. Gurdasani and G. Gustavino and P. Gutierrez and L. F. Gutierrez Zagazeta and M. Gutsche and C. Gutschow and C. Gwenlan and C. B. Gwilliam and E. S. Haaland and A. Haas and M. Habedank and C. Haber and H. K. Hadavand and A. Hadef and A. I. Hagan and J. J. Hahn and E. H. Haines and M. Haleem and J. Haley and G. D. Hallewell and L. Halser and K. Hamano and M. Hamer and E. J. Hampshire and J. Han and L. Han and S. Han and Y. F. Han and K. Hanagaki and M. Hance and D. A. Hangal and H. Hanif and M. D. Hank and J. B. Hansen and P. H. Hansen and D. Harada and T. Harenberg and S. Harkusha and M. L. Harris and Y. T. Harris and J. Harrison and N. M. Harrison and P. F. Harrison and N. M. Hartman and N. M. Hartmann and R. Z. Hasan and Y. Hasegawa and F. Haslbeck and S. Hassan and R. Hauser and C. M. Hawkes and R. J. Hawkings and Y. Hayashi and D. Hayden and C. Hayes and R. L. Hayes and C. P. Hays and J. M. Hays and H. S. Hayward and F. He and M. He and Y. He and N. B. Heatley and V. Hedberg and A. L. Heggelund and N. D. Hehir and C. Heidegger and K. K. Heidegger and J. Heilman and S. Heim and T. Heim and J. G. Heinlein and J. J. Heinrich and L. Heinrich and J. Hejbal and A. Held and S. Hellesund and C. M. Helling and S. Hellman and R. C. W. Henderson and L. Henkelmann and A. M. Henriques Correia and H. Herde and Y. Hernández Jiménez and L. M. Herrmann and T. Herrmann and G. Herten and R. Hertenberger and L. Hervas and M. E. Hesping and N. P. Hessey and J. Hessler and M. Hidaoui and N. Hidic and E. Hill and S. J. Hillier and J. R. Hinds and F. Hinterkeuser and M. Hirose and S. Hirose and D. Hirschbuehl and T. G. Hitchings and B. Hiti and J. Hobbs and R. Hobincu and N. Hod and M. C. Hodgkinson and B. H. Hodkinson and A. Hoecker and D. D. Hofer and J. Hofer and T. Holm and M. Holzbock and L. B. A. H. Hommels and B. P. Honan and J. J. Hong and J. Hong and T. M. Hong and B. H. Hooberman and W. H. Hopkins and M. C. Hoppesch and Y. Horii and M. E. Horstmann and S. Hou and M. R. Housenga and A. S. Howard and J. Howarth and J. Hoya and M. Hrabovsky and A. Hrynevich and T. Hryn’ova and P. J. Hsu and S.-C. Hsu and T. Hsu and M. Hu and Q. Hu and S. Huang and X. Huang and Y. Huang and Z. Huang and Z. Hubacek and M. Huebner and F. Huegging and T. B. Huffman and M. Hufnagel Maranha De Faria and C. A. Hugli and M. Huhtinen and S. K. Huiberts and R. Hulsken and N. Huseynov and J. Huston and J. Huth and R. Hyneman and G. Iacobucci and G. Iakovidis and L. Iconomidou-Fayard and J. P. Iddon and P. Iengo and R. Iguchi and Y. Iiyama and T. Iizawa and Y. Ikegami and N. Ilic and H. Imam and G. Inacio Goncalves and T. Ingebretsen Carlson and J. M. Inglis and G. Introzzi and M. Iodice and V. Ippolito and R. K. Irwin and M. Ishino and W. Islam and C. Issever and S. Istin and H. Ito and R. Iuppa and A. Ivina and J. M. Izen and V. Izzo and P. Jacka and P. Jackson and C. S. Jagfeld and G. Jain and P. Jain and K. Jakobs and T. Jakoubek and J. Jamieson and W. Jang and M. Javurkova and P. Jawahar and L. Jeanty and J. Jejelava and P. Jenni and C. E. Jessiman and C. Jia and H. Jia and J. Jia and X. Jia and Z. Jia and C. Jiang and S. Jiggins and J. Jimenez Pena and S. Jin and A. Jinaru and O. Jinnouchi and P. Johansson and K. A. Johns and J. W. Johnson and F. A. Jolly and D. M. Jones and E. Jones and K. S. Jones and P. Jones and R. W. L. Jones and T. J. Jones and H. L. Joos and R. Joshi and J. Jovicevic and X. Ju and J. J. Junggeburth and T. Junkermann and A. Juste Rozas and M. K. Juzek and S. Kabana and A. Kaczmarska and M. Kado and H. Kagan and M. Kagan and A. Kahn and C. Kahra and T. Kaji and E. Kajomovitz and N. Kakati and I. Kalaitzidou and C. W. Kalderon and N. J. Kang and D. Kar and K. Karava and M. J. Kareem and E. Karentzos and O. Karkout and S. N. Karpov and Z. M. Karpova and V. Kartvelishvili and A. N. Karyukhin and E. Kasimi and J. Katzy and S. Kaur and K. Kawade and M. P. Kawale and C. Kawamoto and T. Kawamoto and E. F. Kay and F. I. Kaya and S. Kazakos and V. F. Kazanin and Y. Ke and J. M. Keaveney and R. Keeler and G. V. Kehris and J. S. Keller and J. J. Kempster and O. Kepka and B. P. Kerridge and S. Kersten and B. P. Kerševan and L. Keszeghova and S. Ketabchi Haghighat and R. A. Khan and A. Khanov and A. G. Kharlamov and T. Kharlamova and E. E. Khoda and M. Kholodenko and T. J. Khoo and G. Khoriauli and J. Khubua and Y. A. R. Khwaira and B. Kibirige and D. Kim and D. W. Kim and Y. K. Kim and N. Kimura and M. K. Kingston and A. Kirchhoff and C. Kirfel and F. Kirfel and J. Kirk and A. E. Kiryunin and S. Kita and C. Kitsaki and O. Kivernyk and M. Klassen and C. Klein and L. Klein and M. H. Klein and S. B. Klein and U. Klein and A. Klimentov and T. Klioutchnikova and P. Kluit and S. Kluth and E. Kneringer and T. M. Knight and A. Knue and D. Kobylianskii and S. F. Koch and M. Kocian and P. Kodyš and D. M. Koeck and P. T. Koenig and T. Koffas and O. Kolay and I. Koletsou and T. Komarek and K. Köneke and A. X. Y. Kong and T. Kono and N. Konstantinidis and P. Kontaxakis and B. Konya and R. Kopeliansky and S. Koperny and K. Korcyl and K. Kordas and A. Korn and S. Korn and I. Korolkov and N. Korotkova and B. Kortman and O. Kortner and S. Kortner and W. H. Kostecka and V. V. Kostyukhin and A. Kotsokechagia and A. Kotwal and A. Koulouris and A. Kourkoumeli-Charalampidi and C. Kourkoumelis and E. Kourlitis and O. Kovanda and R. Kowalewski and W. Kozanecki and A. S. Kozhin and V. A. Kramarenko and G. Kramberger and P. Kramer and M. W. Krasny and A. Krasznahorkay and A. C. Kraus and J. W. Kraus and J. A. Kremer and T. Kresse and L. Kretschmann and J. Kretzschmar and K. Kreul and P. Krieger and K. Krizka and K. Kroeninger and H. Kroha and J. Kroll and K. S. Krowpman and U. Kruchonak and H. Krüger and N. Krumnack and M. C. Kruse and O. Kuchinskaia and S. Kuday and S. Kuehn and R. Kuesters and T. Kuhl and V. Kukhtin and Y. Kulchitsky and S. Kuleshov and M. Kumar and N. Kumari and P. Kumari and A. Kupco and T. Kupfer and A. Kupich and O. Kuprash and H. Kurashige and L. L. Kurchaninov and O. Kurdysh and Y. A. Kurochkin and A. Kurova and M. Kuze and A. K. Kvam and J. Kvita and T. Kwan and N. G. Kyriacou and L. A. O. Laatu and C. Lacasta and F. Lacava and H. Lacker and D. Lacour and N. N. Lad and E. Ladygin and A. Lafarge and B. Laforge and T. Lagouri and F. Z. Lahbabi and S. Lai and J. E. Lambert and S. Lammers and W. Lampl and C. Lampoudis and G. Lamprinoudis and A. N. Lancaster and E. Lançon and U. Landgraf and M. P. J. Landon and V. S. Lang and O. K. B. Langrekken and A. J. Lankford and F. Lanni and K. Lantzsch and A. Lanza and M. Lanzac Berrocal and J. F. Laporte and T. Lari and F. Lasagni Manghi and M. Lassnig and V. Latonova and A. Laurier and S. D. Lawlor and Z. Lawrence and R. Lazaridou and M. Lazzaroni and B. Le and H. D. M. Le and E. M. Le Boulicaut and L. T. Le Pottier and B. Leban and A. Lebedev and M. LeBlanc and F. Ledroit-Guillon and S. C. Lee and S. Lee and T. F. Lee and L. L. Leeuw and M. Lefebvre and C. Leggett and G. Lehmann Miotto and M. Leigh and W. A. Leight and W. Leinonen and A. Leisos and M. A. L. Leite and C. E. Leitgeb and R. Leitner and K. J. C. Leney and T. Lenz and S. Leone and C. Leonidopoulos and A. Leopold and R. Les and C. G. Lester and M. Levchenko and J. Levêque and L. J. Levinson and G. Levrini and M. P. Lewicki and C. Lewis and D. J. Lewis and L. Lewitt and A. Li and B. Li and C. Li and C-Q. Li and H. Li and J. Li and K. Li and L. Li and M. Li and S. Li and T. Li and X. Li and Z. Li and S. Liang and Z. Liang and M. Liberatore and B. Liberti and K. Lie and J. Lieber Marin and H. Lien and H. Lin and K. Lin and L. Linden and R. E. Lindley and J. H. Lindon and J. Ling and E. Lipeles and A. Lipniacka and A. Lister and J. D. Little and B. Liu and B. X. Liu and D. Liu and E. H. L. Liu and J. B. Liu and J. K. K. Liu and K. Liu and M. Liu and M. Y. Liu and P. Liu and Q. Liu and X. Liu and Y. Liu and Y. L. Liu and Y. W. Liu and S. L. Lloyd and E. M. Lobodzinska and P. Loch and E. Lodhi and T. Lohse and K. Lohwasser and E. Loiacono and J. D. Lomas and J. D. Long and I. Longarini and R. Longo and I. Lopez Paz and A. Lopez Solis and N. A. Lopez-canelas and N. Lorenzo Martinez and A. M. Lory and M. Losada and G. Löschcke Centeno and O. Loseva and X. Lou and A. Lounis and P. A. Love and G. Lu and M. Lu and S. Lu and Y. J. Lu and H. J. Lubatti and C. Luci and F. L. Lucio Alves and F. Luehring and O. Lukianchuk and B. S. Lunday and O. Lundberg and B. Lund-Jensen and N. A. Luongo and M. S. Lutz and A. B. Lux and D. Lynn and R. Lysak and E. Lytken and V. Lyubushkin and T. Lyubushkina and M. M. Lyukova and M. Firdaus M. Soberi and H. Ma and K. Ma and L. L. Ma and W. Ma and Y. Ma and J. C. MacDonald and P. C. Machado De Abreu Farias and R. Madar and T. Madula and J. Maeda and T. Maeno and H. Maguire and V. Maiboroda and A. Maio and K. Maj and O. Majersky and S. Majewski and N. Makovec and V. Maksimovic and B. Malaescu and Pa. Malecki and V. P. Maleev and F. Malek and M. Mali and D. Malito and U. Mallik and S. Maltezos and S. Malyukov and J. Mamuzic and G. Mancini and M. N. Mancini and G. Manco and J. P. Mandalia and S. S. Mandarry and I. Mandić and L. Manhaes de Andrade Filho and I. M. Maniatis and J. Manjarres Ramos and D. C. Mankad and A. Mann and S. Manzoni and L. Mao and X. Mapekula and A. Marantis and G. Marchiori and M. Marcisovsky and C. Marcon and M. Marinescu and S. Marium and M. Marjanovic and A. Markhoos and M. Markovitch and M. K. Maroun and E. J. Marshall and Z. Marshall and S. Marti-Garcia and J. Martin and T. A. Martin and V. J. Martin and B. Martin dit Latour and L. Martinelli and M. Martinez and P. Martinez Agullo and V. I. Martinez Outschoorn and P. Martinez Suarez and S. Martin-Haugh and G. Martinovicova and V. S. Martoiu and A. C. Martyniuk and A. Marzin and D. Mascione and L. Masetti and J. Masik and A. L. Maslennikov and S. L. Mason and P. Massarotti and P. Mastrandrea and A. Mastroberardino and T. Masubuchi and T. T. Mathew and T. Mathisen and J. Matousek and D. M. Mattern and J. Maurer and T. Maurin and A. J. Maury and B. Maček and D. A. Maximov and A. E. May and R. Mazini and I. Maznas and M. Mazza and S. M. Mazza and E. Mazzeo and J. P. Mc Gowan and S. P. Mc Kee and C. A. Mc Lean and C. C. McCracken and E. F. McDonald and A. E. McDougall and J. A. Mcfayden and R. P. McGovern and R. P. Mckenzie and T. C. Mclachlan and D. J. Mclaughlin and S. J. McMahon and C. M. Mcpartland and R. A. McPherson and S. Mehlhase and A. Mehta and D. Melini and B. R. Mellado Garcia and A. H. Melo and F. Meloni and A. M. Mendes Jacques Da Costa and H. Y. Meng and L. Meng and S. Menke and M. Mentink and E. Meoni and G. Mercado and S. Merianos and C. Merlassino and L. Merola and C. Meroni and J. Metcalfe and A. S. Mete and E. Meuser and C. Meyer and J-P. Meyer and R. P. Middleton and L. Mijović and G. Mikenberg and M. Mikestikova and M. Mikuž and H. Mildner and A. Milic and D. W. Miller and E. H. Miller and L. S. Miller and A. Milov and D. A. Milstead and T. Min and A. A. Minaenko and I. A. Minashvili and A. I. Mincer and B. Mindur and M. Mineev and Y. Mino and L. M. Mir and M. Miralles Lopez and M. Mironova and M. C. Missio and A. Mitra and V. A. Mitsou and Y. Mitsumori and O. Miu and P. S. Miyagawa and T. Mkrtchyan and M. Mlinarevic and T. Mlinarevic and M. Mlynarikova and S. Mobius and P. Mogg and M. H. Mohamed Farook and A. F. Mohammed and S. Mohapatra and G. Mokgatitswane and L. Moleri and B. Mondal and S. Mondal and K. Mönig and E. Monnier and L. Monsonis Romero and J. Montejo Berlingen and A. Montella and M. Montella and F. Montereali and F. Monticelli and S. Monzani and A. Morancho Tarda and N. Morange and A. L. Moreira De Carvalho and M. Moreno Llácer and C. Moreno Martinez and J. M. Moreno Perez and P. Morettini and S. Morgenstern and M. Morii and M. Morinaga and M. Moritsu and F. Morodei and P. Moschovakos and B. Moser and M. Mosidze and T. Moskalets and P. Moskvitina and J. Moss and P. Moszkowicz and A. Moussa and Y. Moyal and E. J. W. Moyse and O. Mtintsilana and S. Muanza and J. Mueller and D. Muenstermann and R. Müller and G. A. Mullier and A. J. Mullin and J. J. Mullin and A. E. Mulski and D. P. Mungo and D. Munoz Perez and F. J. Munoz Sanchez and M. Murin and W. J. Murray and M. Muškinja and C. Mwewa and A. G. Myagkov and A. J. Myers and G. Myers and M. Myska and B. P. Nachman and K. Nagai and K. Nagano and R. Nagasaka and J. L. Nagle and E. Nagy and A. M. Nairz and Y. Nakahama and K. Nakamura and K. Nakkalil and H. Nanjo and E. A. Narayanan and I. Naryshkin and L. Nasella and S. Nasri and C. Nass and G. Navarro and J. Navarro-Gonzalez and R. Nayak and A. Nayaz and P. Y. Nechaeva and S. Nechaeva and F. Nechansky and L. Nedic and T. J. Neep and A. Negri and M. Negrini and C. Nellist and C. Nelson and K. Nelson and S. Nemecek and M. Nessi and M. S. Neubauer and F. Neuhaus and J. Neundorf and J. Newell and P. R. Newman and C. W. Ng and Y. W. Y. Ng and B. Ngair and H. D. N. Nguyen and R. B. Nickerson and R. Nicolaidou and J. Nielsen and M. Niemeyer and J. Niermann and N. Nikiforou and V. Nikolaenko and I. Nikolic-Audit and K. Nikolopoulos and P. Nilsson and I. Ninca and G. Ninio and A. Nisati and N. Nishu and R. Nisius and N. Nitika and J-E. Nitschke and E. K. Nkadimeng and T. Nobe and T. Nommensen and M. B. Norfolk and B. J. Norman and M. Noury and J. Novak and T. Novak and L. Novotny and R. Novotny and L. Nozka and K. Ntekas and N. M. J. Nunes De Moura Junior and J. Ocariz and A. Ochi and I. Ochoa and S. Oerdek and J. T. Offermann and A. Ogrodnik and A. Oh and C. C. Ohm and H. Oide and R. Oishi and M. L. Ojeda and Y. Okumura and L. F. Oleiro Seabra and I. Oleksiyuk and S. A. Olivares Pino and G. Oliveira Correa and D. Oliveira Damazio and J. L. Oliver and Ö. O. Öncel and A. P. O’Neill and A. Onofre and P. U. E. Onyisi and M. J. Oreglia and D. Orestano and N. Orlando and R. S. Orr and L. M. Osojnak and R. Ospanov and Y. Osumi and G. Otero y Garzon and H. Otono and P. S. Ott and G. J. Ottino and M. Ouchrif and F. Ould-Saada and T. Ovsiannikova and M. Owen and R. E. Owen and V. E. Ozcan and F. Ozturk and N. Ozturk and S. Ozturk and H. A. Pacey and A. Pacheco Pages and C. Padilla Aranda and G. Padovano and S. Pagan Griso and G. Palacino and A. Palazzo and J. Pampel and J. Pan and T. Pan and D. K. Panchal and C. E. Pandini and J. G. Panduro Vazquez and H. D. Pandya and H. Pang and P. Pani and G. Panizzo and L. Panwar and L. Paolozzi and S. Parajuli and A. Paramonov and C. Paraskevopoulos and D. Paredes Hernandez and A. Pareti and K. R. Park and T. H. Park and M. A. Parker and F. Parodi and V. A. Parrish and J. A. Parsons and U. Parzefall and B. Pascual Dias and L. Pascual Dominguez and E. Pasqualucci and S. Passaggio and F. Pastore and P. Patel and U. M. Patel and J. R. Pater and T. Pauly and F. Pauwels and C. I. Pazos and M. Pedersen and R. Pedro and S. V. Peleganchuk and O. Penc and E. A. Pender and S. Peng and G. D. Penn and K. E. Penski and M. Penzin and B. S. Peralva and A. P. Pereira Peixoto and L. Pereira Sanchez and D. V. Perepelitsa and G. Perera and E. Perez Codina and M. Perganti and H. Pernegger and S. Perrella and O. Perrin and K. Peters and R. F. Y. Peters and B. A. Petersen and T. C. Petersen and E. Petit and V. Petousis and C. Petridou and T. Petru and A. Petrukhin and M. Pettee and A. Petukhov and K. Petukhova and R. Pezoa and L. Pezzotti and G. Pezzullo and A. J. Pfleger and T. M. Pham and T. Pham and P. W. Phillips and G. Piacquadio and E. Pianori and F. Piazza and R. Piegaia and D. Pietreanu and A. D. Pilkington and M. Pinamonti and J. L. Pinfold and B. C. Pinheiro Pereira and J. Pinol Bel and A. E. Pinto Pinoargote and L. Pintucci and K. M. Piper and A. Pirttikoski and D. A. Pizzi and L. Pizzimento and A. Pizzini and M.-A. Pleier and V. Pleskot and E. Plotnikova and G. Poddar and R. Poettgen and L. Poggioli and S. Polacek and G. Polesello and A. Poley and A. Polini and C. S. Pollard and Z. B. Pollock and E. Pompa Pacchi and N. I. Pond and D. Ponomarenko and L. Pontecorvo and S. Popa and G. A. Popeneciu and A. Poreba and D. M. Portillo Quintero and S. Pospisil and M. A. Postill and P. Postolache and K. Potamianos and P. A. Potepa and I. N. Potrap and C. J. Potter and H. Potti and J. Poveda and M. E. Pozo Astigarraga and A. Prades Ibanez and J. Pretel and D. Price and M. Primavera and L. Primomo and M. A. Principe Martin and R. Privara and T. Procter and M. L. Proffitt and N. Proklova and K. Prokofiev and G. Proto and J. Proudfoot and M. Przybycien and W. W. Przygoda and A. Psallidas and J. E. Puddefoot and D. Pudzha and D. Pyatiizbyantseva and J. Qian and R. Qian and D. Qichen and Y. Qin and T. Qiu and A. Quadt and M. Queitsch-Maitland and G. Quetant and R. P. Quinn and G. Rabanal Bolanos and D. Rafanoharana and F. Raffaeli and F. Ragusa and J. L. Rainbolt and J. A. Raine and S. Rajagopalan and E. Ramakoti and L. Rambelli and I. A. Ramirez-Berend and K. Ran and D. S. Rankin and N. P. Rapheeha and H. Rasheed and V. Raskina and D. F. Rassloff and A. Rastogi and S. Rave and S. Ravera and B. Ravina and I. Ravinovich and M. Raymond and A. L. Read and N. P. Readioff and D. M. Rebuzzi and G. Redlinger and A. S. Reed and K. Reeves and J. A. Reidelsturz and D. Reikher and A. Rej and C. Rembser and M. Renda and F. Renner and A. G. Rennie and A. L. Rescia and S. Resconi and M. Ressegotti and S. Rettie and J. G. Reyes Rivera and E. Reynolds and O. L. Rezanova and P. Reznicek and H. Riani and N. Ribaric and E. Ricci and R. Richter and S. Richter and E. Richter-Was and M. Ridel and S. Ridouani and P. Rieck and P. Riedler and E. M. Riefel and J. O. Rieger and M. Rijssenbeek and M. Rimoldi and L. Rinaldi and P. Rincke and T. T. Rinn and M. P. Rinnagel and G. Ripellino and I. Riu and J. C. Rivera Vergara and F. Rizatdinova and E. Rizvi and B. R. Roberts and S. S. Roberts and S. H. Robertson and D. Robinson and M. Robles Manzano and A. Robson and A. Rocchi and C. Roda and S. Rodriguez Bosca and Y. Rodriguez Garcia and A. M. Rodríguez Vera and S. Roe and J. T. Roemer and A. R. Roepe-Gier and O. Røhne and R. A. Rojas and C. P. A. Roland and J. Roloff and A. Romaniouk and E. Romano and M. Romano and A. C. Romero Hernandez and N. Rompotis and L. Roos and S. Rosati and B. J. Rosser and E. Rossi and L. P. Rossi and L. Rossini and R. Rosten and M. Rotaru and B. Rottler and C. Rougier and D. Rousseau and D. Rousso and A. Roy and S. Roy-Garand and A. Rozanov and Z. M. A. Rozario and Y. Rozen and A. Rubio Jimenez and V. H. Ruelas Rivera and T. A. Ruggeri and A. Ruggiero and A. Ruiz-Martinez and A. Rummler and Z. Rurikova and N. A. Rusakovich and H. L. Russell and G. Russo and J. P. Rutherfoord and S. Rutherford Colmenares and M. Rybar and E. B. Rye and A. Ryzhov and J. A. Sabater Iglesias and H. F-W. Sadrozinski and F. Safai Tehrani and B. Safarzadeh Samani and S. Saha and M. Sahinsoy and A. Saibel and M. Saimpert and M. Saito and T. Saito and A. Sala and D. Salamani and A. Salnikov and J. Salt and A. Salvador Salas and D. Salvatore and F. Salvatore and A. Salzburger and D. Sammel and E. Sampson and D. Sampsonidis and D. Sampsonidou and J. Sánchez and V. Sanchez Sebastian and H. Sandaker and C. O. Sander and J. A. Sandesara and M. Sandhoff and C. Sandoval and L. Sanfilippo and D. P. C. Sankey and T. Sano and A. Sansoni and L. Santi and C. Santoni and H. Santos and A. Santra and E. Sanzani and K. A. Saoucha and J. G. Saraiva and J. Sardain and O. Sasaki and K. Sato and C. Sauer and E. Sauvan and P. Savard and R. Sawada and C. Sawyer and L. Sawyer and C. Sbarra and A. Sbrizzi and T. Scanlon and J. Schaarschmidt and U. Schäfer and A. C. Schaffer and D. Schaile and R. D. Schamberger and C. Scharf and M. M. Schefer and V. A. Schegelsky and D. Scheirich and M. Schernau and C. Scheulen and C. Schiavi and M. Schioppa and B. Schlag and S. Schlenker and J. Schmeing and M. A. Schmidt and K. Schmieden and C. Schmitt and N. Schmitt and S. Schmitt and L. Schoeffel and A. Schoening and P. G. Scholer and E. Schopf and M. Schott and J. Schovancova and S. Schramm and T. Schroer and H-C. Schultz-Coulon and M. Schumacher and B. A. Schumm and Ph. Schune and A. J. Schuy and H. R. Schwartz and A. Schwartzman and T. A. Schwarz and Ph. Schwemling and R. Schwienhorst and F. G. Sciacca and A. Sciandra and G. Sciolla and F. Scuri and C. D. Sebastiani and K. Sedlaczek and S. C. Seidel and A. Seiden and B. D. Seidlitz and C. Seitz and J. M. Seixas and G. Sekhniaidze and L. Selem and N. Semprini-Cesari and A. Semushin and D. Sengupta and V. Senthilkumar and L. Serin and M. Sessa and H. Severini and F. Sforza and A. Sfyrla and Q. Sha and E. Shabalina and A. H. Shah and R. Shaheen and J. D. Shahinian and D. Shaked Renous and L. Y. Shan and M. Shapiro and A. Sharma and A. S. Sharma and P. Sharma and P. B. Shatalov and K. Shaw and S. M. Shaw and Q. Shen and D. J. Sheppard and P. Sherwood and L. Shi and X. Shi and S. Shimizu and C. O. Shimmin and I. P. J. Shipsey and S. Shirabe and M. Shiyakova and M. J. Shochet and D. R. Shope and B. Shrestha and S. Shrestha and I. Shreyber and M. J. Shroff and P. Sicho and A. M. Sickles and E. Sideras Haddad and A. C. Sidley and A. Sidoti and F. Siegert and Dj. Sijacki and F. Sili and J. M. Silva and I. Silva Ferreira and M. V. Silva Oliveira and S. B. Silverstein and S. Simion and R. Simoniello and E. L. Simpson and H. Simpson and L. R. Simpson and S. Simsek and S. Sindhu and P. Sinervo and S. Singh and S. Sinha and M. Sioli and I. Siral and E. Sitnikova and J. Sjölin and A. Skaf and E. Skorda and P. Skubic and M. Slawinska and V. Smakhtin and B. H. Smart and S. Yu. Smirnov and Y. Smirnov and L. N. Smirnova and O. Smirnova and A. C. Smith and D. R. Smith and E. A. Smith and J. L. Smith and R. Smith and H. Smitmanns and M. Smizanska and K. Smolek and A. A. Snesarev and H. L. Snoek and S. Snyder and R. Sobie and A. Soffer and C. A. Solans Sanchez and E. Yu. Soldatov and U. Soldevila and A. A. Solodkov and S. Solomon and A. Soloshenko and K. Solovieva and O. V. Solovyanov and P. Sommer and A. Sonay and W. Y. Song and A. Sopczak and A. L. Sopio and F. Sopkova and J. D. Sorenson and I. R. Sotarriva Alvarez and V. Sothilingam and O. J. Soto Sandoval and S. Sottocornola and R. Soualah and Z. Soumaimi and D. South and N. Soybelman and S. Spagnolo and M. Spalla and D. Sperlich and G. Spigo and B. Spisso and D. P. Spiteri and M. Spousta and E. J. Staats and R. Stamen and A. Stampekis and E. Stanecka and W. Stanek-Maslouska and M. V. Stange and B. Stanislaus and M. M. Stanitzki and B. Stapf and E. A. Starchenko and G. H. Stark and J. Stark and P. Staroba and P. Starovoitov and S. Stärz and R. Staszewski and G. Stavropoulos and A. Stefl and P. Steinberg and B. Stelzer and H. J. Stelzer and O. Stelzer-Chilton and H. Stenzel and T. J. Stevenson and G. A. Stewart and J. R. Stewart and M. C. Stockton and G. Stoicea and M. Stolarski and S. Stonjek and A. Straessner and J. Strandberg and S. Strandberg and M. Stratmann and M. Strauss and T. Strebler and P. Strizenec and R. Ströhmer and D. M. Strom and R. Stroynowski and A. Strubig and S. A. Stucci and B. Stugu and J. Stupak and N. A. Styles and D. Su and S. Su and W. Su and X. Su and D. Suchy and K. Sugizaki and V. V. Sulin and M. J. Sullivan and D. M. S. Sultan and L. Sultanaliyeva and S. Sultansoy and T. Sumida and S. Sun and O. Sunneborn Gudnadottir and N. Sur and M. R. Sutton and H. Suzuki and M. Svatos and M. Swiatlowski and T. Swirski and I. Sykora and M. Sykora and T. Sykora and D. Ta and K. Tackmann and A. Taffard and R. Tafirout and J. S. Tafoya Vargas and Y. Takubo and M. Talby and A. A. Talyshev and K. C. Tam and N. M. Tamir and A. Tanaka and J. Tanaka and R. Tanaka and M. Tanasini and Z. Tao and S. Tapia Araya and S. Tapprogge and A. Tarek Abouelfadl Mohamed and S. Tarem and K. Tariq and G. Tarna and G. F. Tartarelli and M. J. Tartarin and P. Tas and M. Tasevsky and E. Tassi and A. C. Tate and G. Tateno and Y. Tayalati and G. N. Taylor and W. Taylor and R. Teixeira De Lima and P. Teixeira-Dias and J. J. Teoh and K. Terashi and J. Terron and S. Terzo and M. Testa and R. J. Teuscher and A. Thaler and O. Theiner and T. Theveneaux-Pelzer and O. Thielmann and D. W. Thomas and J. P. Thomas and E. A. Thompson and P. D. Thompson and E. Thomson and R. E. Thornberry and C. Tian and Y. Tian and V. Tikhomirov and Yu. A. Tikhonov and S. Timoshenko and D. Timoshyn and E. X. L. Ting and P. Tipton and A. Tishelman-Charny and S. H. Tlou and K. Todome and S. Todorova-Nova and S. Todt and L. Toffolin and M. Togawa and J. Tojo and S. Tokár and K. Tokushuku and O. Toldaiev and M. Tomoto and L. Tompkins and K. W. Topolnicki and E. Torrence and H. Torres and E. Torró Pastor and M. Toscani and C. Tosciri and M. Tost and D. R. Tovey and I. S. Trandafir and T. Trefzger and A. Tricoli and I. M. Trigger and S. Trincaz-Duvoid and D. A. Trischuk and B. Trocmé and A. Tropina and L. Truong and M. Trzebinski and A. Trzupek and F. Tsai and M. Tsai and A. Tsiamis and P. V. Tsiareshka and S. Tsigaridas and A. Tsirigotis and V. Tsiskaridze and E. G. Tskhadadze and M. Tsopoulou and Y. Tsujikawa and I. I. Tsukerman and V. Tsulaia and S. Tsuno and K. Tsuri and D. Tsybychev and Y. Tu and A. Tudorache and V. Tudorache and A. N. Tuna and S. Turchikhin and I. Turk Cakir and R. Turra and T. Turtuvshin and P. M. Tuts and S. Tzamarias and E. Tzovara and F. Ukegawa and P. A. Ulloa Poblete and E. N. Umaka and G. Unal and A. Undrus and G. Unel and J. Urban and P. Urrejola and G. Usai and R. Ushioda and M. Usman and F. Ustuner and Z. Uysal and V. Vacek and B. Vachon and T. Vafeiadis and A. Vaitkus and C. Valderanis and E. Valdes Santurio and M. Valente and S. Valentinetti and A. Valero and E. Valiente Moreno and A. Vallier and J. A. Valls Ferrer and D. R. Van Arneman and T. R. Van Daalen and A. Van Der Graaf and P. Van Gemmeren and M. Van Rijnbach and S. Van Stroud and I. Van Vulpen and P. Vana and M. Vanadia and U. M. Vande Voorde and W. Vandelli and E. R. Vandewall and D. Vannicola and L. Vannoli and R. Vari and E. W. Varnes and C. Varni and T. Varol and D. Varouchas and L. Varriale and K. E. Varvell and M. E. Vasile and L. Vaslin and A. Vasyukov and L. M. Vaughan and R. Vavricka and T. Vazquez Schroeder and J. Veatch and V. Vecchio and M. J. Veen and I. Veliscek and L. M. Veloce and F. Veloso and S. Veneziano and A. Ventura and S. Ventura Gonzalez and A. Verbytskyi and M. Verducci and C. Vergis and M. Verissimo De Araujo and W. Verkerke and J. C. Vermeulen and C. Vernieri and M. Vessella and M. C. Vetterli and A. Vgenopoulos and N. Viaux Maira and T. Vickey and O. E. Vickey Boeriu and G. H. A. Viehhauser and L. Vigani and M. Vigl and M. Villa and M. Villaplana Perez and E. M. Villhauer and E. Vilucchi and M. G. Vincter and A. Visibile and C. Vittori and I. Vivarelli and E. Voevodina and F. Vogel and J. C. Voigt and P. Vokac and Yu. Volkotrub and E. Von Toerne and B. Vormwald and V. Vorobel and K. Vorobev and M. Vos and K. Voss and M. Vozak and L. Vozdecky and N. Vranjes and M. Vranjes Milosavljevic and M. Vreeswijk and N. K. Vu and R. Vuillermet and O. Vujinovic and I. Vukotic and I. K. Vyas and S. Wada and C. Wagner and J. M. Wagner and W. Wagner and S. Wahdan and H. Wahlberg and C. H. Waits and J. Walder and R. Walker and W. Walkowiak and A. Wall and E. J. Wallin and T. Wamorkar and A. Z. Wang and C. Wang and H. Wang and J. Wang and P. Wang and R. Wang and S. M. Wang and S. Wang and T. Wang and W. T. Wang and W. Wang and X. Wang and Y. Wang and Z. Wang and A. Warburton and R. J. Ward and N. Warrack and S. Waterhouse and A. T. Watson and H. Watson and M. F. Watson and E. Watton and G. Watts and B. M. Waugh and J. M. Webb and C. Weber and H. A. Weber and M. S. Weber and S. M. Weber and C. Wei and Y. Wei and A. R. Weidberg and E. J. Weik and J. Weingarten and C. Weiser and C. J. Wells and T. Wenaus and B. Wendland and T. Wengler and N. S. Wenke and N. Wermes and M. Wessels and A. M. Wharton and A. S. White and A. White and M. J. White and D. Whiteson and L. Wickremasinghe and W. Wiedenmann and M. Wielers and C. Wiglesworth and D. J. Wilbern and H. G. Wilkens and J. J. H. Wilkinson and D. M. Williams and H. H. Williams and S. Williams and S. Willocq and B. J. Wilson and P. J. Windischhofer and F. I. Winkel and F. Winklmeier and B. T. Winter and J. K. Winter and M. Wittgen and M. Wobisch and T. Wojtkowski and Z. Wolffs and J. Wollrath and M. W. Wolter and H. Wolters and M. C. Wong and E. L. Woodward and S. D. Worm and B. K. Wosiek and K. W. Woźniak and S. Wozniewski and K. Wraight and C. Wu and M. Wu and S. L. Wu and X. Wu and Y. Wu and Z. Wu and J. Wuerzinger and T. R. Wyatt and B. M. Wynne and S. Xella and L. Xia and M. Xia and M. Xie and S. Xin and A. Xiong and J. Xiong and D. Xu and H. Xu and L. Xu and R. Xu and T. Xu and Y. Xu and Z. Xu and B. Yabsley and S. Yacoob and Y. Yamaguchi and E. Yamashita and H. Yamauchi and T. Yamazaki and Y. Yamazaki and S. Yan and Z. Yan and H. J. Yang and H. T. Yang and S. Yang and T. Yang and X. Yang and Y. Yang and W-M. Yao and H. Ye and J. Ye and S. Ye and X. Ye and Y. Yeh and I. Yeletskikh and B. Yeo and M. R. Yexley and T. P. Yildirim and P. Yin and K. Yorita and S. Younas and C. J. S. Young and C. Young and C. Yu and Y. Yu and J. Yuan and M. Yuan and R. Yuan and L. Yue and M. Zaazoua and B. Zabinski and E. Zaid and Z. K. Zak and T. Zakareishvili and S. Zambito and J. A. Zamora Saa and J. Zang and D. Zanzi and O. Zaplatilek and C. Zeitnitz and H. Zeng and J. C. Zeng and D. T. Zenger, Jr and O. Zenin and T. Ženiš and S. Zenz and S. Zerradi and D. Zerwas and M. Zhai and D. F. Zhang and J. Zhang and K. Zhang and L. Zhang and P. Zhang and R. Zhang and S. Zhang and T. Zhang and X. Zhang and Y. Zhang and Z. Zhang and H. Zhao and T. Zhao and Y. Zhao and Z. Zhao and A. Zhemchugov and J. Zheng and K. Zheng and X. Zheng and Z. Zheng and D. Zhong and B. Zhou and H. Zhou and N. Zhou and Y. Zhou and C. G. Zhu and J. Zhu and X. Zhu and Y. Zhu and X. Zhuang and K. Zhukov and N. I. Zimine and J. Zinsser and M. Ziolkowski and L. Živković and A. Zoccoli and K. Zoch and T. G. Zorbas and O. Zormpa and W. Zou and L. Zwalinski}, doi = {10.1103/PhysRevLett.134.061803}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061803}, shortjournal = {Phys. Rev. Lett.}, title = {Search for magnetic monopole pair production in ultraperipheral Pb+Pb collisions at sNN=5.36 TeV with the ATLAS detector at the LHC}, volume = {134}, year = {2025}, }
• (2025). Atoms as electron accelerators for measuring the cross section of e+e−→Hadrons. PRL, 134(6), 061802. (www)

  @article{ , abstract = {The hadronic vacuum polarization contribution to ( g − 2 ) μ can be determined via dispersive methods from e + e − → hadrons data. We propose a novel approach to measure the hadronic cross section σ had ( s ) as an alternative to the initial-state radiation and energy scan techniques, which relies on positron annihilation off atomic electrons of a high Z target ( U 238 , Z = 92 ). We show that by leveraging the relativistic electron velocities of the inner atomic shells, a high-intensity 12 GeV positron beam, such as the one foreseen at JLab, can allow measuring σ had ( s ) with high statistical accuracy from the two-pion threshold up to above s ∼ 1 GeV .}, archive = {J_PRL}, author = {Fernando Arias-Aragón and Luc Darmé and Giovanni Grilli di Cortona and Enrico Nardi}, doi = {10.1103/PhysRevLett.134.061802}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061802}, shortjournal = {Phys. Rev. Lett.}, title = {Atoms as electron accelerators for measuring the cross section of e+e−→Hadrons}, volume = {134}, year = {2025}, }
• (2025). Measurement of the branching fraction ratios R(D+) and R(D*+) using muonic τ decays. PRL, 134(6), 061801. (www)

  @article{ , abstract = {The branching fraction ratios of B ¯ 0 → D + τ − ν ¯ τ and B ¯ 0 → D * + τ − ν ¯ τ decays are measured with respect to their muonic counterparts, using a data sample corresponding to an integrated luminosity of 2.0 fb − 1 collected by the LHCb experiment in proton-proton collisions at s = 13 TeV . The reconstructed final states are formed by combining D + mesons with τ − → μ − ν ¯ μ ν τ candidates, where the D + is reconstructed via the D + → K − π + π + decay. The results are R ( D + ) = 0.249 ± 0.043 ± 0.047 , R ( D * + ) = 0.402 ± 0.081 ± 0.085 , where the first uncertainties are statistical and the second systematic. The two measurements have a correlation coefficient of − 0.39 and are compatible with the standard model.}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and W. Baldini and H. Bao and J. Baptista de Souza Leite and M. Barbetti and I. R. Barbosa and R. J. Barlow and M. Barnyakov and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and F. Baryshnikov and J. M. Basels and G. Bassi and B. Batsukh and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and S. Belin and V. Bellee and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and N. Bondar and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and T. J. V. Bowcock and A. Boyer and C. Bozzi and M. J. Bradley and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and A. Butkevich and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and R. Calabrese and S. Calderon Ramirez and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and P. Camargo Magalhaes and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and J. Castro Godinez and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and C. A. Chavez Barajas and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and P. Collins and T. Colombo and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and E. Epple and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and K. M. Fischer and D. S. Fitzgerald and C. Fitzpatrick and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Fuehring and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and B. Ganie and H. Gao and R. Gao and Y. Gao and M. Garau and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and A. Gomes and S. Gomez Fernandez and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and J. Haimberger and M. Hajheidari and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and M. Hartmann and J. He and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and D. Hill and S. E. Hollitt and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and Y. Kang and C. Kar and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and P. Krokovny and W. Krupa and W. Krzemien and O. K. Kshyvanskyi and J. Kubat and S. Kubis and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and B. Leverington and A. Li and H. Li and K. Li and L. Li and P. Li and P.-R. Li and Q. Li and S. Li and T. Li and Y. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and S. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and J. Lomba Castro and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and C. Lucarelli and D. Lucchesi and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and R. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. M. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Santos and F. Martinez Vidal and A. Massafferri and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and S Meloni and F. M. Meng and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and A. Mödden and R. A. Mohammed and R. D. Moise and S. Mokhnenko and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and P. Nogarolli and P. Nogga and N. S. Nolte and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and O. Okhrimenko and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and A. Paul and C. J. Pawley and A. Pellegrino and J. Peng and M. Pepe Altarelli and S. Perazzini and D. Pereima and H. Pereira Da Costa and A. Pereiro Castro and P. Perret and A. Perro and K. Petridis and A. Petrolini and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and V. Pugatch and G. Punzi and S. Qasim and W. Qian and N. Qin and S. Qu and R. Quagliani and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and V. Ramos De Oliveira and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and M. Romero Lamas and A. Romero Vidal and G. Romolini and F. Ronchetti and M. Rotondo and S. R. Roy and M. S. Rudolph and T. Ruf and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and C. Sanchez Gras and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and G. Sarpis and M. Sarpis and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and Q. Shi and E. B. Shields and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and Y. Sun and D. S. Sundfeld Lima and W. Sutcliffe and P. N. Swallow and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and G. Vasquez and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Vesterinen and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and N. Voropaev and K. Vos and G. Vouters and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and J. Wendel and B. D. C. Westhenry and D. J. White and M. Whitehead and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. R. J. Williams and R. Williams and F. F. Wilson and W. Wislicki and M. Witek and L. Witola and C. P. Wong and G. Wormser and S. A. Wotton and H. Wu and J. Wu and Y. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and D. Yang and K. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and C. Y. Yu and J. Yu and X. Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and C. Zeng and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.061801}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061801}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of the branching fraction ratios R(D+) and R(D*+) using muonic τ decays}, volume = {134}, year = {2025}, }
• (2025). Distinguishable consequence of classical gravity on quantum matter. PRL, 134(6), 061501. (www)

  @article{ , abstract = {What if gravity is classical? If true, a consistent coexistence of classical gravity and quantum matter requires that gravity exhibit irreducible fluctuations. These fluctuations can mediate classical correlations, but not quantum entanglement, between the quantized motion of the gravitationally interacting matter. We use a consistent theory of quantum-classical dynamics in the Newtonian limit of gravity to show that experimentally relevant observables can conclusively test the hypothesis that gravity is classical. This can be done, for example, by letting highly coherent source masses interact with each other gravitationally, and performing precise measurements of the cross-correlation of their motion. Theory predicts a characteristic phase response that distinguishes classical gravity from quantum gravity, and from naive sources of decoherence. Such experiments are imminently viable.}, archive = {J_PRL}, author = {Serhii Kryhin and Vivishek Sudhir}, doi = {10.1103/PhysRevLett.134.061501}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061501}, shortjournal = {Phys. Rev. Lett.}, title = {Distinguishable consequence of classical gravity on quantum matter}, volume = {134}, year = {2025}, }
• (2025). Quadratic quasinormal mode dependence on linear mode parity. PRL, 134(6), 061401. (www)

  @article{ , abstract = {Quasinormal modes (QNMs) uniquely describe the dominant piece of the gravitational-wave ringdown of postmerger black holes. While the linear QNM regime has been extensively studied, recent work has highlighted the importance of second-perturbative-order, quadratic QNMs (QQNMs) arising from the nonlinear coupling of linear QNMs. Previous attempts to quantify the magnitude of these QQNMs have shown discrepant results. Using a new hyperboloidal framework, we resolve the discrepancy by showing that the QQNM/QNM ratio is a function not only of the black hole parameters but also of the ratio between even- and odd-parity linear QNMs: the ratio QQNM/QNM depends on what created the ringing black hole, but only through this ratio of even- to odd-parity linear perturbations.}, archive = {J_PRL}, author = {Patrick Bourg and Rodrigo Panosso Macedo and Andrew Spiers and Benjamin Leather and Béatrice Bonga and Adam Pound}, doi = {10.1103/PhysRevLett.134.061401}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061401}, shortjournal = {Phys. Rev. Lett.}, title = {Quadratic quasinormal mode dependence on linear mode parity}, volume = {134}, year = {2025}, }
• (2025). Nuclear recoil calibration at sub-keV energies in LUX and its impact on dark matter search sensitivity. PRL, 134(6), 061002. (www)

  @article{ , abstract = {Dual-phase xenon time projection chamber (TPC) detectors offer heightened sensitivities for dark matter detection across a spectrum of particle masses. To broaden their capability to low-mass dark matter interactions, we investigated the light and charge responses of liquid xenon (LXe) to sub-keV nuclear recoils. Using neutron events from a pulsed Adelphi Deuterium-Deuterium neutron generator, an in situ calibration was conducted on the LUX detector. We demonstrate direct measurements of light and charge yields down to 0.45 and 0.27 keV, respectively, both approaching single quanta production, the physical limit of LXe detectors. These results hold significant implications for the future of dual-phase xenon TPCs in detecting low-mass dark matter via nuclear recoils.}, archive = {J_PRL}, author = {D. S. Akerib and S. Alsum and H. M. Araújo and X. Bai and J. Balajthy and J. Bang and A. Baxter and E. P. Bernard and A. Bernstein and T. P. Biesiadzinski and E. M. Boulton and B. Boxer and P. Brás and S. Burdin and D. Byram and M. C. Carmona-Benitez and C. Chan and J. E. Cutter and L. de Viveiros and E. Druszkiewicz and A. Fan and S. Fiorucci and R. J. Gaitskell and C. Ghag and M. G. D. Gilchriese and C. Gwilliam and C. R. Hall and S. J. Haselschwardt and S. A. Hertel and D. P. Hogan and M. Horn and D. Q. Huang and C. M. Ignarra and R. G. Jacobsen and O. Jahangir and W. Ji and K. Kamdin and K. Kazkaz and D. Khaitan and E. V. Korolkova and S. Kravitz and V. A. Kudryavtsev and E. Leason and K. T. Lesko and J. Liao and J. Lin and A. Lindote and M. I. Lopes and A. Manalaysay and R. L. Mannino and N. Marangou and D. N. McKinsey and D.-M. Mei and J. A. Morad and A. St. J. Murphy and A. Naylor and C. Nehrkorn and H. N. Nelson and F. Neves and A. Nilima and K. C. Oliver-Mallory and K. J. Palladino and C. Rhyne and Q. Riffard and G. R. C. Rischbieter and P. Rossiter and S. Shaw and T. A. Shutt and C. Silva and M. Solmaz and V. N. Solovov and P. Sorensen and T. J. Sumner and N. Swanson and M. Szydagis and D. J. Taylor and R. Taylor and W. C. Taylor and B. P. Tennyson and P. A. Terman and D. R. Tiedt and W. H. To and L. Tvrznikova and U. Utku and A. Vacheret and A. Vaitkus and V. Velan and R. C. Webb and J. T. White and T. J. Whitis and M. S. Witherell and F. L. H. Wolfs and D. Woodward and X. Xiang and J. Xu and C. Zhang}, doi = {10.1103/PhysRevLett.134.061002}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061002}, shortjournal = {Phys. Rev. Lett.}, title = {Nuclear recoil calibration at sub-keV energies in LUX and its impact on dark matter search sensitivity}, volume = {134}, year = {2025}, }
• (2025). Ultrahigh-energy particle collisions and heavy dark matter at phase transitions. PRL, 134(6), 061001. (www)

  @article{ , abstract = {We initiate the study of “bubbletrons,” by which we mean ultrahigh-energy collisions of the particle shells that generically form at the walls of relativistic bubbles in cosmological first-order phase transitions (PT). As an application, we calculate the maximal dark matter mass M DM that bubbletrons can produce in a U ( 1 ) gauge PT, finding M DM ∼ 10 5 / 10 11 / 10 15 GeV for PT scales v ϕ ∼ 10 − 2 / 10 3 / 10 9 GeV . Bubbletrons realize a novel link between ultrahigh-energy phenomena and gravitational waves sourced at the PT, from nanohertz to megahertz frequencies.}, archive = {J_PRL}, author = {Iason Baldes and Maximilian Dichtl and Yann Gouttenoire and Filippo Sala}, doi = {10.1103/PhysRevLett.134.061001}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {061001}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrahigh-energy particle collisions and heavy dark matter at phase transitions}, volume = {134}, year = {2025}, }
• (2025). Observation of the two-photon landau-zener-stückelberg-majorana effect. PRL, 134(6), 060602. (www)

  @article{ , abstract = {Harnessing second-order processes enables new control schemes in quantum dynamics. We show that the Landau-Zener-Stückelberg-Majorana (LZSM) transition can be generalized to a virtual-state process in a three-level system, employing a phase modulated drive whereby two photons excite the system from the first to the third level while avoiding the second one. We implement experimentally this process in a transmon, achieving 98% population transfer. We predict and observe the doubling of LZSM velocity. Furthermore, we demonstrate robustness to amplitude and frequency offsets, made possible by the nearly exact cancellation of the two-photon ac Stark shift due to the presence of the fourth state.}, archive = {J_PRL}, author = {Isak Björkman and Marko Kuzmanović and Gheorghe Sorin Paraoanu}, doi = {10.1103/PhysRevLett.134.060602}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {060602}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of the two-photon landau-zener-stückelberg-majorana effect}, volume = {134}, year = {2025}, }
• (2025). Neural-network-based design of approximate gottesman-kitaev-preskill code. PRL, 134(6), 060601. (www)

  @article{ , abstract = {Gottesman-Kitaev-Preskill (GKP) encoding holds promise for continuous-variable fault-tolerant quantum computing. While an ideal GKP encoding is abstract and impractical due to its nonphysical nature, approximate versions provide viable alternatives. Conventional approximate GKP codewords are superpositions of multiple large-amplitude squeezed coherent states. This feature ensures correctability against single-photon loss and dephasing at short times, but also increases the difficulty of preparing the codewords. To minimize this tradeoff, we utilize a neural network to generate optimal approximate GKP states, allowing effective error correction with just a few squeezed coherent states. We find that such optimized GKP codes outperform the best conventional ones, requiring fewer squeezed coherent states, while maintaining simple and generalized stabilizer operators. Specifically, the former outperform the latter with just one-third of the number of squeezed coherent states at a squeezing level of 9.55 dB. This optimization drastically decreases the complexity of codewords while improving error correctability.}, archive = {J_PRL}, author = {Yexiong Zeng and Wei Qin and Ye-Hong Chen and Clemens Gneiting and Franco Nori}, doi = {10.1103/PhysRevLett.134.060601}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {060601}, shortjournal = {Phys. Rev. Lett.}, title = {Neural-network-based design of approximate gottesman-kitaev-preskill code}, volume = {134}, year = {2025}, }
• (2025). Floquet expansion by counting pump photons. PRL, 134(6), 060401. (www)

  @article{ , abstract = {Periodically driven systems engender a rich competition between the timescales of the drives and those of the system, leading to a limited ability to describe the system in full. We present a framework for the description of interacting bosonic driven systems via a Floquet expansion on top of a quantization that “counts” the drive photons, and provide compelling arguments for the superior performance of our method relative to standard Floquet approaches. Crucially, our approach extends beyond the rotating wave approximation and addresses the long-standing issue of mismatch between the quantum Floquet formalism and its classical counterpart. We, furthermore, pinpoint key corrections to the positions of multiphoton resonances, which are commonly used in the calibration and operation of qubit architectures.}, archive = {J_PRL}, author = {Kilian Seibold and Orjan Ameye and Oded Zilberberg}, doi = {10.1103/PhysRevLett.134.060401}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {060401}, shortjournal = {Phys. Rev. Lett.}, title = {Floquet expansion by counting pump photons}, volume = {134}, year = {2025}, }
• (2025). Quantumlike product states constructed from classical networks. PRL, 134(6), 060202. (www)

  @article{ , abstract = {Can complex classical systems be designed to exhibit superpositions of tensor products of basis states, thereby mimicking quantum states? We exhibit a one-to-one map between the product basis of quantum states comprising an arbitrary number of qubits and the eigenstates of a construction comprising classical oscillator networks. Specifically, we prove the existence of this map based on Cartesian products of graphs, where the graphs depict the layout of oscillator networks. We show how quantumlike gates can act on the classical networks to allow quantumlike operations in the state space.}, archive = {J_PRL}, author = {Gregory D. Scholes and Graziano Amati}, doi = {10.1103/PhysRevLett.134.060202}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {060202}, shortjournal = {Phys. Rev. Lett.}, title = {Quantumlike product states constructed from classical networks}, volume = {134}, year = {2025}, }
• (2025). Multipath and multiparticle tests of complex versus hypercomplex quantum theory. PRL, 134(6), 060201. (www)

  @article{ , abstract = {The axioms of quantum mechanics provide limited information regarding the structure of the Hilbert space, such as the underlying number system. The latter is generally regarded as complex, but generalizations of complex numbers, so-called hypercomplex numbers, cannot be ruled out in theory. Therefore, specialized experiments to test for hypercomplex quantum mechanics are needed. To date, experimental tests are limited to single-particle interference exploiting a closed phase relation in a three-path interferometer called the Peres test. The latter distinguishes complex quantum mechanics from quaternionic quantum mechanics. Here, we propose a general matrix formalism putting the Peres test on a solid mathematical ground. On this basis, we introduce multipath and multiparticle interference tests, which provide a direct probe for any dimension of the number system of quantum mechanics.}, archive = {J_PRL}, author = {Ece İpek Saruhan and Joachim von Zanthier and Marc-Oliver Pleinert}, doi = {10.1103/PhysRevLett.134.060201}, journal = {Physical Review Letters}, month = {2}, number = {6}, pages = {060201}, shortjournal = {Phys. Rev. Lett.}, title = {Multipath and multiparticle tests of complex versus hypercomplex quantum theory}, volume = {134}, year = {2025}, }
• (2025). Direct and retrograde wave propagation in unidirectionally coupled wilson-cowan oscillators. PRL, 134(5), 058401. (www)

  @article{ , abstract = {Some biological systems exhibit both direct and retrograde propagating signal waves despite unidirectional coupling. To explain this phenomenon, we study a chain of unidirectionally coupled Wilson-Cowan oscillators. Surprisingly, we find that changes in the homogeneous global input to the chain suffice to reverse the wave propagation direction. To obtain insights, we analyze the frequencies and bifurcations of the limit cycle solutions of the chain as a function of the global input. Specifically, we determine that the directionality of wave propagation is controlled by differences in the intrinsic frequencies of oscillators caused by the differential proximity of the oscillators to a homoclinic bifurcation.}, archive = {J_PRL}, author = {Guy Elisha and Richard Gast and Sourav Halder and Sara A. Solla and Peter J. Kahrilas and John E. Pandolfino and Neelesh A. Patankar}, doi = {10.1103/PhysRevLett.134.058401}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {058401}, shortjournal = {Phys. Rev. Lett.}, title = {Direct and retrograde wave propagation in unidirectionally coupled wilson-cowan oscillators}, volume = {134}, year = {2025}, }
• (2025). Surface furrowing instability in everting soft solids. PRL, 134(5), 058205. (www)

  @article{ , abstract = {We report a surface instability observed during the extrusion of extremely soft elastic solids in confined geometries. Because of their unique rheological properties, these soft solids can migrate through narrow gaps by continuously everting the bulk material. The extrusion front spontaneously buckles in the direction transverse to the flow, resulting in a furrowlike morphology that deepens over time. We characterize the distinct features of this instability using experiments and theory and contrast the results with known elastic surface instabilities. Our Letter may provide insights into various processes involving the extrusionlike deformations of soft solids, including biomaterials.}, archive = {J_PRL}, author = {Jonghyun Hwang and Mariana Altomare and Howard A. Stone}, doi = {10.1103/PhysRevLett.134.058205}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {058205}, shortjournal = {Phys. Rev. Lett.}, title = {Surface furrowing instability in everting soft solids}, volume = {134}, year = {2025}, }
• (2025). Accessing semiaddressable self-assembly with efficient structure enumeration. PRL, 134(5), 058204. (www)

  @article{ , abstract = {Modern experimental methods enable the creation of self-assembly building blocks with tunable interactions, but optimally exploiting this tunability for the self-assembly of desired structures remains an important challenge. Many studies of this inverse problem start with the so-called fully addressable limit, where every particle in a target structure is different. This leads to clear design principles that often result in high assembly yield, but it is not a scalable approach—at some point, one must grapple with “reusing” building blocks, which lowers the degree of addressability and may cause a multitude of off-target structures to form, complicating the design process. Here, we solve a key obstacle preventing robust inverse design in the “semiaddressable regime” by developing a highly efficient algorithm that enumerates all structures that can be formed from a given set of building blocks. By combining this with established partition-function-based yield calculations, we show that it is almost always possible to find economical semiaddressable designs where the entropic gain from reusing building blocks outweighs the presence of off-target structures and even increases the yield of the target. Thus, not only does our enumeration algorithm enable robust and scalable inverse design in the semiaddressable regime, our results demonstrate that it is possible to operate in this regime while maintaining the level of control often associated with full addressability.}, archive = {J_PRL}, author = {Maximilian C. Hübl and Carl P. Goodrich}, doi = {10.1103/PhysRevLett.134.058204}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {058204}, shortjournal = {Phys. Rev. Lett.}, title = {Accessing semiaddressable self-assembly with efficient structure enumeration}, volume = {134}, year = {2025}, }
• (2025). Universal scaling framework for controlling phase behavior in thickening and jamming suspensions. PRL, 134(5), 058203. (www)

  @article{ , abstract = {Recently, we proposed a universal scaling framework that shows shear thickening in dense suspensions is governed by the crossover between two critical points: one associated with frictionless isotropic jamming and a second corresponding to frictional shear jamming. Here, we show that orthogonal perturbations to the flows, an effective method for tuning shear thickening, can also be folded into this universal scaling framework. Specifically we show that the effect of adding orthogonal shear perturbations can be incorporated into the scaling variable via a multiplicative function, determined through our measurements, to achieve collapse of the entire thickening and dethickening dataset onto a single universal curve. We then show that this universal scaling framework can be used to control the phase behavior in thickening and jamming suspensions.}, archive = {J_PRL}, author = {Meera Ramaswamy and Itay Griniasty and James P. Sethna and Bulbul Chakraborty and Itai Cohen}, doi = {10.1103/PhysRevLett.134.058203}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {058203}, shortjournal = {Phys. Rev. Lett.}, title = {Universal scaling framework for controlling phase behavior in thickening and jamming suspensions}, volume = {134}, year = {2025}, }
• (2025). Statistical mechanics approach to DNA-driven droplet deformation and adhesion. PRL, 134(5), 058202. (www)

  @article{ , abstract = {Adhesion of soft particles with mobile linkers is of importance in colloidal self-assembly, the binding of vesicles, and tissue organization in biology. Here we derive and experimentally test an equilibrium theory that captures the adhesion of DNA-coated emulsion droplets. Notably, we identify a transition from spherical to deformed droplet binding at a characteristic DNA coverage that depends on molecular properties and surface tension. Fitting the data reveals a weak effective binding strength of owing to entropic costs of confinement, crowding, and stretching. Our results pave the path to materials design informed by the choice of molecular-scale parameters.}, archive = {J_PRL}, author = {Nicolas Judd and Angus McMullen and Sascha Hilgenfeldt and Jasna Brujic}, doi = {10.1103/PhysRevLett.134.058202}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {058202}, shortjournal = {Phys. Rev. Lett.}, title = {Statistical mechanics approach to DNA-driven droplet deformation and adhesion}, volume = {134}, year = {2025}, }
• (2025). Emergent metric-like states of active particles with metric-free polar alignment. PRL, 134(5), 058201. (www)

  @article{ , abstract = {We study a model of self-propelled particles interacting with their k nearest neighbors through polar alignment. By exploring its phase space as a function of two nondimensional parameters (alignment strength g and Péclet number Pe), we identify two distinct order-disorder transitions. One occurs at a low critical g value independent of Pe, has no significant density-order coupling, and is consistent with the transition previously predicted by the mean-field approach. Up to the system sizes studied, it appears continuous. The other is discontinuous, depends on a combined control parameter involving Pe and g that controls the alignment strength, and results from the formation of small, dense, highly persistent clusters of particles that follow metric-like dynamics. These dense clusters form at a critical value of the combined control parameter Pe / g α , with α ≈ 1.5 , which appears to be valid for different alignment-based models. Our study shows that models of active particles with metric-free interactions can produce characteristic length scales and self-organize into metric-like collective states that undergo metric-like transitions.}, archive = {J_PRL}, author = {Yinong Zhao and Cristián Huepe and Pawel Romanczuk}, doi = {10.1103/PhysRevLett.134.058201}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {058201}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent metric-like states of active particles with metric-free polar alignment}, volume = {134}, year = {2025}, }
• (2025). Networks with many structural scales: A renormalization group perspective. PRL, 134(5), 057401. (www)

  @article{ , abstract = {Scale invariance profoundly influences the dynamics and structure of complex systems, spanning from critical phenomena to network architecture. Here, we propose a precise definition of scale-invariant networks by leveraging the concept of a constant entropy-loss rate across scales in a renormalization-group coarse-graining setting. This framework enables us to differentiate between scale-free and scale-invariant networks, revealing distinct characteristics within each class. Furthermore, we offer a comprehensive inventory of genuinely scale-invariant networks, both natural and artificially constructed, demonstrating, e.g., that the human connectome exhibits notable features of scale invariance. Our findings open new avenues for exploring the scale-invariant structural properties crucial in biological and sociotechnological systems.}, archive = {J_PRL}, author = {Anna Poggialini and Pablo Villegas and Miguel A. Muñoz and Andrea Gabrielli}, doi = {10.1103/PhysRevLett.134.057401}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {057401}, shortjournal = {Phys. Rev. Lett.}, title = {Networks with many structural scales: A renormalization group perspective}, volume = {134}, year = {2025}, }
• (2025). Tattered membranes and constrained magnets. PRL, 134(5), 057101. (www)

  @article{ , abstract = {We formulate a generalized -dimensional field theory, parametrized by an tensor field with an energetic longitudinal constraint, describing a new class of fluctuating “tattered” membranes, exhibiting a nonzero density of topological connectivity defects—slits, cracks, and faults at an effective medium level. For infinite-coupling constraint, the model reproduces the elastic membrane, with its rich anomalous elasticity realized by, e.g., graphene. Two additional fixed points emerge within the critical manifold: (i) globally attractive, “isotropic” , and (ii) “transverse,” which in is the exact “dual” of the elastic membrane. Their properties are obtained in general , from the renormalization group and the self-consistent screening analyses. They correspond to critical points of an interesting class of constrained spin models.}, archive = {J_PRL}, author = {Pierre Le Doussal and Leo Radzihovsky}, doi = {10.1103/PhysRevLett.134.057101}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {057101}, shortjournal = {Phys. Rev. Lett.}, title = {Tattered membranes and constrained magnets}, volume = {134}, year = {2025}, }
• (2025). Solvated electrons in polar liquids as ϵ-near-zero materials tunable in the terahertz frequency range. PRL, 134(5), 056901. (www)

  @article{ , abstract = {Electrons in polar liquids give rise to a polaron resonance at a terahertz (THz) frequency ν 0 depending on electron concentration. The impact of this resonance on light propagation is studied in experiments, where a femtosecond pump pulse generates electrons via multiphoton ionization and a THz probe pulse propagated through the excited sample is detected in a phase-resolved way. We observe a behavior characteristic for ϵ -near-zero materials with strongly modified phase and group velocities around ν 0 , and a broadening of the THz pulse envelope below ν 0 . Calculations based on a local-field approach reproduce the ϵ -near-zero behavior.}, archive = {J_PRL}, author = {Matthias Runge and Michael Woerner and Denys I. Bondar and Thomas Elsaesser}, doi = {10.1103/PhysRevLett.134.056901}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056901}, shortjournal = {Phys. Rev. Lett.}, title = {Solvated electrons in polar liquids as ϵ-near-zero materials tunable in the terahertz frequency range}, volume = {134}, year = {2025}, }
• (2025). Origin of interstitial doping induced coercive field reduction in ferroelectric hafnia. PRL, 134(5), 056802. (www)

  @article{ , abstract = {Hafnia-based ferroelectrics hold promise for nonvolatile ferroelectric memory devices. However, the high coercive field required for polarization switching remains a prime obstacle to their practical applications. A notable reduction in coercive field has been achieved in ferroelectric films with interstitial Hf(Zr) dopants [ Science 381 , 558 (2023) ], suggesting a less-explored strategy for coercive field optimization. Supported by density functional theory calculations, we demonstrate the phase, with a moderate concentration of interstitial Hf dopants, serves as a minimal model to explain the experimental observations, rather than the originally assumed rhombohedral phase. Large-scale deep potential molecular dynamics simulations suggest that interstitial defects promote the polarization reversal by facilitating -like mobile 180° domain walls. A simple prepoling treatment could reduce the switching field to less than and enable switching on a subnanosecond timescale. High-throughput calculations reveal a negative correlation between the switching barrier and dopant size and identify a few promising interstitial dopants for coercive field reduction.}, archive = {J_PRL}, author = {Tianyuan Zhu and Liyang Ma and Xu Duan and Shiqing Deng and Shi Liu}, doi = {10.1103/PhysRevLett.134.056802}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056802}, shortjournal = {Phys. Rev. Lett.}, title = {Origin of interstitial doping induced coercive field reduction in ferroelectric hafnia}, volume = {134}, year = {2025}, }
• (2025). Dynamics of thermally driven domain transformation in ferroelectric thin films. PRL, 134(5), 056801. (www)

  @article{ , abstract = {An important feature in ultrathin ferroelectric films is the spontaneous formation of nanoscale polarization domain patterns. Epitaxial strain can greatly increase the ferroelectric transition temperature such that films can be in the ferroelectric state during growth. On the other hand, depolarization fields compete with ferroelectricity in ultrathin films, and, consequently, the optimal domain configuration during growth is a moving target. Under these conditions it is readily possible for a grown film to be in a nonequilibrium domain configuration. As the energy landscape in the system is quite complex, the relaxation dynamics by which a system can evolve towards the true equilibrium configuration are also quite interesting. To capture the details of this process we used Bragg-geometry x-ray photon correlation spectroscopy (XPCS), in which x-ray scattering speckle patterns contain the information from the domain arrangements inside the film. With modest heating ( ∼ 15 0 ° C ) domain relaxation from T (tetragonal) to M C (monoclinic) was observed in BaTiO 3 films grown on ultrathin ferroelectric PbTiO 3 layers. Two-time correlation analysis reveals fascinating details associated with sticking points and reversals in the process.}, archive = {J_PRL}, author = {Rui Liu and Anna Gura and Theodore Sauyet and Yugang Zhang and Lutz Wiegart and Andrei Fluerasu and Matthew Dawber}, doi = {10.1103/PhysRevLett.134.056801}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056801}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamics of thermally driven domain transformation in ferroelectric thin films}, volume = {134}, year = {2025}, }
• (2025). Nonresonant electric quantum control of individual on-surface spins. PRL, 134(5), 056703. (www)

  @article{ , abstract = {Quantum control techniques play an important role in manipulating and harnessing the properties of different quantum systems, including isolated atoms. Here, we propose to achieve quantum control over a single on-surface atomic spin using Landau-Zener-Stückelberg-Majorana (LZSM) interferometry implemented with scanning tunneling microscopy (STM). Specifically, we model how the application of time-dependent, nonresonant ac electric fields across the STM tip-surface gap makes it possible to achieve precise quantum state manipulation in an isolated ion on a surface. We propose a protocol to combine Landau-Zener tunneling with LZSM interferometry that permits one to measure the quantum spin tunneling of an individual ion. The proposed experiments can be implemented with ESR-STM instrumentation, opening a new venue in the research of on-surface single spin control.}, archive = {J_PRL}, author = {S. A. Rodríguez and S. S. Gómez and J. Fernández-Rossier and A. Ferrón}, doi = {10.1103/PhysRevLett.134.056703}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056703}, shortjournal = {Phys. Rev. Lett.}, title = {Nonresonant electric quantum control of individual on-surface spins}, volume = {134}, year = {2025}, }
• (2025). Current-induced sliding motion in a helimagnet MnAu2. PRL, 134(5), 056702. (www)

  @article{ , abstract = {We found signatures of current-induced sliding motion in helimagnetic thin films. An abrupt change in differential resistivity occurred at a threshold bias current in the helimagnetic state, whereas it was absent in the induced ferromagnetic state. Broadband voltage noise also emerged above the threshold current in the helimagnetic state. Based on the similarity to canonical charge and spin density wave systems, we ascribed the origin of these phenomena to the sliding motion of the helimagnetic structure.}, archive = {J_PRL}, author = {Yuta Kimoto and Hidetoshi Masuda and Takeshi Seki and Yoichi Nii and Jun-ichiro Ohe and Yusuke Nambu and Yoshinori Onose}, doi = {10.1103/PhysRevLett.134.056702}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056702}, shortjournal = {Phys. Rev. Lett.}, title = {Current-induced sliding motion in a helimagnet MnAu2}, volume = {134}, year = {2025}, }
• (2025). Observation of coherent gapless magnons in an antiferromagnet. PRL, 134(5), 056701. (www)

  @article{ , abstract = {Antiferromagnetic magnons possess high speed and are immune to external disturbance, making them promising for future magnonic circuits. In this Letter, we report the observation of gapless magnons in an easy-axis antiferromagnet 𝛼 − F e 2 ⁢ O 3 at low temperatures. These antiferromagnetic magnons are detected at nearly zero frequency by all-electrical spin-wave spectroscopy and propagate along antiferromagnetic domain walls as revealed by our theoretical model and simulations. Moreover, we demonstrate high coherency of these gapless magnons by showing their strong coupling with microwave photons. Our results open the pathway for antiferromagnetic texture based magnonic devices operating at microwave frequencies.}, archive = {J_PRL}, author = {Jilei Chen and Zhejunyu Jin and Rundong Yuan and Hanchen Wang and Hao Jia and Weiwei Wei and Lutong Sheng and Jinlong Wang and Yuelin Zhang and Song Liu and Dapeng Yu and Jean-Philippe Ansermet and Peng Yan and Haiming Yu}, doi = {10.1103/PhysRevLett.134.056701}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056701}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of coherent gapless magnons in an antiferromagnet}, volume = {134}, year = {2025}, }
• (2025). Hidden zero modes and topology of multiband non-hermitian systems. PRL, 134(5), 056601. (www)

  @article{ , abstract = {In a finite one-dimensional non-Hermitian system, the number of zero modes does not necessarily reflect the topology of the system. This is known as the breakdown of the bulk-boundary correspondence and has led to misconceptions about the topological protection of edge modes in such systems. Here we show why this breakdown does occur and that it typically results in hidden zero modes, extremely long-lived zero energy excitations, which are only revealed when considering the singular value instead of the eigenvalue spectrum. We point out, furthermore, that in a finite multiband non-Hermitian system with Hamiltonian , one needs to consider also the reflected Hamiltonian , which is in general distinct from the adjoint , to properly relate the number of protected zeros to the winding number of .}, archive = {J_PRL}, author = {Kyle Monkman and Jesko Sirker}, doi = {10.1103/PhysRevLett.134.056601}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056601}, shortjournal = {Phys. Rev. Lett.}, title = {Hidden zero modes and topology of multiband non-hermitian systems}, volume = {134}, year = {2025}, }
• (2025). Transient dynamical phase diagram of the spin-boson model. PRL, 134(5), 056502. (www)

  @article{ , abstract = {We investigate the real-time dynamics of the sub-Ohmic spin-boson model across a broad range of coupling strengths, using the numerically exact inchworm quantum Monte Carlo algorithm. From short- and intermediate-time dynamics starting from an initially decoupled state, we extract signatures of the zero-temperature quantum phase transition between localized and delocalized states. We show that the dynamical phase diagram thus obtained differs from the equilibrium phase diagram in both the values of critical couplings and the associated values of the critical exponent. We also identify and quantitatively analyze two competing mechanisms for the crossover between coherent oscillations and incoherent decay. Deep in the sub-Ohmic regime, the crossover is driven by the damping of the oscillation amplitude, while closer to the Ohmic regime the oscillation frequency itself drops sharply to zero at large coupling.}, archive = {J_PRL}, author = {Olga Goulko and Hsing-Ta Chen and Moshe Goldstein and Guy Cohen}, doi = {10.1103/PhysRevLett.134.056502}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056502}, shortjournal = {Phys. Rev. Lett.}, title = {Transient dynamical phase diagram of the spin-boson model}, volume = {134}, year = {2025}, }
• (2025). Hall response in interacting bosonic and fermionic ladders. PRL, 134(5), 056501. (www)

  @article{ , abstract = {We use bosonization, retaining band curvature terms, to analyze the Hall response of interacting bosonic and fermionic two-leg ladders threaded by a flux. We derive an explicit expression of the Hall imbalance in a perturbative expansion in the band curvature, retaining fully the interactions. We show that the flux dependence of the Hall imbalance allows to distinguish the two phases (Meissner and vortex) that are present for a bosonic ladder. For small magnetic field we relate the Hall resistance, both for bosonic and fermionic ladders, to the density dependence of the charge stiffness of the system in absence of flux. Our expression unveils a universal interaction-independent behavior in the Galilean invariant case.}, archive = {J_PRL}, author = {R. Citro and T. Giamarchi and E. Orignac}, doi = {10.1103/PhysRevLett.134.056501}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056501}, shortjournal = {Phys. Rev. Lett.}, title = {Hall response in interacting bosonic and fermionic ladders}, volume = {134}, year = {2025}, }
• (2025). Intrinsic nonlinear spin hall effect and manipulation of perpendicular magnetization. PRL, 134(5), 056301. (www)

  @article{ , abstract = {We propose an intrinsic nonlinear spin Hall effect, which enables the generation of collinearly polarized spin current in a large class of nonmagnetic materials with the corresponding linear response being symmetry forbidden. This opens a new avenue for field-free switching of perpendicular magnetization, which is required for the next-generation information storage technology. We develop the microscopic theory of this effect and clarify its quantum origin in band geometric quantities which can be enhanced by topological nodal features. Combined with first-principles calculations, we predict pronounced effects at room temperature in topological metals and PdGa. Our work establishes a fundamental nonlinear response in spin transport and opens the door to exploring spintronic applications based on nonlinear spin Hall effect.}, archive = {J_PRL}, author = {Hui Wang and Huiying Liu and Xukun Feng and Jin Cao and Weikang Wu and Shen Lai and Weibo Gao and Cong Xiao and Shengyuan A. Yang}, doi = {10.1103/PhysRevLett.134.056301}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056301}, shortjournal = {Phys. Rev. Lett.}, title = {Intrinsic nonlinear spin hall effect and manipulation of perpendicular magnetization}, volume = {134}, year = {2025}, }
• (2025). Sliding ferroelectricity in a bulk misfit layer compound (PbS)1.11VS2. PRL, 134(5), 056202. (www)

  @article{ , abstract = {Twisted heterostructures of two-dimensional crystals can create a moiré landscape, thereby changing the properties of its parent crystals. Here, the alternated stacking of posttransition metal monochalcogenides and transition metal dichalcogenides in misfit layer compound crystals is used as a moiré generator. X-ray diffraction shows the presence of twins with a small twist angle between them. The surface electrical potential from the induced sliding ferroelectricity is seen by using scanning probe microscopy and electron microscopy with domain sizes up to tens of micrometers.}, archive = {J_PRL}, author = {Cinthia Antunes Corrêa and Jiří Volný and Kateřina Tetalová and Klára Uhlířová and Václav Petříček and Martin Vondráček and Jan Honolka and Tim Verhagen}, doi = {10.1103/PhysRevLett.134.056202}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056202}, shortjournal = {Phys. Rev. Lett.}, title = {Sliding ferroelectricity in a bulk misfit layer compound (PbS)1.11VS2}, volume = {134}, year = {2025}, }
• (2025). Augmentation of universal potentials for broad applications. PRL, 134(5), 056201. (www)

  @article{ , abstract = {Universal potentials open the door for DFT level calculations at a fraction of their cost. We find that for application to systems outside the scope of its training data, pretrained CHGNet [Deng et al. , Nat. Mach. Intell. 5 , 1031 (2023)] has the potential to succeed out of the box, but can also fail significantly in predicting the ground state configuration. We demonstrate that via fine-tuning or a Δ -learning approach it is possible to augment the overall performance of universal potentials for specific cluster and surface systems. We utilize this to investigate and explain experimentally observed defects in the Ag(111)-O surface reconstruction and explain the mechanics behind their formation.}, archive = {J_PRL}, author = {Joe Pitfield and Florian Brix and Zeyuan Tang and Andreas Møller Slavensky and Nikolaj Rønne and Mads-Peter Verner Christiansen and Bjørk Hammer}, doi = {10.1103/PhysRevLett.134.056201}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056201}, shortjournal = {Phys. Rev. Lett.}, title = {Augmentation of universal potentials for broad applications}, volume = {134}, year = {2025}, }
• (2025). Learning neural free-energy functionals with pair-correlation matching. PRL, 134(5), 056103. (www)

  @article{ , abstract = {The intrinsic Helmholtz free-energy functional, the centerpiece of classical density functional theory, is at best only known approximately for 3D systems. Here we introduce a method for learning a neural-network approximation of this functional by exclusively training on a dataset of radial distribution functions, circumventing the need to sample costly heterogeneous density profiles in a wide variety of external potentials. For a supercritical Lennard-Jones system with planar symmetry, we demonstrate that the learned neural free-energy functional accurately predicts inhomogeneous density profiles under various complex external potentials obtained from simulations.}, archive = {J_PRL}, author = {Jacobus Dijkman and Marjolein Dijkstra and René van Roij and Max Welling and Jan-Willem van de Meent and Bernd Ensing}, doi = {10.1103/PhysRevLett.134.056103}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056103}, shortjournal = {Phys. Rev. Lett.}, title = {Learning neural free-energy functionals with pair-correlation matching}, volume = {134}, year = {2025}, }
• (2025). Atomistic understanding of dislocation climb in nitride semiconductors: Role of asymmetric jogs. PRL, 134(5), 056102. (www)

  @article{ , abstract = {Effective control of dislocation climb is of fundamental interest and practical importance in tuning the mechanical and electronic properties of semiconductors. However, it remains a big challenge due to the lack of a clear understanding of its inherent mechanism, in particular, in the nitride semiconductors. In this Letter, the atomic-scale climb process of a single dislocation in GaN is observed for the first time, which undergoes an alternating five- and nine-atomic-ring transformation. Combined with first-principles calculations, we reveal that the jogs exhibiting asymmetric atomic configurations play an unexpected role in determining the different dislocation climb behaviors in GaN. Interestingly, tuning the Fermi-level position by electroactive dopants can selectively generate different species of jogs, which can consequently manipulate the dislocation climb behaviors and dislocation dissociation in a controllable way. Our findings not only highlight the significant role the asymmetric jogs play in the dislocation climb in nitrides, but also suggest a clear routine to control dislocation dynamics in semiconductors.}, archive = {J_PRL}, author = {Han Yang and Xiangru Han and Xuelin Yang and Yingming Song and Beile Chen and Zhenghao Chen and Guangxu Ju and Fujun Xu and Ning Tang and Tongjun Yu and Xinqiang Wang and Weikun Ge and Bing Huang and Bo Shen}, doi = {10.1103/PhysRevLett.134.056102}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056102}, shortjournal = {Phys. Rev. Lett.}, title = {Atomistic understanding of dislocation climb in nitride semiconductors: Role of asymmetric jogs}, volume = {134}, year = {2025}, }
• (2025). Effect of grain geometry on the stability of polycrystalline pt at the nanoscale. PRL, 134(5), 056101. (www)

  @article{ , abstract = {Kelvin polycrystals with geometrical packing of tetrakaidecahedra grains were regarded as the only possible stable polycrystalline structures in solids. By intensive plastic straining of Pt, we identified the existence of Kelvin polycrystals with 4 nm grains and Schwarz crystals of 2–3 nm in size connected by minimal-surface grain boundaries, both constrained by twins. We found Schwarz crystals remained stable up to 1923 K, nearly 94% of the melting point of Pt, well above the stability limit of the Kelvin polycrystals (1373 K). It means geometries of grains and their boundary networks play a crucial role in stabilizing polycrystalline face-centered-cubic metals at the nanoscale.}, archive = {J_PRL}, author = {Huangliu Fu and Xin Zhou and Zhipeng Gao and Zhaohui Jin and Xiuyan Li and K. Lu}, doi = {10.1103/PhysRevLett.134.056101}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056101}, shortjournal = {Phys. Rev. Lett.}, title = {Effect of grain geometry on the stability of polycrystalline pt at the nanoscale}, volume = {134}, year = {2025}, }
• (2025). Supersolidity of polariton condensates in photonic crystal waveguides. PRL, 134(5), 056002. (www)

  @article{ , abstract = {Condensation of exciton polaritons has been recently observed in gap-confined states of one-dimensional photonic crystal waveguides. Here we focus on the theoretical emergence of a second emission threshold in this platform, in addition to the one associated with condensation at zero momentum, due to the nonlinear polariton scattering from the condensate into finite momentum eigenmodes. The physics of this spatially modulated condensate is related to a spontaneous breaking of both phase and translational symmetries simultaneously, bearing similarities with the highly sought supersolid phase in Helium and ultracold atomic gases but with a novel mechanism typical of the driven-dissipative scenario. We then propose clear-cut and unequivocal experimental signatures that would allow to identify such non-equilibrium supersolidity of polariton condensates.}, archive = {J_PRL}, author = {Davide Nigro and Dimitrios Trypogeorgos and Antonio Gianfrate and Daniele Sanvitto and Iacopo Carusotto and Dario Gerace}, doi = {10.1103/PhysRevLett.134.056002}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056002}, shortjournal = {Phys. Rev. Lett.}, title = {Supersolidity of polariton condensates in photonic crystal waveguides}, volume = {134}, year = {2025}, }
• (2025). Revealing the orbital origins of exotic electronic states with ti substitution in kagome superconductor CsV3Sb5. PRL, 134(5), 056001. (www)

  @article{ , abstract = {The multiband kagome superconductor CsV 3 Sb 5 exhibits complex orbital textures on the Fermi surface, making the orbital origins of its cascade of correlated electronic states and superconductivity a major scientific puzzle. Chemical doping of the kagome plane can simultaneously tune the exotic states and the Fermi-surface orbital texture and thus offers a unique opportunity to correlate the given states with specific orbitals. In this Letter, by substituting V atoms with Ti in the kagome superconductor CsV 3 Sb 5 , we reveal the orbital origin of a cascade of its correlated electronic states through the orbital-resolved quasiparticle interference. We analyze the quasiparticle interference changes associated with different orbitals, aided by first-principles calculations. We have observed that the in-plane and out-of-plane vanadium 3 d orbitals cooperate to form unidirectional coherent states in pristine CsV 3 Sb 5 , whereas the out-of-plane component disappears with doping-induced suppression of charge density wave and global electronic nematicity. In addition, the Sb p z orbital plays an important role in both the pseudogap and superconducting states in CsV 3 Sb 5 . Our findings offer new insights into multiorbital physics in quantum materials that are generally manifested with intriguing correlations between atomic orbitals and symmetry-encoded correlated electronic states.}, archive = {J_PRL}, author = {Zihao Huang and Hui Chen and Hengxin Tan and Xianghe Han and Yuhan Ye and Bin Hu and Zhen Zhao and Chengmin Shen and Haitao Yang and Binghai Yan and Ziqiang Wang and Feng Liu and Hong-Jun Gao}, doi = {10.1103/PhysRevLett.134.056001}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {056001}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing the orbital origins of exotic electronic states with ti substitution in kagome superconductor CsV3Sb5}, volume = {134}, year = {2025}, }
• (2025). Continuum damping of topologically protected edge modes at the boundary of cold magnetized plasmas. PRL, 134(5), 055301. (www)

  @article{ , abstract = {The recent extension of topological ideas to continuous systems with broken time-reversal symmetry, such as magnetized plasmas, provides new insights into the nature of topologically protected surface plasma waves (TSPWs). We demonstrate a unique characteristic of TSPWs propagating above the electron cyclotron frequency: their collisionless damping via coupling to the continuum of resonant modes localized inside a smooth plasma-vacuum interface. We show that damped TSPWs retain their unidirectional nature and immunity against backscattering, and that these properties can be used to generate highly localized energy sinks using sheared magnetic field.}, archive = {J_PRL}, author = {Roopendra Singh Rajawat and G. Shvets and V. Khudik}, doi = {10.1103/PhysRevLett.134.055301}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {055301}, shortjournal = {Phys. Rev. Lett.}, title = {Continuum damping of topologically protected edge modes at the boundary of cold magnetized plasmas}, volume = {134}, year = {2025}, }
• (2025). Laboratory demonstration of collisionless blob formation via laser-produced plasma self-focusing. PRL, 134(5), 055101. (www)

  @article{ , abstract = {Strongly localized, propagating plasma density structures that are capable of crossing magnetic field lines are known as “blobs.” Here we demonstrate a novel mechanism for the formation and propagation of an ion gyroradius-scale blob-cavity structure at the interface between a super-Alfvénic laser-produced plasma (LPP) and an ambient magnetized plasma. The LPP self-focuses along the edge of the diamagnetic cavity which results in a dense, jetlike structure as compared to ballistic motion. This collimated flow couples momentum to the ambient plasma through a collisionless process known as Larmor coupling. The Larmor electric fields locally displace the ambient ions forming a blob above the LPP flow. In the region between a gyrating blob and collimated LPP flow, a secondary cavity of expelled magnetic field forms. These findings are supported by particle-in-cell simulations that replicate the blob formation mechanism and provide insight to similar processes in space, astrophysical, and laboratory settings characterized by ion kinetic scales.}, archive = {J_PRL}, author = {R. S. Dorst and A. Le and C. G. Constantin and D. J. Larson and J. J. Pilgram and S. Vincena and S. K. P. Tripathi and M. M. Cowee and D. Winske and D. B. Schaeffer and C. Niemann}, doi = {10.1103/PhysRevLett.134.055101}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {055101}, shortjournal = {Phys. Rev. Lett.}, title = {Laboratory demonstration of collisionless blob formation via laser-produced plasma self-focusing}, volume = {134}, year = {2025}, }
• (2025). Bounds on heavy axions with an X-ray free electron laser. PRL, 134(5), 055001. (www)

  @article{ , abstract = {We present new exclusion bounds obtained at the European X-Ray Free Electron Laser facility (EuXFEL) on axionlike particles in the mass range . Our experiment exploits the Primakoff effect via which photons can, in the presence of a strong external electric field, decay into axions, which then convert back into photons after passing through an opaque wall. While similar searches have been performed previously at a third-generation synchrotron [Yamaji et al. , Phys. Lett. B 782 , 523 (2018) ], our work demonstrates improved sensitivity, exploiting the higher brightness of x-rays at EuXFEL.}, archive = {J_PRL}, author = {Jack W. D. Halliday and Giacomo Marocco and Konstantin A. Beyer and Charles Heaton and Motoaki Nakatsutsumi and Thomas R. Preston and Charles D. Arrowsmith and Carsten Baehtz and Sebastian Goede and Oliver Humphries and Alejandro Laso Garcia and Richard Plackett and Pontus Svensson and Georgios Vacalis and Justin Wark and Daniel Wood and Ulf Zastrau and Robert Bingham and Ian Shipsey and Subir Sarkar and Gianluca Gregori}, doi = {10.1103/PhysRevLett.134.055001}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {055001}, shortjournal = {Phys. Rev. Lett.}, title = {Bounds on heavy axions with an X-ray free electron laser}, volume = {134}, year = {2025}, }
• (2025). Turbulent spectrum of 2D internal gravity waves. PRL, 134(5), 054101. (www)

  @article{ , abstract = {We find the turbulent energy spectrum of weakly interacting 2D internal gravity waves using the full, nonhydrostatic dispersion relation. This spectrum is an exact solution of a regularized kinetic equation, from which the zero-frequency shear modes have been excised by a careful limiting process. This is a new method in wave kinetic theory. The turbulent spectrum agrees with the 2D oceanic Garrett-Munk spectrum for frequencies large compared to the Coriolis frequency and vertical scales small compared to the depth of the ocean. We show that this turbulent spectrum is the unique power law solution to the steady kinetic equation with a nonzero radial flux. Our solution provides an interesting insight into a turbulent energy cascade in an anisotropic system—like isotropic turbulence it is self-similar in scale, but its angular part is peaked along the curve of vanishing frequency and is self-similar in frequency.}, archive = {J_PRL}, author = {Michal Shavit and Oliver Bühler and Jalal Shatah}, doi = {10.1103/PhysRevLett.134.054101}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {054101}, shortjournal = {Phys. Rev. Lett.}, title = {Turbulent spectrum of 2D internal gravity waves}, volume = {134}, year = {2025}, }
• (2025). Emergence of capillary waves in miscible coflowing fluids. PRL, 134(5), 054001. (www)

  @article{ , abstract = {We show that capillary waves can exist at the boundary between miscible coflowing fluids. We unveil that the interplay between transient interfacial stresses and confinement drives the progressive transition from the well-known inertial regime, characterized by a frequency independent wave number, to a capillary wave scaling, unexpected for miscible fluids. This allows us to measure the effective interfacial tension between miscible fluids and its rapid decay on timescales never probed so far, which we rationalize with a model going beyond square-gradient theories. Our work potentially opens a new avenue to measure transient interfacial tensions at the millisecond scale in a controlled manner.}, archive = {J_PRL}, author = {Alessandro Carbonaro and Giovanni Savorana and Luca Cipelletti and Rama Govindarajan and Domenico Truzzolillo}, doi = {10.1103/PhysRevLett.134.054001}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {054001}, shortjournal = {Phys. Rev. Lett.}, title = {Emergence of capillary waves in miscible coflowing fluids}, volume = {134}, year = {2025}, }
• (2025). Postselection-free cavity-enhanced narrow-band orbital angular momentum entangled photon source. PRL, 134(5), 053801. (www)

  @article{ , abstract = {Cavity-enhanced spontaneous parametric down-conversion (SPDC) provides a significant way to produce narrow-band photon pairs, which matches the bandwidth of photon for quantum memory. However, the output photon pairs from the cavity are not entangled, and postselection is required to create the entanglement so far, so the direct output of cavity-enhanced narrow-band entangled photon pairs is still an open challenge. Here, we propose a solution that realizes the first postselection-free cavity-enhanced narrow-band entangled photon pairs. The entanglement is achieved in degree of freedom of orbital angular momentum (OAM) by an OAM-conservation SPDC process in an actively and precisely controlled cavity supporting degenerate high-order OAM modes. The measured linewidth and fidelity are 13.8 MHz and 0.969(3), respectively, for the directly generated OAM entangled two photons. We deterministically transfer the OAM entanglement to polarization one with almost no loss and obtain polarization entangled two photons with a fidelity of 0.948(2). Moreover, we produce narrow-band OAM-polarization hyperentangled photon pairs with a fidelity of 0.850(2), which is realized by interfering the two photons on a polarizing beam splitter (PBS) and postselecting the events of one and only one photon on each PBS port. Novel cavity may find applications in cavity-based light-matter interaction. Our results provide an efficient and promising approach to create narrow-band entangled photon sources for memory-based long-distance quantum communication and network.}, archive = {J_PRL}, author = {Pei Wan (万佩 and Wen-Zheng Zhu (朱文正 and Yan-Chao Lou (娄严超 and Zi-Mo Cheng (程子默 and Zhi-Cheng Ren (任志成 and Han Zhang (张涵 and Xi-Lin Wang (汪喜林 and Hui-Tian Wang (王慧田}, doi = {10.1103/PhysRevLett.134.053801}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053801}, shortjournal = {Phys. Rev. Lett.}, title = {Postselection-free cavity-enhanced narrow-band orbital angular momentum entangled photon source}, volume = {134}, year = {2025}, }
• (2025). Suppression of motional dephasing using state mapping. PRL, 134(5), 053604. (www)

  @article{ , abstract = {Rydberg-mediated quantum optics is a useful route toward deterministic quantum information processing based on single photons and quantum networks but is bottlenecked by the fast motional dephasing of Rydberg atoms. Here, we propose and experimentally demonstrate suppressing the motional dephasing by creating an a priori unknown but correct phase to each Rydberg atom in an atomic ensemble. The phase created is exactly proportional to the unknown velocity of the thermal motion, resulting in a condition as if no thermal motion occurs to the Rydberg atom upon the retrieval of the signal photon. Our experiments, though hampered by the noise of lasers and the environment, demonstrate more than one order of magnitude enhancement of the coherence time. The feasibility of realizing long-lived storage of single photons in strongly interacting Rydberg media sheds new light on Rydberg-mediated quantum nonlinear optics.}, archive = {J_PRL}, author = {Yuechun Jiao and Changcheng Li and Xiao-Feng Shi and Jiabei Fan and Jingxu Bai and Suotang Jia and Jianming Zhao and C. Stuart Adams}, doi = {10.1103/PhysRevLett.134.053604}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053604}, shortjournal = {Phys. Rev. Lett.}, title = {Suppression of motional dephasing using state mapping}, volume = {134}, year = {2025}, }
• (2025). Autonomous feedback stabilization of a cavity-coupled spin oscillator. PRL, 134(5), 053603. (www)

  @article{ , abstract = {We report out-of-equilibrium stabilization of the collective spin of an atomic ensemble through autonomous feedback by a driven optical cavity. For a magnetic field applied at an angle to the cavity axis, dispersive coupling to the cavity provides sensitivity to a combination of the longitudinal and transverse spin. Coherent backaction by cavity light onto the atoms, conditioned by the cavity susceptibility, stabilizes the spin state at an arbitrary energy. The setpoint tracking and closed-loop gain spectrum of the feedback system are characterized and found to agree closely with analytic predictions.}, archive = {J_PRL}, author = {Julian Wolf and Olive H. Eilbott and Joshua A. Isaacs and Kevin P. Mours and Jonathan Kohler and Dan M. Stamper-Kurn}, doi = {10.1103/PhysRevLett.134.053603}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053603}, shortjournal = {Phys. Rev. Lett.}, title = {Autonomous feedback stabilization of a cavity-coupled spin oscillator}, volume = {134}, year = {2025}, }
• (2025). Efficient in situ generation of photon-memory entanglement in a nonlinear cavity. PRL, 134(5), 053602. (www)

  @article{ , abstract = {Parametrically driving an optical cavity that simultaneously couples to an atomic ensemble quantum memory enables in situ generation of multimode photon-memory entanglement. A high-rate bipartite photon-memory entanglement can be generated even after discarding one entangled optical mode. This protocol can be realized with existing technologies based on photonic resonators integrated with a rare-earth-ion doped quantum memory. The proposed scheme shows significant advantages in entanglement generation rates compared with prevailing quantum memory protocols and experiments, with theoretical ebit rates of tens of MHz without fine-tuned operating conditions. Such a photon-memory entanglement source offers a versatile resource for quantum networking and interconnect applications.}, archive = {J_PRL}, author = {Hoi-Kwan Lau and Hong Qiao and Aashish A. Clerk and Tian Zhong}, doi = {10.1103/PhysRevLett.134.053602}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053602}, shortjournal = {Phys. Rev. Lett.}, title = {Efficient in situ generation of photon-memory entanglement in a nonlinear cavity}, volume = {134}, year = {2025}, }
• (2025). Observation of photonic mobility edge phases. PRL, 134(5), 053601. (www)

  @article{ , abstract = {Inverse Anderson localizations in lower dimensions predict that, as the hopping rates increase, all localized eigenmodes transition to extended states. Here, through the implementation of a mosaic quasiperiodic photonic waveguide lattice, we experimentally demonstrate a distinctive scenario, where the intermediate-energy eigenmodes become extended, while the low- or high-energy eigenmodes remain localized, leading to the emergence of energy-dependent Anderson localization transitions and mobility edge phases. Our experiment is enabled by developing an adiabatic procedure to prepare the photonic lattice into the zero-energy, lower and upper middle-energy, and ground and highest excited eigenmodes and subsequently measuring their localization properties. Moreover, we also experimentally investigate nonequilibrium quench dynamics for photons and show that photonic Loschmidt echoes can identify the appearance of mobility edge phases. Our study thus opens new avenues for investigating energy-dependent photonic Anderson localizations and harnessing photons to explore intriguing nonequilibrium physics.}, archive = {J_PRL}, author = {Yi-Jun Chang and Jia-Hui Zhang and Yong-Heng Lu and Ying-Yue Yang and Feng Mei and Jie Ma and Suotang Jia and Xian-Min Jin}, doi = {10.1103/PhysRevLett.134.053601}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053601}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of photonic mobility edge phases}, volume = {134}, year = {2025}, }
• (2025). Optical superlattice for engineering hubbard couplings in quantum simulation. PRL, 134(5), 053402. (www)

  @article{ , abstract = {Quantum simulations of Hubbard models with ultracold atoms rely on the exceptional control of coherent motion provided by optical lattices. Here we demonstrate enhanced tunability using an optical superlattice in a fermionic quantum gas microscope, evidenced by long-lived coherent double-well oscillations, next-nearest-neighbor quantum walks in a staggered configuration, and correlated quantum walks of two particles initiated through a resonant pair-breaking mechanism. We furthermore demonstrate tunable spin couplings through local offsets and engineer a spin ladder with ferromagnetic and antiferromagnetic couplings along the rungs and legs, respectively. Our Letter underscores the high potential of optical superlattices for engineering, simulating, and detecting strongly correlated many-body quantum states, with direct applications ranging from the study of mixed-dimensional systems to fermionic quantum computing.}, archive = {J_PRL}, author = {Thomas Chalopin and Petar Bojović and Dominik Bourgund and Si Wang and Titus Franz and Immanuel Bloch and Timon Hilker}, doi = {10.1103/PhysRevLett.134.053402}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053402}, shortjournal = {Phys. Rev. Lett.}, title = {Optical superlattice for engineering hubbard couplings in quantum simulation}, volume = {134}, year = {2025}, }
• (2025). Purcell-enhanced generation of photonic bell states via the inelastic scattering off single atoms. PRL, 134(5), 053401. (www)

  @article{ , abstract = {Single atoms trapped in optical cavities exhibit immense potential as key nodes in future quantum information processing. They have already demonstrated significant advancement in various quantum technologies, particularly regarding the generation of nonclassical light. Here, we efficiently produce genuine photonic Bell states through the inelastic scattering process off single two-level intracavity atoms. An experimental violation of the Bell inequality, arising from the interference between the probability amplitudes of two photons, validates the intrinsic nature of energy-time entanglement. Coupling atoms with an optical cavity in the Purcell regime substantially enhances the two-photon scattering. This Bell state generation process does not require atomic spin control, thereby rendering it inherently immune to decoherence effects. This work advances the comprehension of resonance fluorescence and has the potential to broaden the landscape of quantum technologies and facilitate the application of photonic Bell states.}, archive = {J_PRL}, author = {Jian Wang and Xiao-Long Zhou and Ze-Min Shen and Dong-Yu Huang and Si-Jian He and Qi-Yang Huang and Yi-Jia Liu and Chuan-Feng Li and Guang-Can Guo}, doi = {10.1103/PhysRevLett.134.053401}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053401}, shortjournal = {Phys. Rev. Lett.}, title = {Purcell-enhanced generation of photonic bell states via the inelastic scattering off single atoms}, volume = {134}, year = {2025}, }
• (2025). Many-body adiabatic passage: Instability, chaos, and quantum classical correspondence. PRL, 134(5), 053201. (www)

  @article{ , abstract = {Adiabatic passage in systems of interacting bosons is substantially affected by interactions and interparticle entanglement. We consider stimulated raman-adiabatic-passage-like schemes in Bose-Hubbard chains that exhibit low-dimensional chaos (a three-site chain) and high-dimensional chaos (more than three sites). The dynamics that is generated by a transfer protocol exhibits striking classical and quantum chaos fingerprints that are manifested in the mean-field classical treatment, in the truncated Wigner semiclassical treatment, and in the full many-body quantum simulations.}, archive = {J_PRL}, author = {Anant Vijay Varma and Amichay Vardi and Doron Cohen}, doi = {10.1103/PhysRevLett.134.053201}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053201}, shortjournal = {Phys. Rev. Lett.}, title = {Many-body adiabatic passage: Instability, chaos, and quantum classical correspondence}, volume = {134}, year = {2025}, }
• (2025). Interaction-induced topological phase transition at finite temperature. PRL, 134(5), 053002. (www)

  @article{ , abstract = {We demonstrate the existence of topological phase transitions in interacting, symmetry-protected quantum matter at finite temperatures. Using a combined numerical and analytical approach, we study a one-dimensional Su-Schrieffer-Heeger model with added Hubbard interactions, where no thermodynamic phase transition occurs at finite temperatures. The transition is signalled by a quantized, nonlocal bulk topological order parameter. It is driven by defects, which are enabled by the combination of interaction and thermal activation, with no counterpart in the noninteracting limit. The defects localize topological zero modes, which, when sufficiently abundant, cause the order parameter to vanish. This phenomenon, interpreted via bulk-boundary correspondence, reflects the loss of a topological edge mode at a well-defined critical temperature in the thermodynamic limit. Unlike zero-temperature topological transitions, these finite-temperature transitions lack thermodynamic signatures but remain observable in controlled quantum systems, such as ultracold fermionic atoms in optical lattices.}, archive = {J_PRL}, author = {Ze-Min Huang and Sebastian Diehl}, doi = {10.1103/PhysRevLett.134.053002}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053002}, shortjournal = {Phys. Rev. Lett.}, title = {Interaction-induced topological phase transition at finite temperature}, volume = {134}, year = {2025}, }
• (2025). Dipolar droplets of strongly interacting molecules. PRL, 134(5), 053001. (www)

  @article{ , abstract = {We simulate a molecular Bose-Einstein condensate in the strongly dipolar regime, observing the existence of self-bound droplets, as well as their splitting into multiple droplets by confinement-induced frustration. Our quantum Monte Carlo approach goes beyond the limits of the established effective mean-field theories for dipolar quantum gases, revealing small droplets produced by strong dipolar interactions outside known stable regimes. The simulations include realistic molecular interactions and therefore have direct relevance for current and future experiments.}, archive = {J_PRL}, author = {Tim Langen and Jordi Boronat and Juan Sánchez-Baena and Raúl Bombín and Tijs Karman and Ferran Mazzanti}, doi = {10.1103/PhysRevLett.134.053001}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {053001}, shortjournal = {Phys. Rev. Lett.}, title = {Dipolar droplets of strongly interacting molecules}, volume = {134}, year = {2025}, }
• (2025). Effects of neutron-antineutron transitions in neutron stars. PRL, 134(5), 052701. (www)

  @article{ , abstract = {We analyze effects of neutron-antineutron transitions in neutron stars, specifically on (i) cooling, (ii) rotation rate, and (iii) for binary pulsars, the increase in the orbital period. We show that these effects are negligibly small.}, archive = {J_PRL}, author = {Itzhak Goldman and Rabindra N. Mohapatra and Shmuel Nussinov and Robert Shrock}, doi = {10.1103/PhysRevLett.134.052701}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {052701}, shortjournal = {Phys. Rev. Lett.}, title = {Effects of neutron-antineutron transitions in neutron stars}, volume = {134}, year = {2025}, }
• (2025). Enhanced isomer population via direct irradiation of solid-density targets using a compact laser-plasma accelerator. PRL, 134(5), 052504. (www)

  @article{ , abstract = {Excitation of long-lived states in bromine nuclei using a tabletop laser-plasma accelerator providing pulsed ( ) electron beams provided a sensitive probe of strength and level densities in the nuclear quasicontinuum and may indicate angular momentum coupling through electron-nuclear interactions. Solid-density active targets absorb real and virtual photons up to and deexcite through cascade into different states. A factor of enhancement of the isomeric ratio was observed following electron irradiation, as compared to bremsstrahlung. Additional angular momentum transfer could possibly occur through nuclear-plasma or electron-nuclear interactions enabled by the ultrashort electron beam. Further investigation of these mechanisms could have far-reaching impact including decreased storage of long-term nuclear waste and an improved understanding of heavy element formation in astrophysical settings.}, archive = {J_PRL}, author = {Robert E. Jacob and Speero M. Tannous and Lee A. Bernstein and Joshua Brown and Tobias Ostermayr and Qiang Chen and Dieter H G. Schneider and Carl B. Schroeder and Jeroen van Tilborg and Eric H. Esarey and Cameron G R. Geddes}, doi = {10.1103/PhysRevLett.134.052504}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {052504}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced isomer population via direct irradiation of solid-density targets using a compact laser-plasma accelerator}, volume = {134}, year = {2025}, }
• (2025). Refined topology of the n=20 island of inversion with high precision mass measurements of na31−33 and mg31−35. PRL, 134(5), 052503. (www)

  @article{ , abstract = {Mass measurements of and using the TITAN MR-TOF-MS at TRIUMF’s ISAC facility are presented, with the uncertainty of the mass reduced by over 2 orders of magnitude. The excellent performance of the MR-TOF-MS has also allowed the discovery of a millisecond isomer in . The precision obtained shows that the binding energy of the normally closed neutron shell reaches a minimum for but increases significantly for , hinting at the possibility of enhanced shell strength toward the unbound . We compare the results with new ab initio predictions that raise intriguing questions of nuclear structure beyond the dripline.}, archive = {J_PRL}, author = {E. M. Lykiardopoulou and C. Walls and J. Bergmann and M. Brodeur and C. Brown and J. Cardona and A. Czihaly and T. Dickel and T. Duguet and J.-P. Ebran and M. Frosini and Z. Hockenbery and J. D. Holt and A. Jacobs and S. Kakkar and B. Kootte and T. Miyagi and A. Mollaebrahimi and T. Murboeck and P. Navratil and T. Otsuka and W. R. Plaß and S. Paul and W. S. Porter and M. P. Reiter and A. Scalesi and C. Scheidenberger and V. Somà and N. Shimizu and Y. Wang and D. Lunney and J. Dilling and A. A. Kwiatkowski}, doi = {10.1103/PhysRevLett.134.052503}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {052503}, shortjournal = {Phys. Rev. Lett.}, title = {Refined topology of the n=20 island of inversion with high precision mass measurements of na31−33 and mg31−35}, volume = {134}, year = {2025}, }
• (2025). Revealing the nature of yrast states in neutron-rich polonium isotopes. PRL, 134(5), 052502. (www)

  @article{ , abstract = {Polonium isotopes having two protons above the shell closure at Z = 82 show a wide variety of low-lying, high-spin isomeric states across the whole chain. The structure of neutron-deficient isotopes up to Po 210 ( N = 126 ) is well established as they are easily produced through various methods. However, there is not much information available for the neutron-rich counterparts for which only selective techniques can be used for their production. We report on the first fast-timing measurements of yrast states up to the 8 + level in Po 214 , 216 , 218 isotopes produced in the β − decay of Bi 214 , 216 , 218 at ISOLDE, CERN. In particular, our new half-life value of 607(14) ps for the 8 1 + state in Po 214 is nearly 20 times shorter than the value available in the literature and comparable with the newly measured half-lives of 409(16) and 628(25) ps for the corresponding 8 1 + states in Po 216 , 218 , respectively. The measured B ( E 2 ; 8 1 + → 6 1 + ) transition probability values follow an increasing trend relative to isotope mass, reaching a maximum for Po 216 . The increase contradicts the previous claims of isomerism for the 8 + yrast states in neutron-rich Po 214 and beyond. Together with the other measured yrast transitions, the B ( E 2 ) values provide a crucial test of the different theoretical approaches describing the underlying configurations of the yrast band. The new experimental results are compared to shell-model calculations using the KHPE and H208 effective interactions and their pairing-modified versions, showing an increase in configuration mixing when moving toward the heavier isotopes.}, archive = {J_PRL}, author = {IDS Collaboration and R. Lică and A. N. Andreyev and H. Naïdja and A. Blazhev and P. Van Duppen and B. Andel and A. Algora and S. Antalic and J. Benito and G. Benzoni and T. Berry and M. J. G. Borge and C. Costache and J. G. Cubiss and H. De Witte and L. M. Fraile and H. O. U. Fynbo and P. T. Greenlees and L. J. Harkness-Brennan and M. Huyse and A. Illana and J. Jolie and D. S. Judson and J. Konki and I. Lazarus and M. Madurga and N. Marginean and R. Marginean and C. Mihai and R. E. Mihai and P. Mosat and J. R. Murias and E. Nacher and A. Negret and R. D. Page and A. Perea and V. Pucknell and P. Rahkila and K. Rezynkina and V. Sánchez-Tembleque and K. Schomacker and M. Stryjczyk and C. Sürder and O. Tengblad and V. Vedia and N. Warr}, doi = {10.1103/PhysRevLett.134.052502}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {052502}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing the nature of yrast states in neutron-rich polonium isotopes}, volume = {134}, year = {2025}, }
• (2025). Angular momentum resolved inelastic electron scattering for nuclear giant resonances. PRL, 134(5), 052501. (www)

  @article{ , abstract = {Giant resonances (GRs) provide crucial insights into nuclear physics and astrophysics. Exciting GRs using particles like electrons is effective, yet the angular momentum (AM) transfer of electrons, including both intrinsic spin and orbital degrees of freedom in inelastic scattering, has never been studied. Here, we investigate AM transfer in GRs excited by plane-wave and vortex electrons, developing a comprehensive AM-resolved inelastic electron scattering theory. We find that even plane-wave electrons can model-independently extract transition strengths of higher multipolarity by selecting specific AM states of scattered electrons. Additionally, relativistic vortex electrons with an orbital angular momentum of ± 1 can be efficiently generated. Vortex electrons can also be used to extract GR transition strength as in the plane-wave case, regardless of the position of the nucleus relative to the beam axis. Furthermore, relativistic vortex electrons with larger orbital angular momentum can be generated for on-axis nuclei due to AM conservation. Our method offers new perspectives for nuclear structure research and paves the way for generating vortex particles.}, archive = {J_PRL}, author = {Zhi-Wei Lu and Liang Guo and Mamutjan Ababekri and Jia-Lin Zhang and Xiu-Feng Weng and Yuanbin Wu and Yi-Fei Niu and Jian-Xing Li}, doi = {10.1103/PhysRevLett.134.052501}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {052501}, shortjournal = {Phys. Rev. Lett.}, title = {Angular momentum resolved inelastic electron scattering for nuclear giant resonances}, volume = {134}, year = {2025}, }
• (2025). Flavor hierarchy of jet energy correlators inside the quark-gluon plasma. PRL, 134(5), 052301. (www)

  @article{ , abstract = {Heavy flavor jets provide ideal tools to probe the mass effect on jet substructure in both vacuum and quark-gluon plasma. An energy-energy correlator (EEC) is an excellent jet substructure observable owning to its strong sensitivity to jet physics at different scales. We perform a complete realistic simulation on medium modification of heavy and light flavor jet EECs in heavy-ion collisions. A clear flavor hierarchy is observed for jet EECs in both vacuum and quark-gluon plasma due to the mass effect. The medium modification of inclusive jet EECs at different angular scales exhibits a very rich structure: suppression at intermediate angles, and enhancement at small and large angles, which can be well explained by the interplay of mass effect, energy loss, medium-induced radiation, and medium response. These unique features of jet EECs are shown to probe the physics of jet-medium interaction at different scales, and can be readily validated by upcoming experiments.}, archive = {J_PRL}, author = {Wen-Jing Xing and Shanshan Cao and Guang-You Qin and Xin-Nian Wang}, doi = {10.1103/PhysRevLett.134.052301}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {052301}, shortjournal = {Phys. Rev. Lett.}, title = {Flavor hierarchy of jet energy correlators inside the quark-gluon plasma}, volume = {134}, year = {2025}, }
• (2025). Monopole-fermion scattering and the solution to the Semiton–Unitarity puzzle. PRL, 134(5), 051602. (www)

  @article{ , abstract = {We study Polchinski’s “fermion-rotor system” as an accurate description of charged Weyl fermions scattering on a magnetic monopole core in the limit of zero gauge coupling. Traditionally it was thought such scattering could lead to fractional particle numbers (“semitons”). By direct calculations we show those semitonic processes are in fact free propagation, facilitated by composite fermion-rotor operators interpolating the “forbidden” states, effectively “recovering” both ingoing and outgoing states in every lowest partial wave. Nonsemitonic Callan-Rubakov processes are unchanged.}, archive = {J_PRL}, author = {Vazha Loladze and Takemichi Okui}, doi = {10.1103/PhysRevLett.134.051602}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051602}, shortjournal = {Phys. Rev. Lett.}, title = {Monopole-fermion scattering and the solution to the Semiton–Unitarity puzzle}, volume = {134}, year = {2025}, }
• (2025). All next-to-next-to-extremal one-loop correlators of AdS supergluons and supergravitons. PRL, 134(5), 051601. (www)

  @article{ , abstract = {We bootstrap all of the next-to-next-to-extremal one-loop four-point correlators of supergravitons and supergluons in using a differential representation, and obtain closed formulas that are valid in both position space and Mellin space simultaneously.}, archive = {J_PRL}, author = {Zhongjie Huang (黄中杰 and Bo Wang (王波 and Ellis Ye Yuan (袁野}, doi = {10.1103/PhysRevLett.134.051601}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051601}, shortjournal = {Phys. Rev. Lett.}, title = {All next-to-next-to-extremal one-loop correlators of AdS supergluons and supergravitons}, volume = {134}, year = {2025}, }
• (2025). Boosting supermassive black hole growth in the early universe by fuzzy dark matter solitons. PRL, 134(5), 051402. (www)

  @article{ , abstract = {Observations of massive supermassive black holes (SMBHs) in the early Universe challenge existing black hole formation models. We propose that soliton cores in fuzzy dark matter (FDM) offer a potential solution to this timing problem. Our FDM cosmological zoom-in simulations confirm that, for a particle mass m FDM ∼ 10 − 22 eV , solitons are well developed at redshift z ∼ 7 with masses of ∼ 10 9 M ⊙ , comparable to the observed SMBHs. We then demonstrate using hydrodynamic simulations that, compared to cold dark matter, these high- z massive FDM solitons with mass M s can provide additional gravitational potential to accrete gas and boost the Bondi accretion rate of a growing black hole seed with mass M BH by up to 2–4 orders of magnitude, in the regime of efficient cooling and negligible radiation pressure. This accretion boosting mechanism is effective for 10 − 22 ≲ m FDM ≲ 10 − 20 eV and potentially beyond as long as M s > M BH .}, archive = {J_PRL}, author = {H.-H. Sandy Chiu (邱懷萱 and Hsi-Yu Schive (薛熙于 and Hsiang-Yi Karen Yang (楊湘怡 and Hsinhao Huang (黃新豪 and Massimo Gaspari}, doi = {10.1103/PhysRevLett.134.051402}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051402}, shortjournal = {Phys. Rev. Lett.}, title = {Boosting supermassive black hole growth in the early universe by fuzzy dark matter solitons}, volume = {134}, year = {2025}, }
• (2025). Expanding the quantum-limited gravitational-wave detection horizon. PRL, 134(5), 051401. (www)

  @article{ , abstract = {We demonstrate the potential of new adaptive optical technology to expand the detection horizon of gravitational-wave observatories. Achieving greater quantum-noise-limited sensitivity to spacetime strain hinges on achieving higher circulating laser power, in excess of 1 MW, in conjunction with highly squeezed quantum states of light. The new technology will enable significantly higher levels of laser power and squeezing in gravitational-wave detectors, by providing high-precision, low-noise correction of limiting sources of thermal distortions directly to the core interferometer optics. In simulated projections for LIGO , assuming an input laser power of 125 W and an effective injected squeezing level of 9 dB entering the interferometer, an initial concept of this technology can reduce the noise floor of the detectors by up to 20% from 200 Hz to 5 kHz, corresponding to an increment of 4 Mpc in the sky-averaged detection range for binary neutron star mergers. This work lays the foundation for one of the key technology improvements essential to fully utilize the scientific potential of the existing 4-km LIGO facilities, to observe black hole merger events past a redshift of 5, and opens a realistic pathway towards a next-generation 40-km gravitational-wave observatory in the U.S., Cosmic Explorer.}, archive = {J_PRL}, author = {Liu Tao and Mohak Bhattacharya and Peter Carney and Luis Martin Gutierrez and Luke Johnson and Shane Levin and Cynthia Liang and Xuesi Ma and Michael Padilla and Tyler Rosauer and Aiden Wilkin and Jonathan W. Richardson}, doi = {10.1103/PhysRevLett.134.051401}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051401}, shortjournal = {Phys. Rev. Lett.}, title = {Expanding the quantum-limited gravitational-wave detection horizon}, volume = {134}, year = {2025}, }
• (2025). First result for dark matter search by WINERED. PRL, 134(5), 051004. (www)

  @article{ , abstract = {The identity of dark matter has been a mystery in astronomy, cosmology, and particle theory for about a century. We present the first dark matter search with a high-dispersion spectrograph by using WINERED at the 6.5 m Magellan Clay telescope to measure the photons from the dark matter decays. The dwarf spheroidal galaxies (dSphs) Leo V and Tucana II are observed by utilizing an object-sky-object nodding observation technique. Employing zero consistent flux data after the sky subtraction and performing Doppler shift analysis for further background subtraction, we have established one of the most stringent limits to date on dark matter lifetime in the mass range of 1.8–2.7 eV. The conservative bound is translated to the photon coupling, g ϕ γ γ for axionlike par ticles around g ϕ γ γ ≲ ( 2 – 3 ) × 10 − 11 GeV − 1 ( 10 − 10 GeV − 1 ) for the case that ultrafaint dSphs have the Navarro-Frenk-White (generalized Hernquist) dark matter profile.}, archive = {J_PRL}, author = {Wen Yin and Taiki Bessho and Yuji Ikeda and Hitomi Kobayashi and Daisuke Taniguchi and Hiroaki Sameshima and Noriyuki Matsunaga and Shogo Otsubo and Yuki Sarugaku and Tomomi Takeuchi and Haruki Kato and Satoshi Hamano and Hideyo Kawakita}, doi = {10.1103/PhysRevLett.134.051004}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051004}, shortjournal = {Phys. Rev. Lett.}, title = {First result for dark matter search by WINERED}, volume = {134}, year = {2025}, }
• (2025). Robust integration of fast flavor conversions in classical neutrino transport. PRL, 134(5), 051003. (www)

  @article{ , abstract = {The quantum kinetic evolution of neutrinos in dense environments, such as the core-collapse supernovae or the neutron star mergers, can result in fast flavor conversion (FFC), presenting a significant challenge to achieving robust astrophysical modeling of these systems. Recent works that directly simulate the quantum kinetic transport of neutrinos in localized domains have suggested that the asymptotic outcome of FFCs can be modeled by simple analytical prescriptions when coarse grained over a size much larger than the FFC length scale. In this Letter , by leveraging such a scale separation, we incorporate the analytical prescriptions into global simulations that solve the classical neutrino transport equation including collisions and advection under spherical symmetry. We demonstrate that taking this approach allows to obtain results that quantitatively agree with those directly from the corresponding global quantum kinetic simulations and precisely capture the collisional feedback effect for cases where the FFC happens inside the neutrinosphere. Notably, the effective scheme does not require resolving the FFC time and length scales, hence only adds negligible computational overhead to classical transport. Our work highlights that efficient and robust integration of FFCs in classical neutrino transport used in astrophysical simulation can be feasible.}, archive = {J_PRL}, author = {Zewei Xiong and Meng-Ru Wu and Manu George and Chun-Yu Lin}, doi = {10.1103/PhysRevLett.134.051003}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051003}, shortjournal = {Phys. Rev. Lett.}, title = {Robust integration of fast flavor conversions in classical neutrino transport}, volume = {134}, year = {2025}, }
• (2025). Antiprotons and elementary particles over a solar cycle: Results from the alpha magnetic spectrometer. PRL, 134(5), 051002. (www)

  @article{ , abstract = {We present results over an 11-year Solar cycle of cosmic antiprotons based on events in the rigidity range from 1.00 to 41.9 GV. The fluxes exhibit distinct properties. The magnitude of the flux temporal variation is significantly smaller than those of , and . A hysteresis between the fluxes and the fluxes is observed, whereas the and fluxes show a linear correlation. With a model-independent analysis, we found a universal relation between the shape of the rigidity spectrum and the magnitude of flux temporal variation over an 11-year Solar cycle for both positively and negatively charged particles. The simultaneous results on and , and provide unique information for understanding particle transport in the Solar System as a function of mass, charge, and spectral shape.}, archive = {J_PRL}, author = {AMS Collaboration and M. Aguilar and G. Ambrosi and H. Anderson and L. Arruda and N. Attig and C. Bagwell and F. Barao and M. Barbanera and L. Barrin and A. Bartoloni and R. Battiston and A. Bayyari and N. Belyaev and B. Bertucci and V. Bindi and K. Bollweg and J. Bolster and M. Borchiellini and B. Borgia and M. J. Boschini and M. Bourquin and C. Brugnoni and J. Burger and W. J. Burger and X. D. Cai and M. Capell and J. Casaus and G. Castellini and F. Cervelli and Y. H. Chang and G. M. Chen and G. R. Chen and H. Chen and H. S. Chen and Y. Chen and L. Cheng and H. Y. Chou and S. Chouridou and V. Choutko and C. H. Chung and C. Clark and G. Coignet and C. Consolandi and A. Contin and C. Corti and Z. Cui and K. Dadzie and F. D’Angelo and A. Dass and C. Delgado and S. Della Torre and M. B. Demirköz and L. Derome and S. Di Falco and V. Di Felice and C. Díaz and F. Dimiccoli and P. von Doetinchem and F. Dong and M. Duranti and A. Egorov and A. Eline and F. Faldi and D. Fehr and J. Feng and E. Fiandrini and P. Fisher and V. Formato and R. J. García-López and C. Gargiulo and H. Gast and M. Gervasi and F. Giovacchini and D. M. Gómez-Coral and J. Gong and D. Grandi and M. Graziani and S. Haino and K. C. Han and R. K. Hashmani and Z. H. He and B. Heber and F. Hernández-Nicolás and T. H. Hsieh and J. Y. Hu and B. W. Huang and M. Ionica and M. Incagli and Yi Jia and H. Jinchi and G. Karagöz and Th. Kirn and A. P. Klipfel and O. Kounina and A. Kounine and V. Koutsenko and D. Krasnopevtsev and A. Kuhlman and A. Kulemzin and G. La Vacca and E. Laudi and G. Laurenti and G. LaVecchia and I. Lazzizzera and H. T. Lee and S. C. Lee and H. L. Li and J. H. Li and J. Q. Li and M. Li and Q. Li and Q. Y. Li and S. Li and S. L. Li and Z. H. Li and M. J. Liang and P. Liao and C. H. Lin and T. Lippert and J. H. Liu and P. C. Liu and S. Q. Lu and Y. S. Lu and J. Z. Luo and Q. Luo and S. D. Luo and Xi Luo and C. Mañá and J. Marín and J. Marquardt and G. Martínez and N. Masi and D. Maurin and T. Medvedeva and A. Menchaca-Rocha and Q. Meng and V. V. Mikhailov and M. Molero and P. Mott and L. Mussolin and Y. Najafi Jozani and R. Nicolaidis and N. Nikonov and F. Nozzoli and J. Ocampo-Peleteiro and A. Oliva and M. Orcinha and F. Palmonari and M. Paniccia and A. Pashnin and M. Pauluzzi and D. Pelosi and S. Pensotti and P. Pietzcker and V. Plyaskin and S. Poluianov and D. Pridöhl and Z. Y. Qu and L. Quadrani and P. G. Rancoita and D. Rapin and A. Reina Conde and E. Robyn and I. Rodríguez-García and L. Romaneehsen and F. Rossi and A. Rozhkov and D. Rozza and R. Sagdeev and S. Schael and A. Schultz von Dratzig and G. Schwering and E. S. Seo and B. S. Shan and A. Shukla and T. Siedenburg and G. Silvestre and J. W. Song and X. J. Song and R. Sonnabend and L. Strigari and T. Su and Q. Sun and Z. T. Sun and L. Tabarroni and M. Tacconi and Z. C. Tang and J. Tian and Y. Tian and Samuel C. C. Ting and S. M. Ting and N. Tomassetti and J. Torsti and A. Ubaldi and T. Urban and I. Usoskin and V. Vagelli and R. Vainio and P. Väisänen and M. Valencia-Otero and E. Valente and E. Valtonen and M. Vázquez Acosta and M. Vecchi and M. Velasco and C. X. Wang and J. C. Wang and L. Wang and L. Q. Wang and N. H. Wang and Q. L. Wang and S. Wang and X. Wang and Z. M. Wang and J. Wei and Z. L. Weng and H. Wu and Y. Wu and Z. B. Wu and J. N. Xiao and R. Q. Xiong and X. Z. Xiong and W. Xu and Q. Yan and H. T. Yang and Y. Yang and H. Yi and Y. H. You and Y. M. Yu and Z. Q. Yu and C. Zhang and F. Z. Zhang and J. Zhang and J. H. Zhang and Z. Zhang and P. W. Zhao and C. Zheng and Z. M. Zheng and H. L. Zhuang and V. Zhukov and A. Zichichi and M. Zuberi and P. Zuccon}, doi = {10.1103/PhysRevLett.134.051002}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051002}, shortjournal = {Phys. Rev. Lett.}, title = {Antiprotons and elementary particles over a solar cycle: Results from the alpha magnetic spectrometer}, volume = {134}, year = {2025}, }
• (2025). Solar modulation of cosmic nuclei over a solar cycle: Results from the alpha magnetic spectrometer. PRL, 134(5), 051001. (www)

  @article{ , abstract = {We report the properties of precision time structures of cosmic nuclei He, Li, Be, B, C, N, and O fluxes over an 11-year solar cycle from May 2011 to November 2022 in the rigidity range from 1.92 to 60.3 GV. The nuclei fluxes show similar but not identical time variations with amplitudes decreasing with increasing rigidity. In particular, below 3.64 GV the Li, Be, and B fluxes, and below 2.15 GV the C, N, and O fluxes, are significantly less affected by solar modulation than the He flux. We observe that these differences in solar modulation are linearly correlated with the differences in the spectral indices of the cosmic nuclei fluxes. This shows, in a model-independent way, that solar modulation of galactic cosmic nuclei depends on their spectral shape. In addition, solar modulation differences due to nuclei velocity dependence on the mass-to-charge ratio ( A / Z ) are not observed.}, archive = {J_PRL}, author = {AMS Collaboration and M. Aguilar and B. Alpat and G. Ambrosi and H. Anderson and L. Arruda and N. Attig and C. Bagwell and F. Barao and M. Barbanera and L. Barrin and A. Bartoloni and R. Battiston and A. Bayyari and N. Belyaev and B. Bertucci and V. Bindi and K. Bollweg and J. Bolster and M. Borchiellini and B. Borgia and M. J. Boschini and M. Bourquin and C. Brugnoni and J. Burger and W. J. Burger and N. Burzillà and X. D. Cai and M. Capell and J. Casaus and G. Castellini and F. Cervelli and Y. H. Chang and G. M. Chen and G. R. Chen and H. Chen and H. S. Chen and Y. Chen and L. Cheng and H. Y. Chou and S. Chouridou and V. Choutko and C. H. Chung and C. Clark and G. Coignet and C. Consolandi and A. Contin and C. Corti and Z. Cui and K. Dadzie and F. D’Angelo and A. Dass and C. Delgado and S. Della Torre and M. B. Demirköz and L. Derome and S. Di Falco and V. Di Felice and C. Díaz and F. Dimiccoli and P. von Doetinchem and F. Dong and M. Duranti and A. Egorov and A. Eline and F. Faldi and D. Fehr and J. Feng and E. Fiandrini and P. Fisher and V. Formato and R. J. García-López and C. Gargiulo and H. Gast and M. Gervasi and F. Giovacchini and D. M. Gómez-Coral and J. Gong and D. Grandi and M. Graziani and S. Haino and K. C. Han and R. K. Hashmani and Z. H. He and B. Heber and F. Hernández-Nicolás and T. H. Hsieh and J. Y. Hu and B. W. Huang and M. Ionica and M. Incagli and Yi Jia and H. Jinchi and G. Karagöz and Th. Kirn and A. P. Klipfel and O. Kounina and A. Kounine and V. Koutsenko and D. Krasnopevtsev and A. Kuhlman and A. Kulemzin and G. La Vacca and E. Laudi and G. Laurenti and G. LaVecchia and I. Lazzizzera and H. T. Lee and S. C. Lee and H. L. Li and J. H. Li and J. Q. Li and M. Li and Q. Li and Q. Y. Li and S. Li and S. L. Li and Z. H. Li and M. J. Liang and P. Liao and C. H. Lin and T. Lippert and J. H. Liu and P. C. Liu and Z. Liu and S. Q. Lu and Y. S. Lu and J. Z. Luo and Q. Luo and S. D. Luo and Xi Luo and C. Mañá and J. Marín and J. Marquardt and G. Martínez and N. Masi and D. Maurin and T. Medvedeva and A. Menchaca-Rocha and Q. Meng and V. V. Mikhailov and M. Molero and P. Mott and L. Mussolin and Y. Najafi Jozani and R. Nicolaidis and N. Nikonov and F. Nozzoli and J. Ocampo-Peleteiro and A. Oliva and M. Orcinha and F. Palmonari and M. Paniccia and A. Pashnin and M. Pauluzzi and D. Pelosi and S. Pensotti and P. Pietzcker and V. Plyaskin and S. Poluianov and D. Pridöhl and Z. Y. Qu and L. Quadrani and P. G. Rancoita and D. Rapin and A. Reina Conde and E. Robyn and I. Rodríguez-García and L. Romaneehsen and F. Rossi and A. Rozhkov and D. Rozza and R. Sagdeev and S. Schael and A. Schultz von Dratzig and G. Schwering and E. S. Seo and B. S. Shan and A. Shukla and T. Siedenburg and A. Siemko and G. Silvestre and J. W. Song and X. J. Song and R. Sonnabend and L. Strigari and T. Su and Q. Sun and Z. T. Sun and L. Tabarroni and M. Tacconi and Z. C. Tang and J. Tian and Y. Tian and Samuel C. C. Ting and S. M. Ting and N. Tomassetti and J. Torsti and A. Ubaldi and T. Urban and I. Usoskin and V. Vagelli and R. Vainio and P. Väisänen and M. Valencia-Otero and E. Valente and E. Valtonen and M. Vázquez Acosta and M. Vecchi and M. Velasco and C. X. Wang and J. C. Wang and L. Wang and L. Q. Wang and N. H. Wang and Q. L. Wang and S. Wang and X. Wang and Z. M. Wang and J. Wei and Z. L. Weng and H. Wu and Y. Wu and Z. B. Wu and J. N. Xiao and R. Q. Xiong and X. Z. Xiong and W. Xu and Q. Yan and H. T. Yang and Y. Yang and H. Yi and Y. H. You and Y. M. Yu and Z. Q. Yu and C. Zhang and F. Z. Zhang and J. Zhang and J. H. Zhang and Z. Zhang and P. W. Zhao and C. Zheng and Z. M. Zheng and H. L. Zhuang and V. Zhukov and A. Zichichi and M. Zuberi and P. Zuccon}, doi = {10.1103/PhysRevLett.134.051001}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {051001}, shortjournal = {Phys. Rev. Lett.}, title = {Solar modulation of cosmic nuclei over a solar cycle: Results from the alpha magnetic spectrometer}, volume = {134}, year = {2025}, }
• (2025). Probing dynamics of a two-dimensional dipolar spin ensemble using single qubit sensor. PRL, 134(5), 050801. (www)

  @article{ , abstract = {Understanding the thermalization dynamics of quantum many-body systems at the microscopic level is among the central challenges of modern statistical physics. Here we experimentally investigate individual spin dynamics in a two-dimensional ensemble of electron spins on the surface of a diamond crystal. We use a near-surface nitrogen-vacancy center as a nanoscale magnetic sensor to probe correlation dynamics of individual spins in a dipolar interacting surface spin ensemble. We observe that the relaxation rate for each spin is significantly slower than the naïve expectation based on independently estimated dipolar interaction strengths with nearest neighbors and is strongly correlated with the timescale of the local magnetic field fluctuation. We show that this anomalously slow relaxation rate is due to the presence of strong dynamical disorder and present a quantitative explanation based on dynamic resonance counting. Finally, we use resonant spin-lock driving to control the effective strength of the local magnetic fields and reveal the role of the dynamical disorder in different regimes. Our work paves the way towards microscopic study and control of quantum thermalization in strongly interacting disordered spin ensembles.}, archive = {J_PRL}, author = {Kristine Rezai and Soonwon Choi and Mikhail D. Lukin and Alexander O. Sushkov}, doi = {10.1103/PhysRevLett.134.050801}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050801}, shortjournal = {Phys. Rev. Lett.}, title = {Probing dynamics of a two-dimensional dipolar spin ensemble using single qubit sensor}, volume = {134}, year = {2025}, }
• (2025). Accelerating dissipative state preparation with adaptive open quantum dynamics. PRL, 134(5), 050603. (www)

  @article{ , abstract = {A wide variety of dissipative state preparation schemes suffer from a basic time-entanglement tradeoff: the more entangled the steady state, the slower the relaxation to the steady state. Here, we show how a minimal kind of adaptive dynamics can be used to completely circumvent this tradeoff, and allow the dissipative stabilization of maximally entangled states with a finite timescale. Our approach takes inspiration from simple fermionic stabilization schemes, which surprisingly are immune to entanglement-induced slowdown. We describe schemes for accelerated stabilization of many-body entangled qubit states (including spin squeezed states), both in the form of discretized Floquet circuits, as well as continuous time dissipative dynamics. Our ideas are compatible with a number of experimental platforms.}, archive = {J_PRL}, author = {Andrew Pocklington and Aashish A. Clerk}, doi = {10.1103/PhysRevLett.134.050603}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050603}, shortjournal = {Phys. Rev. Lett.}, title = {Accelerating dissipative state preparation with adaptive open quantum dynamics}, volume = {134}, year = {2025}, }
• (2025). Implementing arbitrary ising models with a trapped-ion quantum processor. PRL, 134(5), 050602. (www)

  @article{ , abstract = {A promising paradigm of quantum computing for achieving practical quantum advantages is quantum annealing or quantum approximate optimization algorithm, where the classical problems are encoded in Ising interactions. However, it is challenging to build a quantum system that can efficiently map any structured problems. Here, we present a trapped-ion quantum processor that can efficient encode arbitrary Ising models with all-to-all connectivity for up to four spins. We implement the spin-spin interactions by using the coupling of trapped ions to multiple collective motional modes and realize the programmability through phase modulation of the Raman laser beams that are individually addressed on ions. As an example, we realize several Ising models with different interaction connectivities, where the interactions can be ferromagnetic or antiferromagnetic. We confirm the programmed interaction geometry by observing the ground states of the corresponding models through quantum state tomography. Our experimental demonstrations serve as an important basis for realizing practical quantum advantages with trapped ions.}, archive = {J_PRL}, author = {Yao Lu and Wentao Chen and Shuaining Zhang and Kuan Zhang and Jialiang Zhang and Jing-Ning Zhang and Kihwan Kim}, doi = {10.1103/PhysRevLett.134.050602}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050602}, shortjournal = {Phys. Rev. Lett.}, title = {Implementing arbitrary ising models with a trapped-ion quantum processor}, volume = {134}, year = {2025}, }
• (2025). Qudit dynamical decoupling on a superconducting quantum processor. PRL, 134(5), 050601. (www)

  @article{ , abstract = {Multilevel qudit systems are increasingly being explored as alternatives to traditional qubit systems due to their denser information storage and processing potential. However, qudits are more susceptible to decoherence than qubits due to increased loss channels, noise sensitivity, and crosstalk. To address these challenges, we develop protocols for dynamical decoupling (DD) of qudit systems based on the Heisenberg-Weyl group. We implement and experimentally verify these DD protocols on a superconducting transmon processor that supports qudit operation based on qutrits ( ) and ququarts ( ). Specifically, we demonstrate single-qudit DD sequences to decouple qutrits and ququarts from system-bath-induced decoherence. We also introduce two-qudit DD sequences designed to suppress the detrimental cross-Kerr couplings between coupled qudits. This allows us to demonstrate a significant improvement in the fidelity of time-evolved qutrit Bell states. Our results highlight the utility of leveraging DD to enable scalable qudit-based quantum computing.}, archive = {J_PRL}, author = {Vinay Tripathi and Noah Goss and Arian Vezvaee and Long B. Nguyen and Irfan Siddiqi and Daniel A. Lidar}, doi = {10.1103/PhysRevLett.134.050601}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050601}, shortjournal = {Phys. Rev. Lett.}, title = {Qudit dynamical decoupling on a superconducting quantum processor}, volume = {134}, year = {2025}, }
• (2025). Quantum origin of limit cycles, fixed points, and critical slowing down. PRL, 134(5), 050407. (www)

  @article{ , abstract = {Among the most iconic features of classical dissipative dynamics are persistent limit-cycle oscillations and critical slowing down at the onset of such oscillations, where the system relaxes purely algebraically in time. On the other hand, quantum systems subject to generic Markovian dissipation decohere exponentially in time, approaching a unique steady state. Here we show how coherent limit-cycle oscillations and algebraic decay can emerge in a quantum system governed by a Markovian master equation as one approaches the classical limit, illustrating general mechanisms using a single-spin model and a two-site lossy Bose-Hubbard model. In particular, we demonstrate that the fingerprint of a limit cycle is a slow-decaying branch with vanishing decoherence rates in the Liouville spectrum, while a power-law decay is realized by a spectral collapse at the bifurcation point. We also show how these are distinct from the case of a classical fixed point, for which the quantum spectrum is gapped and can be generated from the linearized classical dynamics.}, archive = {J_PRL}, author = {Shovan Dutta and Shu Zhang and Masudul Haque}, doi = {10.1103/PhysRevLett.134.050407}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050407}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum origin of limit cycles, fixed points, and critical slowing down}, volume = {134}, year = {2025}, }
• (2025). Quantum detailed fluctuation theorem in curved spacetimes: The observer dependent nature of entropy production. PRL, 134(5), 050406. (www)

  @article{ , abstract = {The interplay between thermodynamics, general relativity, and quantum mechanics has long intrigued researchers. Recently, important advances have been obtained in thermodynamics, mainly regarding its application to the quantum domain through fluctuation theorems. In this Letter, we apply Fermi normal coordinates to report a fully general relativistic detailed quantum fluctuation theorem based on the two point measurement scheme. We demonstrate how the spacetime curvature can produce entropy in a localized quantum system moving in a general spacetime. The example of a quantum harmonic oscillator living in an expanding universe is presented. This result implies that entropy production is strongly observer dependent and deeply connects the arrow of time with the causal structure of the spacetime.}, archive = {J_PRL}, author = {Marcos L. W. Basso and Jonas Maziero and Lucas C. Céleri}, doi = {10.1103/PhysRevLett.134.050406}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050406}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum detailed fluctuation theorem in curved spacetimes: The observer dependent nature of entropy production}, volume = {134}, year = {2025}, }
• (2025). Fock-space delocalization and the emergence of the porter-thomas distribution from dual-unitary dynamics. PRL, 134(5), 050405. (www)

  @article{ , abstract = {The chaotic dynamics of quantum many-body systems are expected to quickly randomize any structured initial state, delocalizing it in the Fock space. In this Letter, we study the spreading of an initial product state in Hilbert space under dual-unitary dynamics, captured by the inverse participation ratios and the distribution of overlaps (bit-string probabilities). We consider the self-dual kicked Ising model, a minimal model of many-body quantum chaos that can be seen as either a periodically driven Floquet model or a dual-unitary quantum circuit. Both analytically and numerically, we show that the inverse participation ratios rapidly approach their ergodic values, corresponding to those of Haar random states, and establish the emergence of the Porter-Thomas distribution for the overlap distribution. Importantly, this convergence happens exponentially fast in time, with a timescale that is independent of system size. We inspect the effect of local perturbations that break dual unitarity and show a slowdown of the spreading in Fock space, indicating that dual-unitary circuits are maximally efficient at preparing random states. Our Letter establishes bridges between the dynamics of many-body systems and random matrix theory through the time evolution of structured initial states and finds natural applications in demonstrating a quantum advantage in random sampling and in benchmarking quantum devices.}, archive = {J_PRL}, author = {Pieter W. Claeys and Giuseppe De Tomasi}, doi = {10.1103/PhysRevLett.134.050405}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050405}, shortjournal = {Phys. Rev. Lett.}, title = {Fock-space delocalization and the emergence of the porter-thomas distribution from dual-unitary dynamics}, volume = {134}, year = {2025}, }
• (2025). Dynamical landauer principle: Quantifying information transmission by thermodynamics. PRL, 134(5), 050404. (www)

  @article{ , abstract = {Energy transfer and information transmission are two fundamental aspects of nature. They are seemingly unrelated, while recent findings suggest that a deep connection between them is to be discovered. This amounts to asking: Can we phrase the processes of transmitting classical bits equivalently as specific energy-transmitting tasks, thereby uncovering foundational links between them? We answer this question positively by showing that, for a broad class of classical communication tasks, a quantum dynamics’ ability to transmit bits of classical information is equivalent to its ability to transmit units of energy in a thermodynamic task. This finding not only provides an analytical correspondence between information transmission and energy extraction tasks, but also quantifies classical communication by thermodynamics. Furthermore, our findings uncover the dynamical version of Landauer’s principle, showing the strong link between transmitting information and energy. In the asymptotic regime, our results further provide thermodynamic meanings for the well-known Holevo-Schumacher-Westmoreland theorem in quantum communication theory.}, archive = {J_PRL}, author = {Chung-Yun Hsieh}, doi = {10.1103/PhysRevLett.134.050404}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050404}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical landauer principle: Quantifying information transmission by thermodynamics}, volume = {134}, year = {2025}, }
• (2025). Volume-entangled exact scar states in the PXP and related models in any dimension. PRL, 134(5), 050403. (www)

  @article{ , abstract = {In this Letter, we report first exact volume-entangled Einstein-Podolsky-Rosen–type scar states hosted by PXP and related Hamiltonians corresponding to various geometric configurations of Rydberg-blockaded atom systems, including the most extensively studied ones such as the chain with periodic boundary conditions (PBCs) and square lattice. We start by introducing a new zero-energy eigenstate of the PBC chain and proceed by generalizing it to a wide variety of geometries and Hamiltonians. We point out the potential experimental relevance of our states by providing a protocol for their preparation on near-term Rydberg quantum devices, which relies only on strictly local measurements and evolution under native Hamiltonians. We also demonstrate the utility of these states for the study of quantum dynamics by describing a protocol for measuring infinite-temperature out-of-time-order correlator functions.}, archive = {J_PRL}, author = {Andrew N. Ivanov and Olexei I. Motrunich}, doi = {10.1103/PhysRevLett.134.050403}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050403}, shortjournal = {Phys. Rev. Lett.}, title = {Volume-entangled exact scar states in the PXP and related models in any dimension}, volume = {134}, year = {2025}, }
• (2025). Multiseed krylov complexity. PRL, 134(5), 050402. (www)

  @article{ , abstract = {Krylov complexity is an attractive measure for the rate at which quantum operators spread in the space of all possible operators under dynamical evolution. One expects that its late-time plateau would distinguish between integrable and chaotic dynamics, but its ability to do so depends precariously on the choice of the initial seed. We propose to apply such considerations not to a single operator, but simultaneously to a collection of initial seeds in the manner of the block-Lanczos algorithm. We furthermore suggest that this collection should comprise all simple (few-body) operators in the theory, which echoes the applications of Nielsen complexity to dynamical evolution. The resulting construction, unlike the conventional Krylov complexity, reliably distinguishes integrable and chaotic Hamiltonians without any need for fine-tuning.}, archive = {J_PRL}, author = {Ben Craps and Oleg Evnin and Gabriele Pascuzzi}, doi = {10.1103/PhysRevLett.134.050402}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050402}, shortjournal = {Phys. Rev. Lett.}, title = {Multiseed krylov complexity}, volume = {134}, year = {2025}, }
• (2025). Heat as a witness of quantum properties. PRL, 134(5), 050401. (www)

  @article{ , abstract = {We present a new approach for witnessing quantum resources, such as entanglement and coherence, based on heat generation. Inspired by Maxwell’s demon, we ask what the optimal heat exchange between a quantum system and a thermal environment is when the process is assisted by a quantum memory. We derive fundamental energy constraints in this scenario and show that quantum states can reveal nonclassical signatures via heat exchange. This approach leads to a heat-based witness for quantum properties, offering an alternative to system-specific measurements, as it only relies on fixed energy measurements in a thermal ancilla. We illustrate our findings with the detection of entanglement in isotropic states and coherence in two-spin systems interacting with a single-mode electromagnetic field.}, archive = {J_PRL}, author = {A. de Oliveira Junior and Jonatan Bohr Brask and Patryk Lipka-Bartosik}, doi = {10.1103/PhysRevLett.134.050401}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050401}, shortjournal = {Phys. Rev. Lett.}, title = {Heat as a witness of quantum properties}, volume = {134}, year = {2025}, }
• (2025). Magic resource can enhance the quantum capacity of channels. PRL, 134(5), 050202. (www)

  @article{ , abstract = {We investigate the role of magic resource in the quantum capacity of channels. We consider the quantum channel of the recently proposed discrete beam splitter with the fixed environmental state. We find that if the fixed environmental state is a stabilizer state, then the quantum capacity is zero. Moreover, we find that the quantum capacity is nonzero for some magic states, and the quantum capacity increases linearly with respect to the number of single-qudit magic states in the environment. We also bound the maximal quantum capacity of the discrete beam splitter in terms of the amount of magic resource in the environmental states. These results suggest that magic resource can increase the quantum capacity of channels; it sheds new insight into the role of stabilizer and magic states in quantum communication.}, archive = {J_PRL}, author = {Kaifeng Bu and Arthur Jaffe}, doi = {10.1103/PhysRevLett.134.050202}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050202}, shortjournal = {Phys. Rev. Lett.}, title = {Magic resource can enhance the quantum capacity of channels}, volume = {134}, year = {2025}, }
• (2025). Entanglement detection length of multipartite quantum states. PRL, 134(5), 050201. (www)

  @article{ , abstract = {Multipartite entanglement is a valuable resource for quantum technologies. However, detecting this resource can be challenging: for genuine multipartite entanglement, the detection may require global measurements that are hard to implement experimentally. Here we introduce the concept of entanglement detection length, defined as the minimum number of particles that have to be jointly measured in order to detect genuine multipartite entanglement. For symmetric states, we show that the entanglement detection length can be determined by testing separability of the marginal states. For general states, we provide an upper bound on the entanglement detection length based on semidefinite programming. We show that the entanglement detection length is generally smaller than the minimum observable length needed to uniquely determine a multipartite state, and we provide examples achieving the maximum gap between these two quantities.}, archive = {J_PRL}, author = {Fei Shi and Lin Chen and Giulio Chiribella and Qi Zhao}, doi = {10.1103/PhysRevLett.134.050201}, journal = {Physical Review Letters}, month = {2}, number = {5}, pages = {050201}, shortjournal = {Phys. Rev. Lett.}, title = {Entanglement detection length of multipartite quantum states}, volume = {134}, year = {2025}, }
• (2025). Connecting anomalous elasticity and sub-arrhenius structural dynamics in a cell-based model. PRL, 134(4), 048203. (www)

  @article{ , abstract = {Understanding the structural dynamics of many-particle glassy systems remains a key challenge in statistical physics. Over the last decade, glassy dynamics has also been reported in biological tissues, but is far from being understood. It was recently shown that vertex models of dense biological tissue exhibit very atypical, sub-Arrhenius dynamics, and here we ask whether such atypical structural dynamics of vertex models are related to unusual elastic properties. It is known that at zero temperature these models have an elasticity controlled by their underconstrained or isostatic nature, but little is known about how their elasticity varies with temperature. To address this question we investigate the 2D Voronoi model and measure the temperature dependence of the intermediate-time plateau shear modulus and the bulk modulus. We find that unlike in conventional glass formers, these moduli increase monotonically with temperature until the system fluidizes. We further show that the structural relaxation time can be quantitatively linked to the plateau shear modulus , i.e. modulates the typical energy barrier scale for cell rearrangements. This suggests that the anomalous, structural dynamics of the 2D Voronoi model originates in its unusual elastic properties. Based on our results, we hypothesize that underconstrained systems might more generally give rise to a new class of “ultrastrong” glass formers.}, archive = {J_PRL}, author = {Chengling Li and Matthias Merkel and Daniel M. Sussman}, doi = {10.1103/PhysRevLett.134.048203}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {048203}, shortjournal = {Phys. Rev. Lett.}, title = {Connecting anomalous elasticity and sub-arrhenius structural dynamics in a cell-based model}, volume = {134}, year = {2025}, }
• (2025). Granular temperature controls local rheology of vibrated granular flows. PRL, 134(4), 048202. (www)

  @article{ , abstract = {We use numerical simulations to demonstrate a local rheology for dense granular flows under shear and vibration. Granular temperature has been suggested as a rheological control but has been difficult to isolate. Here, we consider a granular assembly that is subjected to simple shear and harmonic vibration at the boundary, which provides a controlled source of granular temperature. We find that friction is reduced due to local velocity fluctuations of grains. All data obey a local rheology that relates the material friction coefficient, the granular temperature, and the dimensionless shear rate. We also observe that reduction in material friction due to granular temperature is associated with reduction in fabric anisotropy. We demonstrate that the temperature can be modeled by a heat equation with dissipation with appropriate boundary conditions, which provides complete closure of the system and allows a fully local continuum description of sheared, vibrated granular flows. This success suggests local rheology based on temperature combined with a diffusion equation for granular temperature may provide a general strategy to model dense granular flows.}, archive = {J_PRL}, author = {Mitchell G. Irmer and Emily E. Brodsky and Abram H. Clark}, doi = {10.1103/PhysRevLett.134.048202}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {048202}, shortjournal = {Phys. Rev. Lett.}, title = {Granular temperature controls local rheology of vibrated granular flows}, volume = {134}, year = {2025}, }
• (2025). Void connectivity and criticality in the compression-induced gel-to-glass transition of short-range attractive colloids. PRL, 134(4), 048201. (www)

  @article{ , abstract = {Gels and attractive glasses—both dynamically arrested states formed through short-range attraction—are commonly found in a range of soft matter systems, including colloids, emulsions, proteins, and wet granular materials. Previous studies have revealed intriguing similarities and distinctions in their structural, dynamic, vibrational, and mechanical properties. However, the microstructural mechanisms underlying the gel-to-glass transition remain elusive. To address this, we investigate uniaxial compression-induced gel collapse using confocal microscopy, which provides experimental access to the relationship between mechanical stress and microstructure. Together with Brownian dynamics simulations, our study reveals two sequential transitions in void structure: from gels with percolating voids to isolated voids, and ultimately to voidless glasses. These transitions are closely linked to a shift from superlinear power-law scaling to explosive divergence toward the packing limit in both normal and deviatoric stresses as a function of volume fraction, particularly at lower temperatures. Understanding these mechanically self-organized transitions and their associated criticality deepens our insight into disordered solids, enabling better control over mechanical properties, interfacial characteristics, and transport behavior in porous materials.}, archive = {J_PRL}, author = {Michio Tateno and Yinqiao Wang and Hajime Tanaka}, doi = {10.1103/PhysRevLett.134.048201}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {048201}, shortjournal = {Phys. Rev. Lett.}, title = {Void connectivity and criticality in the compression-induced gel-to-glass transition of short-range attractive colloids}, volume = {134}, year = {2025}, }
• (2025). Electrostatic correlation augmented self-consistent field theory and its application to polyelectrolyte brushes. PRL, 134(4), 048101. (www)

  @article{ , abstract = {Modeling ion correlations in inhomogeneous polymers and soft matters with spatially varying ionic strength or dielectric permittivity remains a great challenge. Here, we develop a new theory that systematically incorporates electrostatic fluctuations into the self-consistent field theory for polymers. The theory is applied to polyelectrolyte brushes to explain abnormal phenomena observed in recent experiments. We show that ion correlations induce a nonmonotonic change of the brush height: collapse followed by reexpansion. The scaling analysis elucidates the origin as the competition between the repulsive osmotic pressure due to translational entropy and the attraction induced by ion correlations. We also clarify the absence of causal relationship between the brush collapse-reexpansion and the inversion of the surface electrostatic potential. Furthermore, strong ion correlations can trigger microphase separation, either in the lateral direction as pinned micelles or in the normal direction as oscillatory layers. Our theoretical predictions are in good agreement with the experimental results reported in the literature.}, archive = {J_PRL}, author = {Chao Duan and Nikhil R. Agrawal and Rui Wang}, doi = {10.1103/PhysRevLett.134.048101}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {048101}, shortjournal = {Phys. Rev. Lett.}, title = {Electrostatic correlation augmented self-consistent field theory and its application to polyelectrolyte brushes}, volume = {134}, year = {2025}, }
• (2025). Macroscopic stochastic model for economic cycle dynamics. PRL, 134(4), 047402. (www)

  @article{ , abstract = {We present a stochastic dynamic model which can explain economic cycles. We show that the macroscopic description yields a complex dynamical landscape consisting of multiple stable fixed points, each corresponding to a split of the population into a large low and a small high income group. The stochastic fluctuations induce switching between the resulting metastable states and excitation oscillations just below a deterministic bifurcation. The shocks are caused by the decisions of a few agents who have a disproportionate influence over the macroscopic state of the economy due to the unequal distribution of wealth among the population. The fluctuations have a long-term effect on the growth of economic output and lead to business cycle oscillations exhibiting coherence resonance, where the correlation time is controlled by the population size which is inversely proportional to the noise intensity.}, archive = {J_PRL}, author = {Sören Nagel and Jobst Heitzig and Eckehard Schöll}, doi = {10.1103/PhysRevLett.134.047402}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {047402}, shortjournal = {Phys. Rev. Lett.}, title = {Macroscopic stochastic model for economic cycle dynamics}, volume = {134}, year = {2025}, }
• (2025). Targeted avoidance in complex networks. PRL, 134(4), 047401. (www)

  @article{ , abstract = {The study of spreading in networks presents a fascinating topic with a wide array of practical applications. Various strategies have been proposed to attack or immunize networks. However, it is often not feasible or necessary to consider the entire network in the context of real-world systems. Here, we focus on a certain group of target nodes with the aim of disconnecting them from the global network structure. For instance, it becomes possible to effectively prevent the transmission of the disease to vulnerable populations, such as infants and the elderly, by isolating some specific nodes such as their caretakers during the epidemic. From this perspective of targeted avoidance, we introduce a series of target centrality indicators and apply them to segment the target nodes from the giant component of the network. Additionally, we propose a more effective iterative graph-segmentation method for targeted immunization. Our experimental findings reveal that our proposed method can substantially reduce the number of nodes required for removal when compared with the methods based on target centrality, which implies a significant cost effectiveness in isolating target nodes from the rest of the network. Finally, we verify our method on a large mobility network in the scenario of the COVID-19 pandemic, and find that our method can effectively protect the elderly by immunizing or isolating a very small group of nodes.}, archive = {J_PRL}, author = {Aobo Zhang and Chi Ho Yeung and Chen Zhao and Ying Fan and An Zeng}, doi = {10.1103/PhysRevLett.134.047401}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {047401}, shortjournal = {Phys. Rev. Lett.}, title = {Targeted avoidance in complex networks}, volume = {134}, year = {2025}, }
• (2025). Electrically switchable longitudinal nonlinear conductivity in magnetic semiconductors. PRL, 134(4), 046801. (www)

  @article{ , abstract = {Writing data by electric field (as opposed to electric current) offers promises for energy efficient memory devices. While this data writing scheme is enabled by the magnetoelectric effect, the narrow spectrum of room-temperature magnetoelectrics hinders the design of practical magnetoelectric memories, and the exploration of other mechanisms toward low-power memories is greatly demanding. Here, we propose a mechanism that allows the electric-field writing of data beyond the framework of magnetoelectric effect. By symmetry analysis, we show that electric field can induce longitudinal nonlinear conductivity (LNC) in a wide spectrum of magnetic materials, including ferromagnets, antiferromagnets, magnetoelectrics, and nonmagnetoelectrics. The LNC is electrically switchable by reversing the electric field, where the switched LNC is detectable by transport measurements. Our first-principles simulations combined with transport calculations further predict and (room-temperature antiferromagnets) to showcase electrically switchable LNC. Our Letter helps enrich the research avenues in nonlinear charge transport, and offers a pathway for designing energy efficient devices based on LNC.}, archive = {J_PRL}, author = {Hong Jian Zhao and Yuhao Fu and Yurong Yang and Yanchao Wang and Laurent Bellaiche and Yanming Ma}, doi = {10.1103/PhysRevLett.134.046801}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046801}, shortjournal = {Phys. Rev. Lett.}, title = {Electrically switchable longitudinal nonlinear conductivity in magnetic semiconductors}, volume = {134}, year = {2025}, }
• (2025). Anisotropic skyrmion and multi-q spin dynamics in centrosymmetric Gd2PdSi3. PRL, 134(4), 046702. (www)

  @article{ , abstract = {Skyrmions are particlelike vortices of magnetization with nontrivial topology, which are usually stabilized by Dzyaloshinskii-Moriya interactions (DMI) in noncentrosymmetric bulk materials. Exceptions are centrosymmetric Gd- and Eu-based skyrmion-lattice (SL) hosts with zero DMI, where both the SL stabilization mechanisms and magnetic ground states remain controversial. We address these here by investigating both the static and dynamical spin properties of the centrosymmetric SL host using muon spectroscopy. We find that spin fluctuations in the noncoplanar SL phase are highly anisotropic, implying that spin anisotropy plays a prominent role in stabilizing this phase. We also observe strongly anisotropic spin dynamics in the ground-state (IC-1) incommensurate magnetic phase of the material, indicating that it hosts a meronlike multi- structure. In contrast, the higher-field, coplanar IC-2 phase is found to be single with nearly isotropic spin dynamics.}, archive = {J_PRL}, author = {M. Gomilšek and T. J. Hicken and M. N. Wilson and K. J. A. Franke and B. M. Huddart and A. Štefančič and S. J. R. Holt and G. Balakrishnan and D. A. Mayoh and M. T. Birch and S. H. Moody and H. Luetkens and Z. Guguchia and M. T. F. Telling and P. J. Baker and S. J. Clark and T. Lancaster}, doi = {10.1103/PhysRevLett.134.046702}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046702}, shortjournal = {Phys. Rev. Lett.}, title = {Anisotropic skyrmion and multi-q spin dynamics in centrosymmetric Gd2PdSi3}, volume = {134}, year = {2025}, }
• (2025). Realizing quantitative quasiparticle modeling of skyrmion dynamics in arbitrary potentials. PRL, 134(4), 046701. (www)

  @article{ , abstract = {We demonstrate fully quantitative Thiele model simulations of magnetic skyrmion dynamics on previously unattainable experimentally relevant large length and time scales by ascertaining the key missing parameters needed to calibrate the experimental and simulation timescales and current-induced forces. Our work allows us to determine complete spatial pinning energy landscapes that enable quantification of experimental studies of diffusion in arbitrary potentials within the Lifson-Jackson framework. Our method enables us to ascertain the timescales, and by isolating the effect of ultralow current density (order ) generated torques we directly infer the total force acting on the skyrmion for a quantitative modeling.}, archive = {J_PRL}, author = {Maarten A. Brems and Tobias Sparmann and Simon M. Fröhlich and Leonie-C. Dany and Jan Rothörl and Fabian Kammerbauer and Elizabeth M. Jefremovas and Oded Farago and Mathias Kläui and Peter Virnau}, doi = {10.1103/PhysRevLett.134.046701}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046701}, shortjournal = {Phys. Rev. Lett.}, title = {Realizing quantitative quasiparticle modeling of skyrmion dynamics in arbitrary potentials}, volume = {134}, year = {2025}, }
• (2025). Exciton condensation in landau levels of quantum spin hall insulators. PRL, 134(4), 046601. (www)

  @article{ , abstract = {We theoretically study the quantum spin Hall insulator (QSHI) in a perpendicular magnetic field. In the noninteracting case, the QSHI with space inversion and/or uniaxial spin rotation symmetry undergoes a topological transition into a normal insulator phase at a critical magnetic field . The exciton condensation in the lowest Landau levels is triggered by Coulomb interactions in the vicinity of at low temperature and spontaneously breaks the inversion and the spin rotation symmetries. We propose that the electron spin resonance spectroscopy with the ac magnetic field also aligned in the perpendicular direction can directly probe the exciton condensation order. Our results should apply to QSHIs such as the quantum wells and monolayer transition-metal dichalcogenides.}, archive = {J_PRL}, author = {Hong-Mao Peng and Zhan Wang and Long Zhang}, doi = {10.1103/PhysRevLett.134.046601}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046601}, shortjournal = {Phys. Rev. Lett.}, title = {Exciton condensation in landau levels of quantum spin hall insulators}, volume = {134}, year = {2025}, }
• (2025). Doped mott phase and charge correlations in monolayer 1T−NbSe2. PRL, 134(4), 046504. (www)

  @article{ , abstract = {The doped Hubbard model is one of the paradigmatic platforms to engineer exotic quantum many-body states, including charge-ordered states, strange metals, and unconventional superconductors. While undoped and doped correlated phases have been experimentally realized in a variety of twisted van der Waals materials, experiments in monolayer materials, and in particular 1 T transition metal dichalcogenides, have solely reached the conventional insulating undoped regime. Correlated phases in monolayer two-dimensional materials have much higher associated energy scales than their twisted counterparts, making doped correlated monolayers an attractive platform for high temperature correlated quantum matter. Here, we demonstrate the realization of a doped Mott phase in a van der Waals dichalcogenide 1 T − NbSe 2 monolayer. The system is electron doped due to electron transfer from a monolayer van der Waals substrate via proximity, leading to a correlated triangular lattice with both half-filled and fully filled sites. We analyze the distribution of the half-filled and filled sites and show the arrangement is unlikely to be controlled by disorder alone, and we show that the presence of competing nonlocal many-body correlations would account for the charge correlations found experimentally. Our results establish 1 T − NbSe 2 as a potential monolayer platform to explore correlated doped Mott physics in a frustrated lattice.}, archive = {J_PRL}, author = {Xin Huang and Jose L. Lado and Jani Sainio and Peter Liljeroth and Somesh Chandra Ganguli}, doi = {10.1103/PhysRevLett.134.046504}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046504}, shortjournal = {Phys. Rev. Lett.}, title = {Doped mott phase and charge correlations in monolayer 1T−NbSe2}, volume = {134}, year = {2025}, }
• (2025). Solvable nonunitary fermionic long-range model with extended symmetry. PRL, 134(4), 046503. (www)

  @article{ , abstract = {We define and study a long-range version of the xx model, arising as the free-fermion point of the xxz -type Haldane-Shastry (HS) chain. It has a description via nonunitary fermions, based on the free-fermion Temperley-Lieb algebra, and may also be viewed as an alternating spin chain. Even and odd lengths behave very differently; we focus on odd length. The model is integrable, and we explicitly identify two commuting Hamiltonians. While nonunitary, their spectrum is real by PT symmetry. One Hamiltonian is chiral and quadratic in fermions, while the other is parity invariant and quartic. Their one-particle spectra have two linear branches, realizing a massless relativistic dispersion on the lattice. The appropriate fermionic modes arise from “quasi-translation” symmetry, which replaces ordinary translation symmetry. The model exhibits exclusion statistics, like the isotropic HS chain, with even more “extended symmetry” and larger degeneracies.}, archive = {J_PRL}, author = {Adel Ben Moussa and Jules Lamers and Didina Serban and Ayman Toufik}, doi = {10.1103/PhysRevLett.134.046503}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046503}, shortjournal = {Phys. Rev. Lett.}, title = {Solvable nonunitary fermionic long-range model with extended symmetry}, volume = {134}, year = {2025}, }
• (2025). Developing fractional quantum hall states at even-denominator fillings 1/6 and 1/8. PRL, 134(4), 046502. (www)

  @article{ , abstract = {In the extreme quantum limit, when the Landau level filling factor ν < 1 , the dominant electron-electron interaction in low-disorder two-dimensional electron systems leads to exotic many-body phases. The ground states at even-denominator ν = 1 / 2 and 1 / 4 are typically Fermi seas of composite fermions carrying two and four flux quanta, surrounded by the Jain fractional quantum Hall states (FQHSs) at odd-denominator fillings ν = p / ( 2 p ± 1 ) and ν = p / ( 4 p ± 1 ) , where p is an integer. For ν < 1 / 5 , an insulating behavior, which is generally believed to signal the formation of a pinned Wigner crystal, is seen. Our experiments on ultra-high-quality, dilute, GaAs two-dimensional electron systems reveal developing FQHSs at ν = p / ( 6 p ± 1 ) and ν = p / ( 8 p ± 1 ) , manifested by magnetoresistance minima superimposed on the insulating background. In stark contrast to ν = 1 / 2 and 1 / 4 , however, we observe a pronounced, sharp minimum in magnetoresistance at ν = 1 / 6 and a somewhat weaker minimum at ν = 1 / 8 , suggesting developing FQHSs, likely stabilized by the pairing of composite fermions that carry six and eight flux quanta. Our results signal the unexpected entry, in ultra-high-quality samples, of FQHSs at even-denominator fillings 1 / 6 and 1 / 8 , which are likely to harbor non-Abelian anyon excitations.}, archive = {J_PRL}, author = {Chengyu Wang and P. T. Madathil and S. K. Singh and A. Gupta and Y. J. Chung and L. N. Pfeiffer and K. W. Baldwin and M. Shayegan}, doi = {10.1103/PhysRevLett.134.046502}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046502}, shortjournal = {Phys. Rev. Lett.}, title = {Developing fractional quantum hall states at even-denominator fillings 1/6 and 1/8}, volume = {134}, year = {2025}, }
• (2025). Landau-level mixing and SU(4) symmetry breaking in graphene. PRL, 134(4), 046501. (www)

  @article{ , abstract = {Recent scanning tunneling microscopy experiments on graphene at charge neutrality under strong magnetic fields have uncovered a ground state characterized by Kekulé distortion (KD). In contrast, nonlocal spin and charge transport experiments in double-encapsulated graphene, which has a higher dielectric constant, have identified an antiferromagnetic (AF) ground state. We propose a mechanism to reconcile these conflicting observations by showing that Landau-level mixing can drive a transition from AF to KD with the reduction of the dielectric screening. Our conclusion is drawn from studying the effect of Landau-level mixing on the lattice-scale, valley-dependent interactions to leading order in graphene’s fine structure constant . This analysis provides three key insights: (1) valley-dependent interactions remain predominantly short-range with the Haldane pseudopotential being at least an order of magnitude greater than the others, affirming the validity of delta-function approximation for these interactions. (2) The phase transition between the AF and KD states is driven by the microscopic process in the double-exchange Feynman diagram. (3) The magnitudes of the coupling constants are significantly boosted by remote Landau levels. Our model also provides a theoretical basis for numerical studies of fractional quantum Hall states in graphene.}, archive = {J_PRL}, author = {Nemin Wei and Guopeng Xu and Inti Sodemann Villadiego and Chunli Huang}, doi = {10.1103/PhysRevLett.134.046501}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046501}, shortjournal = {Phys. Rev. Lett.}, title = {Landau-level mixing and SU(4) symmetry breaking in graphene}, volume = {134}, year = {2025}, }
• (2025). Elastic screening of pseudogauge fields in graphene. PRL, 134(4), 046404. (www)

  @article{ , abstract = {Lattice deformations in graphene couple to the low-energy electronic degrees of freedom as effective scalar and gauge fields. Using molecular dynamics simulations, we show that the optical component of the displacement field, i.e., the relative motion of different sublattices, contributes at equal order as the acoustic component and effectively screens the pseudogauge fields. In particular, we consider twisted bilayer graphene and corrugated monolayer graphene. In both cases, optical lattice displacements significantly reduce the overall magnitude of the pseudomagnetic fields. For corrugated graphene, optical contributions also reshape the pseudomagnetic field and significantly modify the electronic bands near charge neutrality. Previous studies based on continuum elasticity, which ignores this effect, have therefore systematically overestimated the strength of the strain-induced pseudomagnetic field. Our results have important consequences for the interpretation of experiments and design of straintronic applications.}, archive = {J_PRL}, author = {Christophe De Beule and Robin Smeyers and Wilson Nieto Luna and E. J. Mele and Lucian Covaci}, doi = {10.1103/PhysRevLett.134.046404}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046404}, shortjournal = {Phys. Rev. Lett.}, title = {Elastic screening of pseudogauge fields in graphene}, volume = {134}, year = {2025}, }
• (2025). Enforced symmetry breaking for anomalous valley hall effect in two-dimensional hexagonal lattices. PRL, 134(4), 046403. (www)

  @article{ , abstract = {The anomalous valley Hall effect (AVHE) is a pivotal phenomenon that allows for the exploitation of the valley degree of freedom in materials. A general strategy for its realization and manipulation is crucial for valleytronics. Here, by considering all possible symmetries, we propose general rules for the realization and manipulation of AVHE in two-dimensional hexagonal lattices. The realization of AVHE requires breaking the enforced symmetry that is associated with different valleys or reverses the sign of Berry curvature. Further manipulation of AVHE requires asymmetry operators connecting two states with opposite signs of Berry curvature. These rules for realizing and manipulating AVHE are extendable to generic points in momentum space. Combined with first-principles calculations, we realize the controllable AVHE in four representative systems, i.e., monolayer , CrOBr, and bilayer . Our work provides symmetry rules for designing valleytronic materials that could facilitate the experimental detection and realistic applications.}, archive = {J_PRL}, author = {Yongqian Zhu and Jia-Tao Sun and Jinbo Pan and Jun Deng and Shixuan Du}, doi = {10.1103/PhysRevLett.134.046403}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046403}, shortjournal = {Phys. Rev. Lett.}, title = {Enforced symmetry breaking for anomalous valley hall effect in two-dimensional hexagonal lattices}, volume = {134}, year = {2025}, }
• (2025). Short-range excitonic phenomena in low-density metals. PRL, 134(4), 046402. (www)

  @article{ , abstract = {Excitonic effects in metals are usually supposed to be weak, because the Coulomb interaction is strongly screened. Here, we investigate the low-density regime of the homogeneous electron gas, where, besides the usual high-energy plasmons, the existence of low-energy excitonic collective modes has recently been suggested. Using the Bethe-Salpeter equation (BSE), we show that indeed low-energy modes appear, thanks to reduced screening at short distances. This requires going beyond common approximations to ab initio BSE calculations, which suffer from a self-polarization error that overscreens the electron-hole interaction. The electron-hole wave function of the low-energy mode shows strong and very anisotropic electron-hole correlation, which speaks for an excitonic character of this mode. The fact that the electron-hole interaction at short distances is at the origin of these phenomena explains why, on the other hand, also the simple adiabatic local density approximation to time-dependent density functional theory can capture these effects. This exotic regime might be found in doped semiconductors and interfaces.}, archive = {J_PRL}, author = {Jaakko Koskelo and Lucia Reining and Matteo Gatti}, doi = {10.1103/PhysRevLett.134.046402}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046402}, shortjournal = {Phys. Rev. Lett.}, title = {Short-range excitonic phenomena in low-density metals}, volume = {134}, year = {2025}, }
• (2025). Magnetic exciton of EuS revealed by resonant inelastic X-ray scattering. PRL, 134(4), 046401. (www)

  @article{ , abstract = {We report the valence-to-core resonant inelastic x-ray scattering of EuS measured at the L 3 edge of Eu. The obtained data reveal two sets of excitations: one set is composed of a hole in the S 3p bands and an electron excited to extended Eu 5d band states, and the other is made up from a hole in the Eu 4f states and an electron in localized Eu 5d states bound to the 4f hole by its Coulomb potential. The delocalized excitations arise from the dipole-allowed 5 d → 2 p emissions, whereas the localized excitations result from the dipole-forbidden (quadrupole-allowed) 4 f → 2 p emissions. Both these emission channels have a comparable intensity thanks to a small number of occupied 5d states ( ≈ 0.6 ) combined with a large number of occupied 4f states (seven). We identify the localized electron-hole pairs with the “magnetic excitons” suggested in the past as an interpretation of the sharp features seen in the optical absorption spectra. Our observations provide a direct experimental evidence of these excitons, which has been missing up to now.}, archive = {J_PRL}, author = {Lucia Amidani and Jonas J. Joos and Pieter Glatzel and Jindřich Kolorenč}, doi = {10.1103/PhysRevLett.134.046401}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046401}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic exciton of EuS revealed by resonant inelastic X-ray scattering}, volume = {134}, year = {2025}, }
• (2025). Real-time detection and control of correlated charge tunneling in a quantum dot. PRL, 134(4), 046303. (www)

  @article{ , abstract = {We experimentally demonstrate the real-time detection and control of correlated charge tunneling in a dynamically driven quantum dot. Specifically, we measure the joint distribution of waiting times between tunneling charges and show that the waiting times for holes may be strongly correlated due to the periodic drive and the Coulomb interactions on the dot, although the electron waiting times are not. Our measurements are in excellent agreement with a theoretical model that allows us to develop a detailed understanding of the correlated tunneling events. We also demonstrate that the degree of correlations can be controlled by the drive. Our experiment paves the way for systematic real-time investigations of correlated electron transport in low-dimensional nanostructures.}, archive = {J_PRL}, author = {Johannes C. Bayer and Fredrik Brange and Adrian Schmidt and Timo Wagner and Eddy P. Rugeramigabo and Christian Flindt and Rolf J. Haug}, doi = {10.1103/PhysRevLett.134.046303}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046303}, shortjournal = {Phys. Rev. Lett.}, title = {Real-time detection and control of correlated charge tunneling in a quantum dot}, volume = {134}, year = {2025}, }
• (2025). Anderson transition for light in a three-dimensional random medium. PRL, 134(4), 046302. (www)

  @article{ , abstract = {We study Anderson transition for light in three dimensions by performing large-scale simulations of electromagnetic wave transport in disordered ensembles of perfect-electric-conducting spatially overlapping spheres. A mobility edge that separates diffusive transport and Anderson localization is identified, revealing a sharp transition from diffusion to localization for light. Critical behavior in the vicinity of the mobility edge is well described by a single-parameter scaling law. The critical exponent is found to be consistent with the value known for the Anderson transition of the orthogonal universality class. Statistical distribution of total transmission at the mobility edge is described without any fit parameter by the diagrammatic perturbation theory originally developed for scalar wave diffusion, but notable deviation from the theory is found when Anderson localization sets in.}, archive = {J_PRL}, author = {Alexey Yamilov and Hui Cao and Sergey E. Skipetrov}, doi = {10.1103/PhysRevLett.134.046302}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046302}, shortjournal = {Phys. Rev. Lett.}, title = {Anderson transition for light in a three-dimensional random medium}, volume = {134}, year = {2025}, }
• (2025). Epitaxially defined luttinger liquids on MoS2 bicrystals. PRL, 134(4), 046301. (www)

  @article{ , abstract = {A mirror twin boundary (MTB) in a transition metal dichalcogenide monolayer can host one-dimensional electron liquid of a topological nature with tunable interactions. Unfortunately, electrical characterization of such boundaries has been challenging due to the paucity of samples with large enough size and high quality. Here, we report the conductance measurements of individual MTBs in epitaxially grown monolayer molybdenum disulfide bicrystals that are tens of micrometers long. These MTBs exhibit power-law behaviors of conductance as a function of temperature and bias voltage up to room temperature, consistent with electrons tunneling into a Luttinger liquid. Transport measurements of two distinct types of MTBs reveal the critical role of the atomic-scale defects. This study demonstrates that MTBs in transition metal dichalcogenide monolayers provide an exciting new platform for studying the interplay between electronic interactions and topology.}, archive = {J_PRL}, author = {Bingchen Deng and Heonsu Ahn and Jue Wang and Gunho Moon and Cheolhee Han and Ninad Dongre and Chao Lei and Giovanni Scuri and Jiho Sung and Elise Brutschea and Kenji Watanabe and Takashi Taniguchi and Fan Zhang and Moon-Ho Jo and Hongkun Park}, doi = {10.1103/PhysRevLett.134.046301}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046301}, shortjournal = {Phys. Rev. Lett.}, title = {Epitaxially defined luttinger liquids on MoS2 bicrystals}, volume = {134}, year = {2025}, }
• (2025). Constant-potential modeling of electrical double layers accounting for electron spillover. PRL, 134(4), 046201. (www)

  @article{ , abstract = {Constant-potential molecular dynamics (MD) simulations are indispensable for understanding the structure, capacitance, and dynamics of electrical double layers (EDLs) at the atomistic level. However, the classical constant-potential method, relying on the so-called “fluctuating charges” to keep electrode equipotential, overlooks quantum effects on the electrode and always underestimates EDL capacitance for typical metal electrode and aqueous electrolyte interfaces. Here, we propose a constant potential method accounting for electron spillover on the outermost nuclei of the electrode . For EDLs at Au(111) electrodes, our MD simulation reveals bell-shaped capacitance curves in magnitude and shape both quantitatively consistent with experiments. It unveils the electrode-polarization-dependent local electric fields, agreeing with experimental observations of redshift vibration of interfacial water under negative polarization and predicting a blueshift under positive polarization, and further identifies geometry dependence of two timescales during charging.}, archive = {J_PRL}, author = {Zhenxiang Wang and Ming Chen and Jiedu Wu and Xiangyu Ji and Liang Zeng and Jiaxing Peng and Jiawei Yan and Alexei A. Kornyshev and Bingwei Mao and Guang Feng}, doi = {10.1103/PhysRevLett.134.046201}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046201}, shortjournal = {Phys. Rev. Lett.}, title = {Constant-potential modeling of electrical double layers accounting for electron spillover}, volume = {134}, year = {2025}, }
• (2025). Importance of density for phase-change materials demonstrated by ab initio simulations of amorphous antimony. PRL, 134(4), 046101. (www)

  @article{ , abstract = {Phase change materials (PCMs) serve as useful components in electronics and photonics. Here we demonstrate that various kinds of material properties of a PCM are significantly influenced by the realized mass density. Using ab initio simulations, we investigate supercooled-liquid antimony and the subsequent transition to a glassy phase. We observe a transition in the supercooled-liquid phase from an undistorted high-temperature to an increasingly Peierls-like distorted low-temperature phase. This transition also manifests in both the electronic density of states and optical properties. The strong dependence of these properties on mass density leads the way to explorations of property design for nanoconfined devices beyond the usual compositional modifications.}, archive = {J_PRL}, author = {Nils Holle and Sebastian Walfort and Jakob Ballmaier and Riccardo Mazzarello and Martin Salinga}, doi = {10.1103/PhysRevLett.134.046101}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {046101}, shortjournal = {Phys. Rev. Lett.}, title = {Importance of density for phase-change materials demonstrated by ab initio simulations of amorphous antimony}, volume = {134}, year = {2025}, }
• (2025). Demonstration of similarity laws and scaling networks for radio-frequency plasmas. PRL, 134(4), 045301. (www)

  @article{ , abstract = {We experimentally demonstrate similarity laws for capacitive radio-frequency (rf) plasmas, showing that two rf discharges are scale-invariant in geometrically similar systems in which the gas pressure, gap dimension, and driving frequency are proportionally tuned. Spatiotemporal distributions of the excitation rate are measured based on phase-resolved optical emission spectroscopy, and the tendencies of the excitation dynamics scaling with control parameters are presented and agree well with particle-in-cell simulations. Furthermore, similarity-based scaling networks are established, which extensively correlate the discharge states (i.e., the initial, intermediate, and similarity states), enabling an effective strategy for determining scaling relations with fewer experiments. The framework of the scaling networks is interpreted based on the kinetic Boltzmann equation coupled with Poisson’s equation. The present work reveals the nature of discharge similarity and provides an additional knob for the exploration of upscaled rf plasma sources for industrial applications, such as large-area etching facilities.}, archive = {J_PRL}, author = {Dong Yang and John P. Verboncoeur and Yangyang Fu}, doi = {10.1103/PhysRevLett.134.045301}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {045301}, shortjournal = {Phys. Rev. Lett.}, title = {Demonstration of similarity laws and scaling networks for radio-frequency plasmas}, volume = {134}, year = {2025}, }
• (2025). Role of nonlinear landau damping for cosmic-ray transport. PRL, 134(4), 045201. (www)

  @article{ , abstract = {We present the first assessment, using hybrid PIC simulations, of the role of nonlinear Landau damping in the process of self-generated scattering in a high β plasma, conditions appropriate for CR scattering in the halo of the Galaxy. The drift speed of CRs reduces due to scattering, but remains super-Alfvénic due to damping. Furthermore, this damping process manifests itself in the form of heating of the background plasma. We also show that the damping leads to an inverse cascade process, consisting of producing nonresonant large scale modes, a novel result with many potential phenomenological implications.}, archive = {J_PRL}, author = {Benedikt Schroer and Damiano Caprioli and Pasquale Blasi}, doi = {10.1103/PhysRevLett.134.045201}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {045201}, shortjournal = {Phys. Rev. Lett.}, title = {Role of nonlinear landau damping for cosmic-ray transport}, volume = {134}, year = {2025}, }
• (2025). Steering laser-produced THz radiation in air with superluminal ionization fronts. PRL, 134(4), 045001. (www)

  @article{ , abstract = {We demonstrate that pulsed THz radiation produced in air by a focused ultrashort laser pulse can be steered to large angles or even in the backward direction with respect to the laser propagation axis. The emission angle is adjusted by the flying focus technique, which determines the speed and direction of the ionization front created by the single-color laser pulse. This easily adjustable THz source, being well separated from the intense laser, opens exciting applications for remote THz spectroscopy.}, archive = {J_PRL}, author = {Silin Fu and Baptiste Groussin and Yi Liu and André Mysyrowicz and Vladimir Tikhonchuk and Aurélien Houard}, doi = {10.1103/PhysRevLett.134.045001}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {045001}, shortjournal = {Phys. Rev. Lett.}, title = {Steering laser-produced THz radiation in air with superluminal ionization fronts}, volume = {134}, year = {2025}, }
• (2025). Optimal navigation in microfluidics via the optimization of a discrete loss. PRL, 134(4), 044001. (www)

  @article{ , abstract = {Optimal path planning and control of microscopic devices navigating in fluid environments is essential for applications ranging from targeted drug delivery to environmental monitoring. These tasks are challenging due to the complexity of microdevice-flow interactions. We introduce a closed-loop control method that optimizes a discrete loss (ODIL) in terms of dynamics and path objectives. In comparison with reinforcement learning, ODIL is more robust, up to 3 orders faster, and excels in high-dimensional action and state spaces, making it a powerful tool for navigating complex flow environments.}, archive = {J_PRL}, author = {Petr Karnakov and Lucas Amoudruz and Petros Koumoutsakos}, doi = {10.1103/PhysRevLett.134.044001}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {044001}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal navigation in microfluidics via the optimization of a discrete loss}, volume = {134}, year = {2025}, }
• (2025). Upper bound for the quantum coupling between free electrons and photons. PRL, 134(4), 043804. (www)

  @article{ , abstract = {The quantum interaction between free electrons and photons is fundamental to free-electron-based light sources and free-electron quantum optics applications. A large coupling between free electrons and photons is generally desired. In this Letter, I obtain the upper bound for the quantum coupling between free electrons and photons. The upper bound has a straightforward expression and can be applied to a broad range of optical materials, especially widely used low-loss photonic materials. The upper bound depends on the optical medium, the free-electron velocity, and the separation between the free electron and the optical medium. With simple structures, the numerically calculated coupling coefficient can reach ∼ 99 % of the upper bound. This study provides simple and practical guidance to reach the strong coupling between free electrons and photons.}, archive = {J_PRL}, author = {Zhexin Zhao}, doi = {10.1103/PhysRevLett.134.043804}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043804}, shortjournal = {Phys. Rev. Lett.}, title = {Upper bound for the quantum coupling between free electrons and photons}, volume = {134}, year = {2025}, }
• (2025). Maximal quantum interaction between free electrons and photons. PRL, 134(4), 043803. (www)

  @article{ , abstract = {The emerging field of free-electron quantum optics enables electron-photon entanglement and holds the potential for generating nontrivial photon states for quantum information processing. Although recent experimental studies have entered the quantum regime, rapid theoretical developments predict that qualitatively unique phenomena only emerge beyond a certain interaction strength. It is thus pertinent to identify the maximal electron-photon interaction strength and the materials, geometries, and particle energies that enable one to approach it. We derive an upper limit to the quantum vacuum interaction strength between free electrons and single-mode photons, which illuminates the conditions for the strongest interaction. Crucially, we obtain an explicit energy selection recipe for electrons and photons to achieve maximal interaction at arbitrary separations and identify two optimal regimes favoring either fast or slow electrons over those with intermediate velocities. We validate the limit by analytical and numerical calculations on canonical geometries and provide near-optimal designs indicating the feasibility of strong quantum interactions. Our findings offer fundamental intuition for maximizing the quantum interaction between free electrons and photons and provide practical design rules for future experiments on electron-photon and electron-mediated photon-photon entanglement. They should also enable the evaluation of key metrics for applications such as the maximum power of free-electron radiation sources and the maximum acceleration gradient of dielectric laser accelerators.}, archive = {J_PRL}, author = {Zetao Xie and Zeling Chen and Hao Li and Qinghui Yan and Hongsheng Chen and Xiao Lin and Ido Kaminer and Owen D. Miller and Yi Yang}, doi = {10.1103/PhysRevLett.134.043803}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043803}, shortjournal = {Phys. Rev. Lett.}, title = {Maximal quantum interaction between free electrons and photons}, volume = {134}, year = {2025}, }
• (2025). Smith-purcell radiation in two dimensions. PRL, 134(4), 043802. (www)

  @article{ , abstract = {Smith-Purcell radiation (SPR) is an electromagnetic radiation generated by the motion of free electrons in close to a periodic structure. Over the past 70 years, there has been significant interest in the generation of light in three-dimensional (3D) free space through SPR. Here, by using the interaction between moving electrons and a designed metallic nanoaperture array, the observation of two-dimensional (2D) SPR, e.g., the plasmon polaritons propagating on metal surfaces, is presented. This phenomenon was confirmed using cathodoluminescence under grazing incidence, by decoupling 2D SPR with specially designed optical grating into far field. Moreover, by utilizing the phased array radar effect in 2D, the radiation direction of 2D SPR is demonstrated to be manipulated by rotating the aperture orientation. This work not only expands our understanding of SPR from the 3D to 2D, but also provides a practical approach for controlling the propagation of 2D SPR.}, archive = {J_PRL}, author = {Zhiguo Sun and Liyuan Cao and Lei Wang and Wei Wu and Huadong Yang and Jiawei Wang and Weiwei Luo and Mengxin Ren and Wei Cai and Jingjun Xu}, doi = {10.1103/PhysRevLett.134.043802}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043802}, shortjournal = {Phys. Rev. Lett.}, title = {Smith-purcell radiation in two dimensions}, volume = {134}, year = {2025}, }
• (2025). Control of chirality and directionality of nonlinear metasurface light source via moiré engineering. PRL, 134(4), 043801. (www)

  @article{ , abstract = {Metasurfaces have revolutionized nonlinear and quantum light manipulation in the past decade, enabling the design of materials that can tune polarization, frequency, and direction of light simultaneously. However, tuning of metasurfaces is traditionally achieved by changing their microscopic structure, which does not allow in situ tuning and dynamic optimization of the metasurfaces. In this Letter, we explore the concept of twisted bilayer and tetralayer nonlinear metasurfaces, which offer rich tunability in its effective nonlinear susceptibilities. Using gold-based metasurfaces, we demonstrate that a number of different singularities of nonlinear susceptibilities can exist in the parameter space of twist angle and interlayer gap between different twisted layers. At the singularities, reflected or transmitted light from the nonlinear process (such as second-harmonic generation) can either become circularly polarized (for C points), or entirely vanish (for V points). By further breaking symmetries of the system, we can independently tune all aspects of the reflected and transmitted nonlinear emission, achieving unidirectional emission with full-Poincaré polarization tunability, a dark state ( V − V point), or any other bidirectional output. Our work paves the way for multidimensional control of polarization and directionality in nonlinear light sources, opening new avenues in ultrafast optics, optical communication, sensing, and quantum optics.}, archive = {J_PRL}, author = {Huanyu Zhou and Xueqi Ni and Beicheng Lou and Shanhui Fan and Yuan Cao and Haoning Tang}, doi = {10.1103/PhysRevLett.134.043801}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043801}, shortjournal = {Phys. Rev. Lett.}, title = {Control of chirality and directionality of nonlinear metasurface light source via moiré engineering}, volume = {134}, year = {2025}, }
• (2025). Coherent control of a long-lived nuclear memory spin in a germanium-vacancy multi-qubit node. PRL, 134(4), 043603. (www)

  @article{ , abstract = {The ability to process and store information on surrounding nuclear spins is a major requirement for group-IV color center-based repeater nodes. We demonstrate coherent control of a nuclear spin strongly coupled to a negatively charged germanium-vacancy center in diamond with coherence times beyond 2.5 s at mK temperatures, which is the longest reported for group-IV defects. Detailed analysis allows us to model the system’s dynamics, extract the coupling parameters, and characterize noise. We estimate an achievable memory time of 18.1 s with heating limitations considered, paving the way to successful applications as a quantum repeater node.}, archive = {J_PRL}, author = {Nick Grimm and Katharina Senkalla and Philipp J. Vetter and Jurek Frey and Prithvi Gundlapalli and Tommaso Calarco and Genko Genov and Matthias M. Müller and Fedor Jelezko}, doi = {10.1103/PhysRevLett.134.043603}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043603}, shortjournal = {Phys. Rev. Lett.}, title = {Coherent control of a long-lived nuclear memory spin in a germanium-vacancy multi-qubit node}, volume = {134}, year = {2025}, }
• (2025). Observation of subnatural-linewidth biphotons in a two-level atomic ensemble. PRL, 134(4), 043602. (www)

  @article{ , abstract = {Biphotons and single photons with narrow bandwidths and long coherence times are essential to the realization of long-distance quantum communication (LDQC) and linear optical quantum computing (LOQC). In this Letter, we manipulate the biphoton wave functions of the spontaneous four-wave mixing in a two-level atomic ensemble with a single-laser pump scheme. Our innovative experimental approach enables the generation of biphotons with a sub-MHz bandwidth of 0.36 MHz, a record spectral brightness of 2.28 × 10 7 s − 1 mW − 1 MHz − 1 , and a temporally symmetric wave packet at moderate optical depth. The strong nonclassical cross-correlation of the biphotons also enables the observation of heralded sub-MHz-linewidth single photons with a pronounced single-photon nature. The generation of sub-MHz-linewidth biphotons and single photons with a two-level atomic ensemble not only finds applications in quantum repeaters and large cluster states for LDQC and LOQC but also opens up the opportunity to miniaturize the biphoton or single-photon sources for chip-scale quantum technologies.}, archive = {J_PRL}, author = {Jyun-Kai Lin and Tzu-Hsiang Chien and Chin-Te Wu and Ravikumar Chinnarasu and Shengwang Du and Ite A. Yu and Chih-Sung Chuu}, doi = {10.1103/PhysRevLett.134.043602}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043602}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of subnatural-linewidth biphotons in a two-level atomic ensemble}, volume = {134}, year = {2025}, }
• (2025). Optomechanical dark-mode-breaking cooling. PRL, 134(4), 043601. (www)

  @article{ , abstract = {Optomechanical cooling of multiple degenerate mechanical modes is prevented by the mechanical dark mode due to destructive interference. Here, we report the first experimental demonstration of simultaneous cooling of two near-degenerate mechanical modes by breaking the mechanical dark mode in a two-membrane cavity optomechanical system. The dark mode is generated as the system passes the exceptional point of the anti-parity-time symmetric scheme. By introducing a second cavity mode for the additional dissipative channel, the dark mode is broken and the total phonon number is reduced by more than an order of magnitude below the dark mode cooling limit. Owing to the flexible tunability of the optomechanical coupling rates of such a four-mode coupled system, the optimized cooling efficiency can be achieved by investigating different parameter ranges. Our results provide an important step toward the ground state cooling and entanglement among multiple degenerate mechanical resonators.}, archive = {J_PRL}, author = {Yan Cao and Cheng Yang and Jiteng Sheng and Haibin Wu}, doi = {10.1103/PhysRevLett.134.043601}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043601}, shortjournal = {Phys. Rev. Lett.}, title = {Optomechanical dark-mode-breaking cooling}, volume = {134}, year = {2025}, }
• (2025). Homogeneous fermionic hubbard gases in a flattop optical lattice. PRL, 134(4), 043403. (www)

  @article{ , abstract = {Fermionic atoms in a large-scale, homogeneous optical lattice provide an ideal quantum simulator for investigating the fermionic Hubbard model, yet achieving this remains challenging. Here, by developing a hybrid potential that integrates a flat-top optical lattice with an optical box trap, we successfully realize the creation of three-dimensional, homogeneous fermionic Hubbard gases across approximately lattice sites. This homogeneous system enables us to capture a well-defined energy band occupation that aligns perfectly with the theoretical calculations for a zero-temperature, ideal fermionic Hubbard model. Furthermore, by employing novel radio-frequency spectroscopy, we precisely measure the doublon fraction as a function of interaction strength and temperature , respectively. The crossover from metal to Mott insulator is detected, where smoothly decreases with increasing . More importantly, we observe a nonmonotonic temperature dependence in , revealing the Pomeranchuk effect and the development of extended antiferromagnetic correlations.}, archive = {J_PRL}, author = {Yu-Xuan Wang and Hou-Ji Shao and Yan-Song Zhu and De-Zhi Zhu and Hao-Nan Sun and Si-Yuan Chen and Xing-Can Yao and Yu-Ao Chen and Jian-Wei Pan}, doi = {10.1103/PhysRevLett.134.043403}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043403}, shortjournal = {Phys. Rev. Lett.}, title = {Homogeneous fermionic hubbard gases in a flattop optical lattice}, volume = {134}, year = {2025}, }
• (2025). Shell-shaped quantum droplet in a three-component ultracold bose gas. PRL, 134(4), 043402. (www)

  @article{ , abstract = {Shell-shaped Bose-Einstein condensate is a typical quantum system in curved geometry. Here, we propose a new type of shell-shaped Bose-Einstein condensate with a self-bound character, thereby liberating it from stringent conditions such as microgravity or a fine-tuned trap. Specifically, we consider a three-component (1, 2, 3) ultracold Bose gas where (1, 2) and (2, 3) both form quantum droplets. The two droplets are mutually immiscible due to strong 1–3 repulsion, while still linked by component-2 to form a globally self-bound object. The outer droplet then naturally develops a shell structure without any trapping potential. It is shown that the shell structure can significantly modify the equilibrium density of the core, and lead to unique collective excitations highlighting the core-shell correlation. All results have been demonstrated in a realistic mixture. By extending quantum droplets from flat to curved geometries, this Letter paves the way for future explorations of the interplay of quantum fluctuations and nontrivial real-space topologies in ultracold gases.}, archive = {J_PRL}, author = {Yinfeng Ma and Xiaoling Cui}, doi = {10.1103/PhysRevLett.134.043402}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043402}, shortjournal = {Phys. Rev. Lett.}, title = {Shell-shaped quantum droplet in a three-component ultracold bose gas}, volume = {134}, year = {2025}, }
• (2025). Cold beam optical clock with multifrequency spectroscopy. PRL, 134(4), 043401. (www)

  @article{ , abstract = {We demonstrate an optical clock based on Ramsey-Bordé interferometry in a laser-cooled beam. The mean velocity is reduced by an order of magnitude relative to a thermal beam and the transverse temperature approaches the Doppler limit, enabling the measurement of sub-kHz linewidth fringes in a compact interferometer. Using tailored phase and intensity modulation of the spectroscopy laser to add uniform frequency sidebands, we interrogate atoms throughout the transverse velocity distribution, increasing the Ramsey-Bordé fringe amplitude by a factor of 14 and improving the Allan deviation to at one second averaging time.}, archive = {J_PRL}, author = {William G. Tobias and Bryan Hemingway and Steven Peil}, doi = {10.1103/PhysRevLett.134.043401}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043401}, shortjournal = {Phys. Rev. Lett.}, title = {Cold beam optical clock with multifrequency spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Quantum offset of velocity imaging-based electron spectrometry and the electron affinity of arsenic. PRL, 134(4), 043001. (www)

  @article{ , abstract = {Electron imaging has been routinely used for electron spectrometry. It has been ignored, however, that the maximum-intensity circles that surround electric field-produced electron spots do not materialize envelopes of trajectories, but the first interior fringes of a caustic. Neglecting the gap between the fringe and the parent envelope has resulted in spectrometric errors, notably on some reference values of electron affinities. Evidence for the effect is given by photodetachment microscopy of and a measurement of the electron affinity of , which is found to be 0.804 486(3) eV.}, archive = {J_PRL}, author = {Christophe Blondel and Cyril Drag}, doi = {10.1103/PhysRevLett.134.043001}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {043001}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum offset of velocity imaging-based electron spectrometry and the electron affinity of arsenic}, volume = {134}, year = {2025}, }
• (2025). Prominent bump in the two-neutron separation energies of neutron-rich lanthanum isotopes revealed by high-precision mass spectrometry. PRL, 134(4), 042501. (www)

  @article{ , abstract = {We report on high-precision atomic mass measurements of and performed with the JYFLTRAP double Penning trap using the phase-imaging ion-cyclotron-resonance technique. The masses of were experimentally determined for the first time. We confirm the sharp kink in the two-neutron separation energies at the neutron number in the cerium ( ) isotopic chain. Our precision mass measurements of the most exotic neutron-rich lanthanum ( ) isotopes reveal a unexpected sudden increase in two-neutron separation energies from to . Unlike in the cerium isotopic chain, the kink is not sharp but extends to forming a prominent bump. The gain in energy is about 0.4 MeV, making it one of the strongest changes in two-neutron separation energies over the whole chart of nuclides, away from nuclear shell closures. The results, correlated with a predicted onset of quadrupole deformation for , call for further studies to elucidate the structure of neutron-rich lanthanum isotopes.}, archive = {J_PRL}, author = {A. Jaries and M. Stryjczyk and A. Kankainen and T. Eronen and O. Beliuskina and T. Dickel and M. Flayol and Z. Ge and M. Hukkanen and M. Mougeot and S. Nikas and I. Pohjalainen and A. Raggio and M. Reponen and J. Ruotsalainen and V. Virtanen}, doi = {10.1103/PhysRevLett.134.042501}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {042501}, shortjournal = {Phys. Rev. Lett.}, title = {Prominent bump in the two-neutron separation energies of neutron-rich lanthanum isotopes revealed by high-precision mass spectrometry}, volume = {134}, year = {2025}, }
• (2025). Probing gluonic saturation in deeply virtual meson production beyond leading power. PRL, 134(4), 041901. (www)

  @article{ , abstract = {Exclusive diffractive meson production represents a golden channel for investigating gluonic saturation inside nucleons and nuclei. In this Letter, we settle a systematic framework to deal with beyond leading power corrections at small , including the saturation regime, and obtain the impact factor with both incoming photon and outgoing meson carrying arbitrary polarizations. This is of particular interest since the saturation scale at modern colliders, although entering a perturbative regime, is not large enough to prevent higher-twist effects to be sizable.}, archive = {J_PRL}, author = {Renaud Boussarie and Michael Fucilla and Lech Szymanowski and Samuel Wallon}, doi = {10.1103/PhysRevLett.134.041901}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041901}, shortjournal = {Phys. Rev. Lett.}, title = {Probing gluonic saturation in deeply virtual meson production beyond leading power}, volume = {134}, year = {2025}, }
• (2025). Early universe hypercharge breaking and neutrino mass generation. PRL, 134(4), 041802. (www)

  @article{ , abstract = {We show that the conditions allowing for a spontaneous breaking of the hypercharge gauge symmetry of the standard model (SM) in the early Universe are generically present in extensions of the SM addressing the generation of light neutrino masses via radiative contributions. In such scenarios, the breaking of (hyper)charge at high temperatures yields new possibilities for explaining the observed matter-antimatter asymmetry of the Universe. Considering for concreteness the Zee-Babu radiative neutrino mass generation model, we show that a period of hypercharge breaking prior to the electroweak phase transition could allow for successful baryogenesis via a nonconventional leptogenesis mechanism, based on the presence of charge-breaking masses for the SM leptons in the early Universe.}, archive = {J_PRL}, author = {S. López-Zurdo and A. Lozano-Onrubia and L. Merlo and J. M. No}, doi = {10.1103/PhysRevLett.134.041802}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041802}, shortjournal = {Phys. Rev. Lett.}, title = {Early universe hypercharge breaking and neutrino mass generation}, volume = {134}, year = {2025}, }
• (2025). Search for new resonances decaying to pairs of merged diphotons in proton-proton collisions at s=13 TeV. PRL, 134(4), 041801. (www)

  @article{ , abstract = {A search is presented for an extended Higgs sector with two new particles, and , in the process . Novel neural networks classify events with diphotons that are merged and determine the diphoton masses. The search uses LHC proton-proton collision data at collected with the CMS detector, corresponding to an integrated luminosity of . No evidence of such resonances is seen. Upper limits are set on the production cross section for between 300 and 3000 GeV and between 0.5% and 2.5%, representing the most sensitive search in this channel.}, archive = {J_PRL}, author = {CMS Collaboration and A. Hayrapetyan and A. Tumasyan and W. Adam and J. W. Andrejkovic and T. Bergauer and S. Chatterjee and K. Damanakis and M. Dragicevic and P. S. Hussain and M. Jeitler and N. Krammer and A. Li and D. Liko and I. Mikulec and J. Schieck and R. Schöfbeck and D. Schwarz and M. Sonawane and S. Templ and W. Waltenberger and C.-E. Wulz and M. R. Darwish and T. Janssen and P. Van Mechelen and E. S. Bols and J. D’Hondt and S. Dansana and A. De Moor and M. Delcourt and S. Lowette and I. Makarenko and D. Müller and S. Tavernier and M. Tytgat and G. P. Van Onsem and S. Van Putte and D. Vannerom and B. Clerbaux and A. K. Das and G. De Lentdecker and H. Evard and L. Favart and P. Gianneios and D. Hohov and J. Jaramillo and A. Khalilzadeh and F. A. Khan and K. Lee and M. Mahdavikhorrami and A. Malara and S. Paredes and L. Thomas and M. Vanden Bemden and C. Vander Velde and P. Vanlaer and M. De Coen and D. Dobur and Y. Hong and J. Knolle and L. Lambrecht and G. Mestdach and K. Mota Amarilo and C. Rendón and A. Samalan and K. Skovpen and N. Van Den Bossche and J. van der Linden and L. Wezenbeek and A. Benecke and A. Bethani and G. Bruno and C. Caputo and C. Delaere and I. S. Donertas and A. Giammanco and Sa. Jain and V. Lemaitre and J. Lidrych and P. Mastrapasqua and T. T. Tran and S. Wertz and G. A. Alves and E. Coelho and C. Hensel and T. Menezes De Oliveira and A. Moraes and P. Rebello Teles and M. Soeiro and W. L. Aldá Júnior and M. Alves Gallo Pereira and M. Barroso Ferreira Filho and H. Brandao Malbouisson and W. Carvalho and J. Chinellato and E. M. Da Costa and G. G. Da Silveira and D. De Jesus Damiao and S. Fonseca De Souza and R. Gomes De Souza and M. Macedo and J. Martins and C. Mora Herrera and L. Mundim and H. Nogima and J. P. Pinheiro and A. Santoro and A. Sznajder and M. Thiel and A. Vilela Pereira and C. A. Bernardes and L. Calligaris and T. R. Fernandez Perez Tomei and E. M. Gregores and P. G. Mercadante and S. F. Novaes and B. Orzari and Sandra S. Padula and A. Aleksandrov and G. Antchev and R. Hadjiiska and P. Iaydjiev and M. Misheva and M. Shopova and G. Sultanov and A. Dimitrov and L. Litov and B. Pavlov and P. Petkov and A. Petrov and E. Shumka and S. Keshri and S. Thakur and T. Cheng and T. Javaid and L. Yuan and Z. Hu and J. Liu and K. Yi and G. M. Chen and H. S. Chen and M. Chen and F. Iemmi and C. H. Jiang and A. Kapoor and H. Liao and Z.-A. Liu and R. Sharma and J. N. Song and J. Tao and C. Wang and J. Wang and Z. Wang and H. Zhang and A. Agapitos and Y. Ban and A. Levin and C. Li and Q. Li and Y. Mao and S. J. Qian and X. Sun and D. Wang and H. Yang and L. Zhang and C. Zhou and Z. You and K. Jaffel and N. Lu and G. Bauer and X. Gao and Z. Lin and C. Lu and M. Xiao and C. Avila and D. A. Barbosa Trujillo and A. Cabrera and C. Florez and J. Fraga and J. A. Reyes Vega and J. Mejia Guisao and F. Ramirez and M. Rodriguez and J. D. Ruiz Alvarez and D. Giljanovic and N. Godinovic and D. Lelas and A. Sculac and M. Kovac and T. Sculac and P. Bargassa and V. Brigljevic and B. K. Chitroda and D. Ferencek and K. Jakovcic and S. Mishra and A. Starodumov and T. Susa and A. Attikis and K. Christoforou and A. Hadjiagapiou and J. Mousa and C. Nicolaou and L. Paizanos and F. Ptochos and P. A. Razis and H. Rykaczewski and H. Saka and A. Stepennov and M. Finger and M. Finger, Jr and A. Kveton and E. Ayala and E. Carrera Jarrin and Y. Assran and S. Elgammal and M. A. Mahmoud and Y. Mohammed and K. Ehataht and M. Kadastik and T. Lange and S. Nandan and C. Nielsen and J. Pata and M. Raidal and L. Tani and C. Veelken and H. Kirschenmann and K. Osterberg and M. Voutilainen and S. Bharthuar and E. Brücken and F. Garcia and K. T. S. Kallonen and R. Kinnunen and T. Lampén and K. Lassila-Perini and S. Lehti and T. Lindén and L. Martikainen and M. Myllymäki and M. m. Rantanen and H. Siikonen and E. Tuominen and J. Tuominiemi and P. Luukka and H. Petrow and M. Besancon and F. Couderc and M. Dejardin and D. Denegri and J. L. Faure and F. Ferri and S. Ganjour and P. Gras and G. Hamel de Monchenault and V. Lohezic and J. Malcles and F. Orlandi and L. Portales and J. Rander and A. Rosowsky and M. Ö. Sahin and A. Savoy-Navarro and P. Simkina and M. Titov and M. Tornago and F. Beaudette and A. Buchot Perraguin and P. Busson and A. Cappati and C. Charlot and M. Chiusi and F. Damas and O. Davignon and A. De Wit and I. T. Ehle and B. A. Fontana Santos Alves and S. Ghosh and A. Gilbert and R. Granier de Cassagnac and A. Hakimi and B. Harikrishnan and L. Kalipoliti and G. Liu and J. Motta and M. Nguyen and C. Ochando and R. Salerno and J. B. Sauvan and Y. Sirois and A. Tarabini and E. Vernazza and A. Zabi and A. Zghiche and J.-L. Agram and J. Andrea and D. Apparu and D. Bloch and J.-M. Brom and E. C. Chabert and C. Collard and S. Falke and U. Goerlach and C. Grimault and R. Haeberle and A.-C. Le Bihan and M. Meena and G. Saha and M. A. Sessini and P. Van Hove and S. Beauceron and B. Blancon and G. Boudoul and N. Chanon and D. Contardo and P. Depasse and C. Dozen and H. El Mamouni and J. Fay and S. Gascon and M. Gouzevitch and C. Greenberg and G. Grenier and B. Ille and I. B. Laktineh and M. Lethuillier and L. Mirabito and S. Perries and A. Purohit and M. Vander Donckt and P. Verdier and J. Xiao and G. Adamov and I. Lomidze and Z. Tsamalaidze and V. Botta and L. Feld and K. Klein and M. Lipinski and D. Meuser and A. Pauls and N. Röwert and M. Teroerde and S. Diekmann and A. Dodonova and N. Eich and D. Eliseev and F. Engelke and J. Erdmann and M. Erdmann and P. Fackeldey and B. Fischer and T. Hebbeker and K. Hoepfner and F. Ivone and A. Jung and M. y. Lee and F. Mausolf and M. Merschmeyer and A. Meyer and S. Mukherjee and D. Noll and F. Nowotny and A. Pozdnyakov and Y. Rath and W. Redjeb and F. Rehm and H. Reithler and U. Sarkar and V. Sarkisovi and A. Schmidt and A. Sharma and J. L. Spah and A. Stein and F. Torres Da Silva De Araujo and S. Wiedenbeck and S. Zaleski and C. Dziwok and G. Flügge and W. Haj Ahmad and T. Kress and A. Nowack and O. Pooth and A. Stahl and T. Ziemons and A. Zotz and H. Aarup Petersen and M. Aldaya Martin and J. Alimena and S. Amoroso and Y. An and S. Baxter and M. Bayatmakou and H. Becerril Gonzalez and O. Behnke and A. Belvedere and S. Bhattacharya and F. Blekman and K. Borras and A. Campbell and A. Cardini and C. Cheng and F. Colombina and S. Consuegra Rodríguez and G. Correia Silva and M. De Silva and G. Eckerlin and D. Eckstein and L. I. Estevez Banos and O. Filatov and E. Gallo and A. Geiser and A. Giraldi and V. Guglielmi and M. Guthoff and A. Hinzmann and A. Jafari and L. Jeppe and B. Kaech and M. Kasemann and C. Kleinwort and R. Kogler and M. Komm and D. Krücker and W. Lange and D. Leyva Pernia and K. Lipka and W. Lohmann and F. Lorkowski and R. Mankel and I.-A. Melzer-Pellmann and M. Mendizabal Morentin and A. B. Meyer and G. Milella and A. Mussgiller and L. P. Nair and A. Nürnberg and Y. Otarid and J. Park and D. Pérez Adán and E. Ranken and A. Raspereza and D. Rastorguev and B. Ribeiro Lopes and J. Rübenach and A. Saggio and M. Scham and S. Schnake and P. Schütze and C. Schwanenberger and D. Selivanova and K. Sharko and M. Shchedrolosiev and R. E. Sosa Ricardo and D. Stafford and F. Vazzoler and A. Ventura Barroso and R. Walsh and Q. Wang and Y. Wen and K. Wichmann and L. Wiens and C. Wissing and Y. Yang and A. Zimermmane Castro Santos and A. Albrecht and S. Albrecht and M. Antonello and S. Bein and L. Benato and S. Bollweg and M. Bonanomi and P. Connor and K. El Morabit and Y. Fischer and E. Garutti and A. Grohsjean and J. Haller and H. R. Jabusch and G. Kasieczka and P. Keicher and R. Klanner and W. Korcari and T. Kramer and V. Kutzner and F. Labe and J. Lange and A. Lobanov and C. Matthies and L. Moureaux and M. Mrowietz and A. Nigamova and Y. Nissan and A. Paasch and K. J. Pena Rodriguez and T. Quadfasel and B. Raciti and M. Rieger and D. Savoiu and J. Schindler and P. Schleper and M. Schröder and J. Schwandt and M. Sommerhalder and H. Stadie and G. Steinbrück and A. Tews and M. Wolf and S. Brommer and M. Burkart and E. Butz and T. Chwalek and A. Dierlamm and A. Droll and N. Faltermann and M. Giffels and A. Gottmann and F. Hartmann and R. Hofsaess and M. Horzela and U. Husemann and J. Kieseler and M. Klute and R. Koppenhöfer and J. M. Lawhorn and M. Link and A. Lintuluoto and B. Maier and S. Maier and S. Mitra and M. Mormile and Th. Müller and M. Neukum and M. Oh and E. Pfeffer and M. Presilla and G. Quast and K. Rabbertz and B. Regnery and N. Shadskiy and I. Shvetsov and H. J. Simonis and M. Toms and N. Trevisani and R. F. Von Cube and M. Wassmer and S. Wieland and F. Wittig and R. Wolf and X. Zuo and G. Anagnostou and G. Daskalakis and A. Kyriakis and A. Papadopoulos and A. Stakia and P. Kontaxakis and G. Melachroinos and Z. Painesis and A. Panagiotou and I. Papavergou and I. Paraskevas and N. Saoulidou and K. Theofilatos and E. Tziaferi and K. Vellidis and I. Zisopoulos and G. Bakas and T. Chatzistavrou and G. Karapostoli and K. Kousouris and I. Papakrivopoulos and E. Siamarkou and G. Tsipolitis and A. Zacharopoulou and K. Adamidis and I. Bestintzanos and I. Evangelou and C. Foudas and C. Kamtsikis and P. Katsoulis and P. Kokkas and P. G. Kosmoglou Kioseoglou and N. Manthos and I. Papadopoulos and J. Strologas and M. Bartók and C. Hajdu and D. Horvath and K. Márton and A. J. Rádl and F. Sikler and V. Veszpremi and M. Csanád and K. Farkas and M. M. A. Gadallah and Á. Kadlecsik and P. Major and K. Mandal and G. Pásztor and G. I. Veres and P. Raics and B. Ujvari and G. Zilizi and G. Bencze and S. Czellar and J. Molnar and Z. Szillasi and T. Csorgo and F. Nemes and T. Novak and J. Babbar and S. Bansal and S. B. Beri and V. Bhatnagar and G. Chaudhary and S. Chauhan and N. Dhingra and A. Kaur and H. Kaur and M. Kaur and S. Kumar and K. Sandeep and T. Sheokand and J. B. Singh and A. Singla and A. Ahmed and A. Bhardwaj and A. Chhetri and B. C. Choudhary and A. Kumar and M. Naimuddin and K. Ranjan and S. Saumya and S. Baradia and S. Barman and S. Dutta and S. Sarkar and M. M. Ameen and P. K. Behera and S. C. Behera and P. Jana and P. Kalbhor and J. R. Komaragiri and D. Kumar and P. R. Pujahari and N. R. Saha and A. K. Sikdar and S. Verma and S. Dugad and M. Kumar and G. B. Mohanty and P. Suryadevara and A. Bala and S. Banerjee and R. M. Chatterjee and R. K. Dewanjee and M. Guchait and Sh. Jain and A. Jaiswal and G. Majumder and K. Mazumdar and S. Parolia and A. Thachayath and S. Bahinipati and C. Kar and D. Maity and P. Mal and T. Mishra and V. K. Muraleedharan Nair Bindhu and K. Naskar and A. Nayak and P. Sadangi and S. K. Swain and S. Varghese and D. Vats and S. Acharya and A. Alpana and S. Dube and B. Gomber and P. Hazarika and B. Kansal and A. Laha and B. Sahu and S. Sharma and K. Y. Vaish and H. Bakhshiansohi and E. Khazaie and M. Zeinali and S. Bashiri and S. Chenarani and S. M. Etesami and M. Khakzad and M. Mohammadi Najafabadi and S. Tizchang and M. Grunewald and M. Abbrescia and R. Aly and A. Colaleo and D. Creanza and B. D’Anzi and N. De Filippis and M. De Palma and A. Di Florio and W. Elmetenawee and L. Fiore and G. Iaselli and M. Louka and G. Maggi and M. Maggi and I. Margjeka and V. Mastrapasqua and S. My and S. Nuzzo and A. Pellecchia and A. Pompili and G. Pugliese and R. Radogna and G. Ramirez-Sanchez and D. Ramos and A. Ranieri and L. Silvestris and F. M. Simone and Ü. Sözbilir and A. Stamerra and R. Venditti and P. Verwilligen and A. Zaza and G. Abbiendi and C. Battilana and D. Bonacorsi and L. Borgonovi and P. Capiluppi and A. Castro and F. R. Cavallo and M. Cuffiani and G. M. Dallavalle and T. Diotalevi and F. Fabbri and A. Fanfani and D. Fasanella and P. Giacomelli and L. Giommi and C. Grandi and L. Guiducci and S. Lo Meo and L. Lunerti and S. Marcellini and G. Masetti and F. L. Navarria and A. Perrotta and F. Primavera and A. M. Rossi and T. Rovelli and G. P. Siroli and S. Costa and A. Di Mattia and R. Potenza and A. Tricomi and C. Tuve and P. Assiouras and G. Barbagli and G. Bardelli and B. Camaiani and A. Cassese and R. Ceccarelli and V. Ciulli and C. Civinini and R. D’Alessandro and E. Focardi and T. Kello and G. Latino and P. Lenzi and M. Lizzo and M. Meschini and S. Paoletti and A. Papanastassiou and G. Sguazzoni and L. Viliani and L. Benussi and S. Bianco and S. Meola and D. Piccolo and P. Chatagnon and F. Ferro and E. Robutti and S. Tosi and A. Benaglia and G. Boldrini and F. Brivio and F. Cetorelli and F. De Guio and M. E. Dinardo and P. Dini and S. Gennai and R. Gerosa and A. Ghezzi and P. Govoni and L. Guzzi and M. T. Lucchini and M. Malberti and S. Malvezzi and A. Massironi and D. Menasce and L. Moroni and M. Paganoni and S. Palluotto and D. Pedrini and B. S. Pinolini and G. Pizzati and S. Ragazzi and T. Tabarelli de Fatis and S. Buontempo and A. Cagnotta and F. Carnevali and N. Cavallo and F. Fabozzi and A. O. M. Iorio and L. Lista and P. Paolucci and B. Rossi and C. Sciacca and R. Ardino and P. Azzi and N. Bacchetta and M. Biasotto and D. Bisello and P. Bortignon and G. Bortolato and A. Bragagnolo and A. C. M. Bulla and R. Carlin and P. Checchia and T. Dorigo and F. Gasparini and U. Gasparini and E. Lusiani and M. Margoni and F. Marini and M. Migliorini and J. Pazzini and P. Ronchese and R. Rossin and F. Simonetto and G. Strong and M. Tosi and A. Triossi and S. Ventura and M. Zanetti and P. Zotto and A. Zucchetta and G. Zumerle and S. Abu Zeid and C. Aimè and A. Braghieri and S. Calzaferri and D. Fiorina and P. Montagna and V. Re and C. Riccardi and P. Salvini and I. Vai and P. Vitulo and S. Ajmal and G. M. Bilei and D. Ciangottini and L. Fanò and M. Magherini and V. Mariani and M. Menichelli and F. Moscatelli and A. Rossi and A. Santocchia and D. Spiga and T. Tedeschi and P. Asenov and P. Azzurri and G. Bagliesi and R. Bhattacharya and L. Bianchini and T. Boccali and E. Bossini and D. Bruschini and R. Castaldi and M. A. Ciocci and M. Cipriani and V. D’Amante and R. Dell’Orso and S. Donato and A. Giassi and F. Ligabue and D. Matos Figueiredo and A. Messineo and M. Musich and F. Palla and A. Rizzi and G. Rolandi and S. Roy Chowdhury and T. Sarkar and A. Scribano and P. Spagnolo and R. Tenchini and G. Tonelli and N. Turini and F. Vaselli and A. Venturi and P. G. Verdini and C. Baldenegro Barrera and P. Barria and C. Basile and M. Campana and F. Cavallari and L. Cunqueiro Mendez and D. Del Re and E. Di Marco and M. Diemoz and F. Errico and E. Longo and P. Meridiani and J. Mijuskovic and G. Organtini and F. Pandolfi and R. Paramatti and C. Quaranta and S. Rahatlou and C. Rovelli and F. Santanastasio and L. Soffi and N. Amapane and R. Arcidiacono and S. Argiro and M. Arneodo and N. Bartosik and R. Bellan and A. Bellora and C. Biino and C. Borca and N. Cartiglia and M. Costa and R. Covarelli and N. Demaria and L. Finco and M. Grippo and B. Kiani and F. Legger and F. Luongo and C. Mariotti and L. Markovic and S. Maselli and A. Mecca and E. Migliore and M. Monteno and R. Mulargia and M. M. Obertino and G. Ortona and L. Pacher and N. Pastrone and M. Pelliccioni and M. Ruspa and F. Siviero and V. Sola and A. Solano and A. Staiano and C. Tarricone and D. Trocino and G. Umoret and E. Vlasov and R. White and S. Belforte and V. Candelise and M. Casarsa and F. Cossutti and K. De Leo and G. Della Ricca and S. Dogra and J. Hong and C. Huh and B. Kim and D. H. Kim and J. Kim and H. Lee and S. W. Lee and C. S. Moon and Y. D. Oh and M. S. Ryu and S. Sekmen and Y. C. Yang and M. S. Kim and G. Bak and P. Gwak and H. Kim and D. H. Moon and E. Asilar and J. Choi and D. Kim and T. J. Kim and J. A. Merlin and S. Choi and S. Han and B. Hong and K. S. Lee and S. Lee and S. K. Park and J. Yoo and J. Goh and S. Yang and H. S. Kim and Y. Kim and J. Almond and J. H. Bhyun and W. Jun and S. Ko and H. Kwon and J. Lee and B. H. Oh and S. B. Oh and H. Seo and U. K. Yang and I. Yoon and W. Jang and D. Y. Kang and Y. Kang and S. Kim and B. Ko and J. S. H. Lee and Y. Lee and I. C. Park and Y. Roh and I. J. Watson and S. Ha and H. D. Yoo and M. Choi and M. R. Kim and I. Yu and T. Beyrouthy and K. Dreimanis and A. Gaile and G. Pikurs and A. Potrebko and M. Seidel and N. R. Strautnieks and M. Ambrozas and A. Juodagalvis and A. Rinkevicius and G. Tamulaitis and N. Bin Norjoharuddeen and I. Yusuff and Z. Zolkapli and J. F. Benitez and A. Castaneda Hernandez and H. A. Encinas Acosta and L. G. Gallegos Maríñez and M. León Coello and J. A. Murillo Quijada and A. Sehrawat and L. Valencia Palomo and G. Ayala and H. Castilla-Valdez and H. Crotte Ledesma and E. De La Cruz-Burelo and I. Heredia-De La Cruz and R. Lopez-Fernandez and C. A. Mondragon Herrera and A. Sánchez Hernández and C. Oropeza Barrera and M. Ramírez García and I. Bautista and I. Pedraza and H. A. Salazar Ibarguen and C. Uribe Estrada and I. Bubanja and N. Raicevic and P. H. Butler and A. Ahmad and M. I. Asghar and A. Awais and M. I. M. Awan and H. R. Hoorani and W. A. Khan and V. Avati and L. Grzanka and M. Malawski and H. Bialkowska and M. Bluj and B. Boimska and M. Górski and M. Kazana and M. Szleper and P. Zalewski and K. Bunkowski and K. Doroba and A. Kalinowski and M. Konecki and J. Krolikowski and A. Muhammad and K. Pozniak and W. Zabolotny and M. Araujo and D. Bastos and C. Beirão Da Cruz E Silva and A. Boletti and M. Bozzo and T. Camporesi and G. Da Molin and P. Faccioli and M. Gallinaro and J. Hollar and N. Leonardo and T. Niknejad and A. Petrilli and M. Pisano and J. Seixas and J. Varela and J. W. Wulff and P. Adzic and P. Milenovic and M. Dordevic and J. Milosevic and V. Rekovic and M. Aguilar-Benitez and J. Alcaraz Maestre and Cristina F. Bedoya and Oliver M. Carretero and M. Cepeda and M. Cerrada and N. Colino and B. De La Cruz and A. Delgado Peris and A. Escalante Del Valle and D. Fernández Del Val and J. P. Fernández Ramos and J. Flix and M. C. Fouz and O. Gonzalez Lopez and S. Goy Lopez and J. M. Hernandez and M. I. Josa and D. Moran and C. M. Morcillo Perez and Á. Navarro Tobar and C. Perez Dengra and A. Pérez-Calero Yzquierdo and J. Puerta Pelayo and I. Redondo and D. D. Redondo Ferrero and L. Romero and S. Sánchez Navas and L. Urda Gómez and J. Vazquez Escobar and C. Willmott and J. F. de Trocóniz and B. Alvarez Gonzalez and J. Cuevas and J. Fernandez Menendez and S. Folgueras and I. Gonzalez Caballero and J. R. González Fernández and P. Leguina and E. Palencia Cortezon and C. Ramón Álvarez and V. Rodríguez Bouza and A. Soto Rodríguez and A. Trapote and C. Vico Villalba and P. Vischia and S. Bhowmik and S. Blanco Fernández and J. A. Brochero Cifuentes and I. J. Cabrillo and A. Calderon and J. Duarte Campderros and M. Fernandez and G. Gomez and C. Lasaosa García and R. Lopez Ruiz and C. Martinez Rivero and P. Martinez Ruiz del Arbol and F. Matorras and P. Matorras Cuevas and E. Navarrete Ramos and J. Piedra Gomez and L. Scodellaro and I. Vila and J. M. Vizan Garcia and M. K. Jayananda and B. Kailasapathy and D. U. J. Sonnadara and D. D. C. Wickramarathna and W. G. D. Dharmaratna and K. Liyanage and N. Perera and N. Wickramage and D. Abbaneo and C. Amendola and E. Auffray and G. Auzinger and J. Baechler and D. Barney and A. Bermúdez Martínez and M. Bianco and B. Bilin and A. A. Bin Anuar and A. Bocci and C. Botta and E. Brondolin and C. Caillol and G. Cerminara and N. Chernyavskaya and D. d’Enterria and A. Dabrowski and A. David and A. De Roeck and M. M. Defranchis and M. Deile and M. Dobson and L. Forthomme and G. Franzoni and W. Funk and S. Giani and D. Gigi and K. Gill and F. Glege and L. Gouskos and M. Haranko and J. Hegeman and B. Huber and V. Innocente and T. James and P. Janot and O. Kaluzinska and S. Laurila and P. Lecoq and E. Leutgeb and C. Lourenço and L. Malgeri and M. Mannelli and A. C. Marini and M. Matthewman and A. Mehta and F. Meijers and S. Mersi and E. Meschi and V. Milosevic and F. Monti and F. Moortgat and M. Mulders and I. Neutelings and S. Orfanelli and F. Pantaleo and G. Petrucciani and A. Pfeiffer and M. Pierini and D. Piparo and H. Qu and D. Rabady and M. Rovere and H. Sakulin and S. Scarfi and C. Schwick and M. Selvaggi and K. Shchelina and P. Silva and P. Sphicas and A. G. Stahl Leiton and A. Steen and S. Summers and D. Treille and P. Tropea and A. Tsirou and D. Walter and J. Wanczyk and S. Wuchterl and P. Zehetner and P. Zejdl and W. D. Zeuner and T. Bevilacqua and L. Caminada and A. Ebrahimi and W. Erdmann and R. Horisberger and Q. Ingram and H. C. Kaestli and D. Kotlinski and C. Lange and M. Missiroli and L. Noehte and T. Rohe and T. K. Aarrestad and K. Androsov and M. Backhaus and G. Bonomelli and A. Calandri and C. Cazzaniga and K. Datta and A. De Cosa and G. Dissertori and M. Dittmar and M. Donegà and F. Eble and M. Galli and K. Gedia and F. Glessgen and C. Grab and N. Härringer and T. G. Harte and D. Hits and W. Lustermann and A.-M. Lyon and R. A. Manzoni and M. Marchegiani and L. Marchese and C. Martin Perez and A. Mascellani and F. Nessi-Tedaldi and F. Pauss and V. Perovic and S. Pigazzini and C. Reissel and T. Reitenspiess and B. Ristic and F. Riti and R. Seidita and J. Steggemann and D. Valsecchi and R. Wallny and C. Amsler and P. Bärtschi and M. F. Canelli and K. Cormier and J. K. Heikkilä and M. Huwiler and W. Jin and A. Jofrehei and B. Kilminster and S. Leontsinis and S. P. Liechti and A. Macchiolo and P. Meiring and U. Molinatti and A. Reimers and P. Robmann and S. Sanchez Cruz and M. Senger and E. Shokr and F. Stäger and Y. Takahashi and R. Tramontano and C. Adloff and D. Bhowmik and C. M. Kuo and W. Lin and P. K. Rout and P. C. Tiwari and S. S. Yu and L. Ceard and Y. Chao and K. F. Chen and P. s. Chen and Z. g. Chen and A. De Iorio and W.-S. Hou and T. h. Hsu and Y. w. Kao and S. Karmakar and R. Khurana and G. Kole and Y. y. Li and R.-S. Lu and E. Paganis and X. f. Su and J. Thomas-Wilsker and L. s. Tsai and H. y. Wu and E. Yazgan and C. Asawatangtrakuldee and N. Srimanobhas and V. Wachirapusitanand and D. Agyel and F. Boran and Z. S. Demiroglu and F. Dolek and I. Dumanoglu and E. Eskut and Y. Guler and E. Gurpinar Guler and C. Isik and O. Kara and A. Kayis Topaksu and U. Kiminsu and G. Onengut and K. Ozdemir and A. Polatoz and B. Tali and U. G. Tok and S. Turkcapar and E. Uslan and I. S. Zorbakir and G. Sokmen and M. Yalvac and B. Akgun and I. O. Atakisi and E. Gülmez and M. Kaya and O. Kaya and S. Tekten and A. Cakir and K. Cankocak and G. G. Dincer and Y. Komurcu and S. Sen and O. Aydilek and S. Cerci and V. Epshteyn and B. Hacisahinoglu and I. Hos and B. Kaynak and S. Ozkorucuklu and O. Potok and H. Sert and C. Simsek and C. Zorbilmez and B. Isildak and D. Sunar Cerci and A. Boyaryntsev and B. Grynyov and L. Levchuk and D. Anthony and J. J. Brooke and A. Bundock and F. Bury and E. Clement and D. Cussans and H. Flacher and M. Glowacki and J. Goldstein and H. F. Heath and M.-L. Holmberg and L. Kreczko and S. Paramesvaran and L. Robertshaw and S. Seif El Nasr-Storey and V. J. Smith and N. Stylianou and K. Walkingshaw Pass and A. H. Ball and K. W. Bell and A. Belyaev and C. Brew and R. M. Brown and D. J. A. Cockerill and C. Cooke and K. V. Ellis and K. Harder and S. Harper and J. Linacre and K. Manolopoulos and D. M. Newbold and E. Olaiya and D. Petyt and T. Reis and A. R. Sahasransu and G. Salvi and T. Schuh and C. H. Shepherd-Themistocleous and I. R. Tomalin and T. Williams and R. Bainbridge and P. Bloch and C. E. Brown and O. Buchmuller and V. Cacchio and C. A. Carrillo Montoya and G. S. Chahal and D. Colling and J. S. Dancu and I. Das and P. Dauncey and G. Davies and J. Davies and M. Della Negra and S. Fayer and G. Fedi and G. Hall and M. H. Hassanshahi and A. Howard and G. Iles and M. Knight and J. Langford and J. León Holgado and L. Lyons and A.-M. Magnan and S. Malik and M. Mieskolainen and J. Nash and M. Pesaresi and B. C. Radburn-Smith and A. Richards and A. Rose and K. Savva and C. Seez and R. Shukla and A. Tapper and K. Uchida and G. P. Uttley and L. H. Vage and T. Virdee and M. Vojinovic and N. Wardle and D. Winterbottom and K. Coldham and J. E. Cole and A. Khan and P. Kyberd and I. D. Reid and S. Abdullin and A. Brinkerhoff and B. Caraway and E. Collins and J. Dittmann and K. Hatakeyama and J. Hiltbrand and B. McMaster and S. Sawant and C. Sutantawibul and J. Wilson and R. Bartek and A. Dominguez and C. Huerta Escamilla and A. E. Simsek and R. Uniyal and A. M. Vargas Hernandez and B. Bam and R. Chudasama and S. I. Cooper and S. V. Gleyzer and C. U. Perez and P. Rumerio and E. Usai and R. Yi and A. Akpinar and D. Arcaro and C. Cosby and Z. Demiragli and C. Erice and C. Fangmeier and C. Fernandez Madrazo and E. Fontanesi and D. Gastler and F. Golf and S. Jeon and I. Reed and J. Rohlf and K. Salyer and D. Sperka and D. Spitzbart and I. Suarez and A. Tsatsos and S. Yuan and A. G. Zecchinelli and G. Benelli and X. Coubez and D. Cutts and M. Hadley and U. Heintz and J. M. Hogan and T. Kwon and G. Landsberg and K. T. Lau and D. Li and J. Luo and S. Mondal and M. Narain and N. Pervan and S. Sagir and F. Simpson and M. Stamenkovic and N. Venkatasubramanian and X. Yan and W. Zhang and S. Abbott and J. Bonilla and C. Brainerd and R. Breedon and H. Cai and M. Calderon De La Barca Sanchez and M. Chertok and M. Citron and J. Conway and P. T. Cox and R. Erbacher and F. Jensen and O. Kukral and G. Mocellin and M. Mulhearn and D. Pellett and W. Wei and Y. Yao and F. Zhang and M. Bachtis and R. Cousins and A. Datta and G. Flores Avila and J. Hauser and M. Ignatenko and M. A. Iqbal and T. Lam and E. Manca and A. Nunez Del Prado and D. Saltzberg and V. Valuev and R. Clare and J. W. Gary and M. Gordon and G. Hanson and W. Si and S. Wimpenny and J. G. Branson and S. Cittolin and S. Cooperstein and D. Diaz and J. Duarte and L. Giannini and J. Guiang and R. Kansal and V. Krutelyov and R. Lee and J. Letts and M. Masciovecchio and F. Mokhtar and M. Pieri and M. Quinnan and B. V. Sathia Narayanan and V. Sharma and M. Tadel and E. Vourliotis and F. Würthwein and Y. Xiang and A. Yagil and A. Barzdukas and L. Brennan and C. Campagnari and J. Incandela and A. J. Li and P. Masterson and H. Mei and J. Richman and U. Sarica and R. Schmitz and F. Setti and J. Sheplock and D. Stuart and T. Á. Vámi and S. Wang and A. Bornheim and O. Cerri and A. Latorre and J. Mao and H. B. Newman and G. Reales Gutiérrez and M. Spiropulu and J. R. Vlimant and S. Xie and R. Y. Zhu and J. Alison and S. An and M. B. Andrews and P. Bryant and M. Cremonesi and V. Dutta and T. Ferguson and A. Harilal and C. Liu and T. Mudholkar and S. Murthy and P. Palit and M. Paulini and A. Roberts and A. Sanchez and W. Terrill and J. P. Cumalat and W. T. Ford and A. Hart and A. Hassani and G. Karathanasis and N. Manganelli and A. Perloff and C. Savard and N. Schonbeck and K. Stenson and K. A. Ulmer and S. R. Wagner and N. Zipper and D. Zuolo and J. Alexander and S. Bright-Thonney and X. Chen and D. J. Cranshaw and J. Fan and X. Fan and S. Hogan and P. Kotamnives and J. Monroy and M. Oshiro and J. R. Patterson and J. Reichert and M. Reid and A. Ryd and J. Thom and P. Wittich and R. Zou and M. Albrow and M. Alyari and O. Amram and G. Apollinari and A. Apresyan and L. A. T. Bauerdick and D. Berry and J. Berryhill and P. C. Bhat and K. Burkett and J. N. Butler and A. Canepa and G. B. Cerati and H. W. K. Cheung and F. Chlebana and G. Cummings and J. Dickinson and I. Dutta and V. D. Elvira and Y. Feng and J. Freeman and A. Gandrakota and Z. Gecse and L. Gray and D. Green and A. Grummer and S. Grünendahl and D. Guerrero and O. Gutsche and R. M. Harris and R. Heller and T. C. Herwig and J. Hirschauer and L. Horyn and B. Jayatilaka and S. Jindariani and M. Johnson and U. Joshi and T. Klijnsma and B. Klima and K. H. M. Kwok and S. Lammel and D. Lincoln and R. Lipton and T. Liu and C. Madrid and K. Maeshima and C. Mantilla and D. Mason and P. McBride and P. Merkel and S. Mrenna and S. Nahn and J. Ngadiuba and D. Noonan and V. Papadimitriou and N. Pastika and K. Pedro and C. Pena and F. Ravera and A. Reinsvold Hall and L. Ristori and E. Sexton-Kennedy and N. Smith and A. Soha and L. Spiegel and S. Stoynev and J. Strait and L. Taylor and S. Tkaczyk and N. V. Tran and L. Uplegger and E. W. Vaandering and A. Whitbeck and I. Zoi and C. Aruta and P. Avery and D. Bourilkov and L. Cadamuro and P. Chang and V. Cherepanov and R. D. Field and E. Koenig and M. Kolosova and J. Konigsberg and A. Korytov and K. Matchev and N. Menendez and G. Mitselmakher and K. Mohrman and A. Muthirakalayil Madhu and N. Rawal and D. Rosenzweig and S. Rosenzweig and T. Adams and A. Al Kadhim and A. Askew and S. Bower and R. Habibullah and V. Hagopian and R. Hashmi and R. S. Kim and T. Kolberg and G. Martinez and H. Prosper and P. R. Prova and M. Wulansatiti and R. Yohay and J. Zhang and B. Alsufyani and M. M. Baarmand and S. Butalla and S. Das and T. Elkafrawy and M. Hohlmann and R. Kumar Verma and M. Rahmani and E. Yanes and M. R. Adams and A. Baty and C. Bennett and R. Cavanaugh and R. Escobar Franco and O. Evdokimov and C. E. Gerber and M. Hawksworth and A. Hingrajiya and D. J. Hofman and J. h. Lee and D. S. Lemos and A. H. Merrit and C. Mills and S. Nanda and G. Oh and B. Ozek and D. Pilipovic and R. Pradhan and E. Prifti and T. Roy and S. Rudrabhatla and M. B. Tonjes and N. Varelas and M. A. Wadud and Z. Ye and M. Alhusseini and D. Blend and K. Dilsiz and L. Emediato and G. Karaman and O. K. Köseyan and J.-P. Merlo and A. Mestvirishvili and J. Nachtman and O. Neogi and H. Ogul and Y. Onel and A. Penzo and C. Snyder and E. Tiras and B. Blumenfeld and L. Corcodilos and J. Davis and A. V. Gritsan and L. Kang and S. Kyriacou and P. Maksimovic and M. Roguljic and J. Roskes and S. Sekhar and M. Swartz and A. Abreu and L. F. Alcerro Alcerro and J. Anguiano and P. Baringer and A. Bean and Z. Flowers and D. Grove and J. King and G. Krintiras and M. Lazarovits and C. Le Mahieu and J. Marquez and N. Minafra and M. Murray and M. Nickel and M. Pitt and S. Popescu and C. Rogan and C. Royon and R. Salvatico and S. Sanders and C. Smith and G. Wilson and B. Allmond and R. Gujju Gurunadha and A. Ivanov and K. Kaadze and A. Kalogeropoulos and Y. Maravin and J. Natoli and D. Roy and G. Sorrentino and F. Rebassoo and D. Wright and A. Baden and A. Belloni and Y. M. Chen and S. C. Eno and N. J. Hadley and S. Jabeen and R. G. Kellogg and T. Koeth and Y. Lai and S. Lascio and A. C. Mignerey and S. Nabili and C. Palmer and C. Papageorgakis and M. M. Paranjpe and L. Wang and J. Bendavid and I. A. Cali and M. D’Alfonso and J. Eysermans and C. Freer and G. Gomez-Ceballos and M. Goncharov and G. Grosso and P. Harris and D. Hoang and D. Kovalskyi and J. Krupa and L. Lavezzo and Y.-J. Lee and K. Long and A. Novak and C. Paus and D. Rankin and C. Roland and G. Roland and S. Rothman and G. S. F. Stephans and B. Wyslouch and T. J. Yang and B. Crossman and B. M. Joshi and C. Kapsiak and M. Krohn and D. Mahon and J. Mans and B. Marzocchi and S. Pandey and M. Revering and R. Rusack and R. Saradhy and N. Schroeder and N. Strobbe and L. M. Cremaldi and K. Bloom and D. R. Claes and G. Haza and J. Hossain and C. Joo and I. Kravchenko and J. E. Siado and W. Tabb and A. Vagnerini and A. Wightman and F. Yan and D. Yu and H. Bandyopadhyay and L. Hay and I. Iashvili and A. Kharchilava and M. Morris and D. Nguyen and S. Rappoccio and H. Rejeb Sfar and A. Williams and G. Alverson and E. Barberis and J. Dervan and Y. Haddad and Y. Han and A. Krishna and J. Li and M. Lu and G. Madigan and R. Mccarthy and D. M. Morse and V. Nguyen and T. Orimoto and A. Parker and L. Skinnari and D. Wood and J. Bueghly and Z. Chen and S. Dittmer and K. A. Hahn and Y. Liu and Y. Miao and D. G. Monk and M. H. Schmitt and A. Taliercio and M. Velasco and G. Agarwal and R. Band and R. Bucci and S. Castells and A. Das and R. Goldouzian and M. Hildreth and K. W. Ho and K. Hurtado Anampa and T. Ivanov and C. Jessop and K. Lannon and J. Lawrence and N. Loukas and L. Lutton and J. Mariano and N. Marinelli and I. Mcalister and T. McCauley and C. Mcgrady and C. Moore and Y. Musienko and H. Nelson and M. Osherson and A. Piccinelli and R. Ruchti and A. Townsend and Y. Wan and M. Wayne and H. Yockey and M. Zarucki and L. Zygala and A. Basnet and B. Bylsma and M. Carrigan and L. S. Durkin and C. Hill and M. Joyce and M. Nunez Ornelas and K. Wei and B. L. Winer and B. R. Yates and F. M. Addesa and H. Bouchamaoui and P. Das and G. Dezoort and P. Elmer and A. Frankenthal and B. Greenberg and N. Haubrich and G. Kopp and S. Kwan and D. Lange and A. Loeliger and D. Marlow and I. Ojalvo and J. Olsen and A. Shevelev and D. Stickland and C. Tully and A. S. Bakshi and V. E. Barnes and S. Chandra and R. Chawla and A. Gu and L. Gutay and M. Jones and A. W. Jung and D. Kondratyev and A. M. Koshy and M. Liu and G. Negro and N. Neumeister and G. Paspalaki and S. Piperov and V. Scheurer and J. F. Schulte and M. Stojanovic and J. Thieman and A. K. Virdi and F. Wang and W. Xie and J. Dolen and N. Parashar and A. Pathak and D. Acosta and T. Carnahan and K. M. Ecklund and P. J. Fernández Manteca and S. Freed and P. Gardner and F. J. M. Geurts and W. Li and O. Miguel Colin and B. P. Padley and R. Redjimi and J. Rotter and E. Yigitbasi and Y. Zhang and A. Bodek and P. de Barbaro and R. Demina and J. L. Dulemba and A. Garcia-Bellido and O. Hindrichs and A. Khukhunaishvili and N. Parmar and P. Parygin and E. Popova and R. Taus and K. Goulianos and B. Chiarito and J. P. Chou and S. V. Clark and D. Gadkari and Y. Gershtein and E. Halkiadakis and M. Heindl and C. Houghton and D. Jaroslawski and O. Karacheban and S. Konstantinou and I. Laflotte and A. Lath and R. Montalvo and K. Nash and H. Routray and P. Saha and S. Salur and S. Schnetzer and S. Somalwar and R. Stone and S. A. Thayil and S. Thomas and J. Vora and H. Wang and H. Acharya and D. Ally and A. G. Delannoy and S. Fiorendi and S. Higginbotham and T. Holmes and A. R. Kanuganti and N. Karunarathna and L. Lee and E. Nibigira and S. Spanier and D. Aebi and M. Ahmad and O. Bouhali and R. Eusebi and J. Gilmore and T. Huang and T. Kamon and S. Luo and R. Mueller and D. Overton and D. Rathjens and A. Safonov and N. Akchurin and J. Damgov and V. Hegde and A. Hussain and Y. Kazhykarim and K. Lamichhane and A. Mankel and T. Peltola and I. Volobouev and E. Appelt and Y. Chen and S. Greene and A. Gurrola and W. Johns and R. Kunnawalkam Elayavalli and A. Melo and F. Romeo and P. Sheldon and S. Tuo and J. Velkovska and J. Viinikainen and B. Cardwell and B. Cox and J. Hakala and R. Hirosky and A. Ledovskoy and C. Neu and C. E. Perez Lara and P. E. Karchin and A. Aravind and K. Black and T. Bose and S. Dasu and I. De Bruyn and P. Everaerts and C. Galloni and H. He and M. Herndon and A. Herve and C. K. Koraka and A. Lanaro and R. Loveless and J. Madhusudanan Sreekala and A. Mallampalli and A. Mohammadi and G. Parida and L. Pétré and D. Pinna and A. Savin and V. Shang and W. H. Smith and D. Teague and H. F. Tsoi and W. Vetens and A. Warden and S. Afanasiev and V. Andreev and Yu. Andreev and T. Aushev and M. Azarkin and I. Azhgirey and A. Babaev and V. Blinov and E. Boos and V. Borshch and D. Budkouski and M. Chadeeva and V. Chekhovsky and R. Chistov and A. Dermenev and T. Dimova and D. Druzhkin and M. Dubinin and L. Dudko and A. Ershov and G. Gavrilov and V. Gavrilov and S. Gninenko and V. Golovtcov and N. Golubev and I. Golutvin and I. Gorbunov and A. Gribushin and Y. Ivanov and V. Kachanov and V. Karjavine and A. Karneyeu and V. Kim and M. Kirakosyan and D. Kirpichnikov and M. Kirsanov and V. Klyukhin and O. Kodolova and D. Konstantinov and V. Korenkov and A. Kozyrev and N. Krasnikov and A. Lanev and P. Levchenko and N. Lychkovskaya and V. Makarenko and A. Malakhov and V. Matveev and V. Murzin and A. Nikitenko and S. Obraztsov and V. Oreshkin and V. Palichik and V. Perelygin and S. Petrushanko and S. Polikarpov and V. Popov and O. Radchenko and R. Ryutin and M. Savina and V. Savrin and V. Shalaev and S. Shmatov and S. Shulha and Y. Skovpen and S. Slabospitskii and V. Smirnov and A. Snigirev and D. Sosnov and V. Sulimov and E. Tcherniaev and A. Terkulov and O. Teryaev and I. Tlisova and A. Toropin and L. Uvarov and A. Uzunian and A. Vorobyev and N. Voytishin and B. S. Yuldashev and A. Zarubin and I. Zhizhin and A. Zhokin}, doi = {10.1103/PhysRevLett.134.041801}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041801}, shortjournal = {Phys. Rev. Lett.}, title = {Search for new resonances decaying to pairs of merged diphotons in proton-proton collisions at s=13 TeV}, volume = {134}, year = {2025}, }
• (2025). Defining the type IIB matrix model without breaking lorentz symmetry. PRL, 134(4), 041603. (www)

  @article{ , abstract = {The type IIB matrix model is a promising nonperturbative formulation of superstring theory, which may elucidate the emergence of ( )-dimensional space-time. However, the partition function is divergent due to the Lorentz symmetry, which is represented by a noncompact group. This divergence has been regularized conventionally by introducing some infrared cutoff, which breaks the Lorentz symmetry. Here we point out, in a simple model, that Lorentz-invariant observables become classical as one removes the infrared cutoff and that this “classicalization” is actually an artifact of the Lorentz symmetry breaking cutoff. In order to overcome this problem, we propose a natural way to “gauge-fix” the Lorentz symmetry in a fully nonperturbative manner. Thus, we arrive at a new definition of the type IIB matrix model, which also enables us to perform numerical simulations in such a way that the time evolution can be extracted from the generated configurations.}, archive = {J_PRL}, author = {Yuhma Asano and Jun Nishimura and Worapat Piensuk and Naoyuki Yamamori}, doi = {10.1103/PhysRevLett.134.041603}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041603}, shortjournal = {Phys. Rev. Lett.}, title = {Defining the type IIB matrix model without breaking lorentz symmetry}, volume = {134}, year = {2025}, }
• (2025). Ultraviolet-complete local field theory of persistent symmetry breaking in 2+1 dimensions. PRL, 134(4), 041602. (www)

  @article{ , abstract = {Spontaneous symmetry breaking can persist at all temperatures in certain biconical O ( N ) × Z 2 vector models when the underlying field theories are ultraviolet complete. So far, the existence of such theories has been established in fractional dimensions for local but nonunitary models or in 2 + 1 dimensions but for nonlocal models. Here, we study local models at zero and finite temperature directly in 2 + 1 dimensions employing functional methods. At zero temperature, we establish that our approach describes the quantum critical behavior with good accuracy for all N ≥ 2 . We then exhibit the mechanism of discrete symmetry breaking from O ( N ) × Z 2 → O ( N ) for increasing temperature near the biconical critical point when N is finite but large. We calculate the corresponding finite-temperature phase diagram and further show that the Hohenberg-Mermin-Wagner theorem is fully respected within this approach, i.e., symmetry breaking only occurs in the Z 2 sector. Finally, we determine the critical N above which this phenomenon can be observed to be N c ≈ 15 .}, archive = {J_PRL}, author = {Bilal Hawashin and Junchen Rong and Michael M. Scherer}, doi = {10.1103/PhysRevLett.134.041602}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041602}, shortjournal = {Phys. Rev. Lett.}, title = {Ultraviolet-complete local field theory of persistent symmetry breaking in 2+1 dimensions}, volume = {134}, year = {2025}, }
• (2025). Multiparticle flux-tube S-matrix bootstrap. PRL, 134(4), 041601. (www)

  @article{ , abstract = {We introduce the notion of jets, states of collinear flux-tube excitations. We argue for the analyticity, crossing, and unitarity of the multiparticle scattering of these jets and, through the S-matrix bootstrap, place bounds on a set of finite-energy multiparticle sum rules. Such bounds define a matrioska with a smaller and smaller allowed regions as we impose more constraints. The Yang-Mills flux tube, as well as other interesting flux-tube theories recently studied through lattice simulations, lie inside a tiny island hundreds of times smaller than the most general space of allowed theories.}, archive = {J_PRL}, author = {Andrea Guerrieri and Alexandre Homrich and Pedro Vieira}, doi = {10.1103/PhysRevLett.134.041601}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041601}, shortjournal = {Phys. Rev. Lett.}, title = {Multiparticle flux-tube S-matrix bootstrap}, volume = {134}, year = {2025}, }
• (2025). Enhancing cosmological model selection with interpretable machine learning. PRL, 134(4), 041002. (www)

  @article{ , abstract = {We propose a novel approach using neural networks (NNs) to differentiate between cosmological models, and implemented lime as an interpretability approach to identify the key features influencing our model’s decisions. We show the potential of NNs to enhance the extraction of meaningful information from cosmological large-scale structure data, based on current galaxy-clustering survey specifications, for the cosmological constant and cold dark matter ( Λ CDM ) model and the Hu-Sawicki f ( R ) model. We find that the NN can successfully distinguish between Λ C D M and the f ( R ) models, by predicting the correct model with approximately 97% overall accuracy, thus demonstrating that NNs can maximize the potential of current and next generation surveys to probe for deviations from general relativity.}, archive = {J_PRL}, author = {Indira Ocampo and George Alestas and Savvas Nesseris and Domenico Sapone}, doi = {10.1103/PhysRevLett.134.041002}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041002}, shortjournal = {Phys. Rev. Lett.}, title = {Enhancing cosmological model selection with interpretable machine learning}, volume = {134}, year = {2025}, }
• (2025). Exploring new physics with PandaX-4T low energy electronic recoil data. PRL, 134(4), 041001. (www)

  @article{ , abstract = {New particles beyond the standard model of particle physics, such as axions, can be effectively searched through their interactions with electrons. We use the large liquid xenon detector PandaX-4T to search for novel electronic recoil signals induced by solar axions, neutrinos with anomalous magnetic moment, axionlike particles, dark photons, and light fermionic dark matter. A detailed background model is established using the latest datasets with 1.54 ton yr exposure. No significant excess above the background has been observed, and we have obtained competitive constraints for axion couplings, neutrino magnetic moment, and fermionic dark matter interactions.}, archive = {J_PRL}, author = {PandaX Collaboration and Xinning Zeng and Zihao Bo and Wei Chen and Xun Chen and Yunhua Chen and Zhaokan Cheng and Xiangyi Cui and Yingjie Fan and Deqing Fang and Zhixing Gao and Lisheng Geng and Karl Giboni and Xunan Guo and Xuyuan Guo and Zichao Guo and Chencheng Han and Ke Han and Changda He and Jinrong He and Di Huang and Houqi Huang and Junting Huang and Ruquan Hou and Yu Hou and Xiangdong Ji and Xiangpan Ji and Yonglin Ju and Chenxiang Li and Jiafu Li and Mingchuan Li and Shuaijie Li and Tao Li and Zhiyuan Li and Qing Lin and Jianglai Liu and Congcong Lu and Xiaoying Lu and Lingyin Luo and Yunyang Luo and Wenbo Ma and Yugang Ma and Yajun Mao and Yue Meng and Xuyang Ning and Binyu Pang and Ningchun Qi and Zhicheng Qian and Xiangxiang Ren and Dong Shan and Xiaofeng Shang and Xiyuan Shao and Guofang Shen and Manbin Shen and Wenliang Sun and Yi Tao and Anqing Wang and Guanbo Wang and Hao Wang and Jiamin Wang and Lei Wang and Meng Wang and Qiuhong Wang and Shaobo Wang and Siguang Wang and Wei Wang and Xiuli Wang and Xu Wang and Zhou Wang and Yuehuan Wei and Weihao Wu and Yuan Wu and Mengjiao Xiao and Xiang Xiao and Kaizhi Xiong and Yifan Xu and Shunyu Yao and Binbin Yan and Xiyu Yan and Yong Yang and Peihua Ye and Chunxu Yu and Ying Yuan and Zhe Yuan and Youhui Yun and Minzhen Zhang and Peng Zhang and Shibo Zhang and Shu Zhang and Tao Zhang and Wei Zhang and Yang Zhang and Yingxin Zhang and Yuanyuan Zhang and Li Zhao and Jifang Zhou and Jiaxu Zhou and Jiayi Zhou and Ning Zhou and Xiaopeng Zhou and Yubo Zhou and Zhizhen Zhou}, doi = {10.1103/PhysRevLett.134.041001}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {041001}, shortjournal = {Phys. Rev. Lett.}, title = {Exploring new physics with PandaX-4T low energy electronic recoil data}, volume = {134}, year = {2025}, }
• (2025). Experimental measurement-device-independent quantum cryptographic conferencing. PRL, 134(4), 040802. (www)

  @article{ , abstract = {Quantum cryptographic conferencing (QCC) allows sharing secret keys among multiple distant users and plays a crucial role in quantum networks. Because of the fragility and low generation rate of genuine multipartite entangled states required in QCC, realizing and extending QCC with the entanglement-based protocol is challenging. Measurement-device-independent (MDI) QCC, which removes all detector side channels, is a feasible long-distance quantum communication scheme to practically generate multipartite correlation with multiphoton projection measurement. Here we experimentally realize the three-user MDI QCC protocol with four-intensity decoy-state method, in which we employ the polarization encoding and the Greenberger-Horne-Zeilinger state projection measurement. Our work demonstrates the experimental feasibility of the MDI QCC, which lays the foundation for the future realization of quantum networks with multipartite communication tasks.}, archive = {J_PRL}, author = {Yifeng Du and Yufeng Liu and Chengdong Yang and Xiaodong Zheng and Shining Zhu and Xiao-song Ma}, doi = {10.1103/PhysRevLett.134.040802}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {040802}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental measurement-device-independent quantum cryptographic conferencing}, volume = {134}, year = {2025}, }
• (2025). Engineering one axis twisting via a dissipative berry phase using strong symmetries. PRL, 134(4), 040801. (www)

  @article{ , abstract = {We show how a driven-dissipative cavity coupled to a collective ensemble of atoms can dynamically generate metrologically useful spin-squeezed states. In contrast to other dissipative approaches, we do not rely on complex engineered dissipation or input states, nor do we require tuning the system to a critical point. Instead, we utilize a strong symmetry, a special type of symmetry that can occur in open quantum systems and emerges naturally in systems with collective dissipation, such as superradiance. This symmetry preserves coherence and allows for the accumulation of an atom number-dependent Berry phase which in turn creates spin-squeezed states via emergent one axis twisting dynamics. This work shows that it is possible to generate entanglement in an atom-cavity resonant regime with macroscopic optical excitations of the system, going beyond the typical dispersive regime with negligible optical excitations often utilized in current cavity-QED experiments.}, archive = {J_PRL}, author = {Jeremy T. Young and Edwin Chaparro and Asier Piñeiro Orioli and James K. Thompson and Ana Maria Rey}, doi = {10.1103/PhysRevLett.134.040801}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {040801}, shortjournal = {Phys. Rev. Lett.}, title = {Engineering one axis twisting via a dissipative berry phase using strong symmetries}, volume = {134}, year = {2025}, }
• (2025). Certifying quantum temporal correlation via randomized measurements: Theory and experiment. PRL, 134(4), 040201. (www)

  @article{ , abstract = {We consider the certification of temporal quantum correlations using the pseudo-density operator (PDO), an extension of the density matrix to the time domain, where negative eigenvalues are key indicators of temporal correlations. Conventional methods for detecting these correlations rely on PDO tomography, which often involves excessive redundant information and requires exponential resources. In this work, we develop an efficient protocol for temporal correlation detection by virtually preparing the PDO within a single time slice and estimating its second-order moments using randomized measurements. Through sample complexity analysis, we demonstrate that our protocol requires only a constant number of measurement bases, making it particularly advantageous for systems utilizing ensemble average measurements, as it maintains constant runtime complexity regardless of the number of qubits. We experimentally validate our protocol on a nuclear magnetic resonance platform, a typical thermodynamic quantum system, where the experimental results closely align with theoretical predictions, confirming the effectiveness of our protocol.}, archive = {J_PRL}, author = {Hongfeng Liu and Zhenhuan Liu and Shu Chen and Xinfang Nie and Xiangjing Liu and Dawei Lu}, doi = {10.1103/PhysRevLett.134.040201}, journal = {Physical Review Letters}, month = {1}, number = {4}, pages = {040201}, shortjournal = {Phys. Rev. Lett.}, title = {Certifying quantum temporal correlation via randomized measurements: Theory and experiment}, volume = {134}, year = {2025}, }
• (2025). Atomic description of the reciprocal action between supercoils and melting bubbles on linear DNA. PRL, 134(3), 038403. (www)

  @article{ , abstract = {Although the mechanical response of DNA to physiological torsion and tension is well characterized, the detailed structures are not yet known. By using molecular dynamics simulations on linear DNA with 300 base-pairs, we provide, for the first time, the conformational phase diagram at atomic resolution. Our simulations also reveal the dynamics and diffusion of supercoils. We observe a new state in negative supercoiling, where denaturation bubbles form in adenine/thymine-rich regions independently of the underlying DNA topology. We thus propose sequence-dependent bubbles could position plectonemes in longer DNA.}, archive = {J_PRL}, author = {Matthew Burman and Agnes Noy}, doi = {10.1103/PhysRevLett.134.038403}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {038403}, shortjournal = {Phys. Rev. Lett.}, title = {Atomic description of the reciprocal action between supercoils and melting bubbles on linear DNA}, volume = {134}, year = {2025}, }
• (2025). High-speed combinatorial polymerization through kinetic-trap encoding. PRL, 134(3), 038402. (www)

  @article{ , abstract = {Like the letters in the alphabet forming words, reusing components of a heterogeneous mixture is an efficient strategy for assembling a large number of target structures. Examples range from synthetic DNA origami to proteins self-assembling into complexes. The standard self-assembly paradigm views target structures as free-energy minima of a mixture. While this is an appealing picture, at high speed structures may be kinetically trapped in local minima, reducing self-assembly accuracy. How then can high speed, high accuracy, and combinatorial usage of components coexist? We propose to reconcile these three concepts not by avoiding kinetic traps, but by exploiting them to encode target structures. This can be achieved by sculpting the kinetic pathways of the mixture, instead of its free-energy landscape. We formalize these ideas in a minimal toy model, for which we analytically estimate the encoding capacity and kinetic characteristics, in agreement with simulations. Our results may be generalized to other soft-matter systems capable of computation, such as liquid mixtures or elastic networks, and pave the way for high-dimensional information processing far from equilibrium.}, archive = {J_PRL}, author = {Félix Benoist and Pablo Sartori}, doi = {10.1103/PhysRevLett.134.038402}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {038402}, shortjournal = {Phys. Rev. Lett.}, title = {High-speed combinatorial polymerization through kinetic-trap encoding}, volume = {134}, year = {2025}, }
• (2025). Criticality in the luria-delbrück model with an arbitrary mutation rate. PRL, 134(3), 038401. (www)

  @article{ , abstract = {The Luria-Delbrück model is a classic model of population dynamics with random mutations, that has been used historically to prove that random mutations drive evolution. In typical scenarios, the relevant mutation rate is exceedingly small, and mutants are counted only at the final time point. Here, inspired by recent experiments on DNA repair, we study a mathematical model that is formally equivalent to the Luria-Delbrück setup, with the repair rate p playing the role of mutation rate, albeit taking on large values, of order unity per cell division. We find that although at large times the fraction of repaired cells approaches one, the variance of the number of repaired cells undergoes a phase transition: when p > 1 / 2 the variance decreases with time, but, intriguingly, for p < 1 / 2 even though the fraction of repaired cells approaches 1, the variance in the number of repaired cells increases with time. Analyzing DNA-repair experiments, we find that in order to explain the data the model should also take into account the probability of a successful repair process once it is initiated. Taken together, our work shows how the study of variability can lead to surprising phase transitions as well as provide biological insights into the process of DNA repair.}, archive = {J_PRL}, author = {Deng Pan and Jie Lin and Ariel Amir}, doi = {10.1103/PhysRevLett.134.038401}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {038401}, shortjournal = {Phys. Rev. Lett.}, title = {Criticality in the luria-delbrück model with an arbitrary mutation rate}, volume = {134}, year = {2025}, }
• (2025). Biased ensembles of pulsating active matter. PRL, 134(3), 038301. (www)

  @article{ , abstract = {We discover unexpected connections between packing configurations and rare fluctuations in dense systems of active particles subject to pulsation of size. Using large deviation theory, we examine biased ensembles which select atypical realizations of the dynamics exhibiting high synchronization in particle size. We show that the order emerging at high bias can manifest as distinct dynamical states featuring high to vanishing pulsation current. Remarkably, transitions between these states arise from changing the system geometry at fixed bias and constant density. We rationalize such transitions as arising from the change in packing configurations which, depending on box geometry, may induce highly ordered or geometrically frustrated structures. Furthermore, we reveal that a master curve in the unbiased dynamics, correlating polydispersity and current, helps predict the dynamical state emerging in the biased dynamics. Finally, we demonstrate that deformation waves can propagate under suitable geometries when biasing with local order.}, archive = {J_PRL}, author = {William D. Piñeros and Étienne Fodor}, doi = {10.1103/PhysRevLett.134.038301}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {038301}, shortjournal = {Phys. Rev. Lett.}, title = {Biased ensembles of pulsating active matter}, volume = {134}, year = {2025}, }
• (2025). Glass transition in monolayers of rough colloidal ellipsoids. PRL, 134(3), 038202. (www)

  @article{ , abstract = {Structure-dynamics correlation is one of the major ongoing debates in the glass transition, although a number of structural features have been found connected to the dynamic heterogeneity in different glass-forming colloidal systems. Here, using colloidal experiments combined with coarse-grained molecular dynamics simulations, we investigate the glass transition in monolayers of rough colloidal ellipsoids. Compared with smooth colloidal ellipsoids, the surface roughness of ellipsoids is found to significantly change the nature of glass transition. In particular, we find that the surface roughness induced by coating only a few small hemispheres on the ellipsoids can eliminate the existence of orientational glass and the two-step glass transition found in monolayers of smooth ellipsoids. This is due to the surface roughness-induced coupling between the translational and rotational degrees of freedom in colloidal ellipsoids, which also destroys the structure-dynamics correlation found in glass-forming suspensions of colloidal ellipsoids. Our results not only suggest a new way of using surface roughness to manipulate the glass transition in colloidal systems, but also highlight the importance of detailed particle shape on the glass transition and structure-dynamics correlation in suspensions of anisotropic colloids.}, archive = {J_PRL}, author = {Jian Liang and Xuan Feng and Ning Zheng and Huaguang Wang and Ran Ni and Zexin Zhang}, doi = {10.1103/PhysRevLett.134.038202}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {038202}, shortjournal = {Phys. Rev. Lett.}, title = {Glass transition in monolayers of rough colloidal ellipsoids}, volume = {134}, year = {2025}, }
• (2025). Nonmonotonic constitutive curves and shear banding in dry and wet granular flows. PRL, 134(3), 038201. (www)

  @article{ , abstract = {We use particle simulations to map comprehensively the shear rheology of dry and wet granular matter comprising particles of finite stiffness, in both fixed pressure and fixed volume protocols. At fixed pressure we find nonmonotonic constitutive curves that are shear thinning, whereas at fixed volume we find nonmonotonic constitutive curves that are shear thickening. We show that the presence of one nonmonotonicity does not imply the other. Instead, there exists a signature in the volume fraction measured under fixed pressure that, when present, ensures nonmonotonic constitutive curves at fixed volume. In the context of dry granular flow we show that gradient and vorticity bands arise under fixed pressure and volume, respectively, as implied by the constitutive curves. For wet systems our results are consistent with a recent experimental observation of shear thinning at fixed pressure. We furthermore predict discontinuous shear thickening in the absence of critical load friction.}, archive = {J_PRL}, author = {Christopher Ness and Suzanne M. Fielding}, doi = {10.1103/PhysRevLett.134.038201}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {038201}, shortjournal = {Phys. Rev. Lett.}, title = {Nonmonotonic constitutive curves and shear banding in dry and wet granular flows}, volume = {134}, year = {2025}, }
• (2025). Dynamical mean-field theory of complex systems on sparse directed networks. PRL, 134(3), 037401. (www)

  @article{ , abstract = {Although real-world complex systems typically interact through sparse and heterogeneous networks, analytic solutions of their dynamics are limited to models with all-to-all interactions. Here, we solve the dynamics of a broad range of nonlinear models of complex systems on sparse directed networks with a random structure. By generalizing dynamical mean-field theory to sparse systems, we derive an exact equation for the path probability describing the effective dynamics of a single degree of freedom. Our general solution applies to key models in the study of neural networks, ecosystems, epidemic spreading, and synchronization. Using the population dynamics algorithm, we solve the path-probability equation to determine the phase diagram of a seminal neural network model in the sparse regime, showing that this model undergoes a transition from a fixed-point phase to chaos as a function of the network topology.}, archive = {J_PRL}, author = {Fernando L. Metz}, doi = {10.1103/PhysRevLett.134.037401}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {037401}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical mean-field theory of complex systems on sparse directed networks}, volume = {134}, year = {2025}, }
• (2025). Dynamics of microscale and nanoscale systems in the weak-memory regime. PRL, 134(3), 037101. (www)

  @article{ , abstract = {Memory effects are ubiquitous in small-scale systems. They emerge from interactions between accessible and inaccessible degrees of freedom and give rise to evolution equations that are nonlocal in time. If the characteristic timescales of accessible and inaccessible degrees of freedom are sharply separated, locality can be restored through the standard Markov approximation. Here, we show that this approach can be rigorously extended to a well-defined weak-memory regime, where the relevant timescales can be of comparable order of magnitude. We derive explicit bounds on the error of the local approximation and a convergent perturbation scheme for its construction. Being applicable to any nonlocal time evolution equation that is autonomous and linear in the variables of interest, our theory provides a unifying framework for the systematic description of memory effects.}, archive = {J_PRL}, author = {Kay Brandner}, doi = {10.1103/PhysRevLett.134.037101}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {037101}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamics of microscale and nanoscale systems in the weak-memory regime}, volume = {134}, year = {2025}, }
• (2025). Unifying floquet theory of longitudinal and dispersive readout. PRL, 134(3), 037003. (www)

  @article{ , abstract = {We devise a Floquet theory of longitudinal and dispersive readout in circuit quantum electrodynamics (cQED). By studying qubits coupled to cavity photons and driven at the resonance frequency of the cavity ω r , we establish a universal connection between the qubit ac Stark shift and the longitudinal and dispersive coupling to photons. We find that the longitudinal coupling g ∥ is controlled by the slope of the ac Stark shift as function of the driving strength A q , while the dispersive shift χ depends on its curvature. The two quantities become proportional to each other in the weak drive limit ( A q → 0 ). Our approach unifies the adiabatic limit ( ω r → 0 )—where g ∥ is generated by the static spectrum curvature (or quantum capacitance)—with the diabatic limit, where ω r is large and the static spectrum plays no role. We derive analytical results supported by exact numerical simulations. We apply them to superconducting and spin-hybrid cQED systems, showcasing the flexibility of faster-than-dispersive longitudinal readout.}, archive = {J_PRL}, author = {A. Chessari and E. A. Rodríguez-Mena and J. C. Abadillo-Uriel and V. Champain and S. Zihlmann and R. Maurand and Y.-M. Niquet and M. Filippone}, doi = {10.1103/PhysRevLett.134.037003}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {037003}, shortjournal = {Phys. Rev. Lett.}, title = {Unifying floquet theory of longitudinal and dispersive readout}, volume = {134}, year = {2025}, }
• (2025). Reconfiguring surface acoustic wave microfluidics via in situ control of elastic wave polarization. PRL, 134(3), 037002. (www)

  @article{ , abstract = {We demonstrate in situ control of the elastic wave polarization in a surface acoustic wave (SAW). It allows us to create highly reconfigurable SAW microfluidics that can be switched on demand between the acoustohydrodynamic (AHD) regime and electrohydrodynamic (EHD) regime for manipulating particles and cells. The control of wave polarization comes from our experimental and theoretical identification of an unexpected shear-horizontal (SH) wave mode in a conventional Rayleigh (R) wave design, which is stereotyped to excite only vertically polarized Rayleigh SAWs. The SH wave mode is predominantly horizontally polarized and can be selectively excited to propagate in the same direction as the Rayleigh SAW. Such a selective wave generation between the SH mode and R mode allows for reconfiguration between AHD and EHD regimes that leads to unprecedented colloidal patterns and assembly dynamics. Such a reconfiguration of the particle manipulation mechanism can be explained by the controllable competition or synergism between the coexisting acoustic and electric fields. Remarkably, in the EHD regime, a virtual zero-boundary electric quadrupole is created, and a novel colloidal diamond-shaped assembly is observed in this piezoelectric-quadrupole trap, which was rarely reported in acoustic or electric microfluidics. The presented in situ control of polarization revolutionizes our understanding of SAW and acoustofluidics, expands its potential by assuming the advantages of AHD and EHD on demand, and inspires new strategies in micro- and nanoscale manufacturing and manipulation, with applications beyond fundamental scientific interest.}, archive = {J_PRL}, author = {Yu Gao (郜煜 and Thomas Voglhuber-Brunnmaier and Yuekang Li and Leyla Akh and Nicholas H. Patino and Apresio Kefin Fajrial and Massimo Ruzzene and Bernhard Jakoby and Xiaoyun Ding}, doi = {10.1103/PhysRevLett.134.037002}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {037002}, shortjournal = {Phys. Rev. Lett.}, title = {Reconfiguring surface acoustic wave microfluidics via in situ control of elastic wave polarization}, volume = {134}, year = {2025}, }
• (2025). Single-electron quantization of dark current in quanta image sensors. PRL, 134(3), 037001. (www)

  @article{ , abstract = {We present a first experimental study of dark current in a quanta image sensor (QIS) based on complementary metal-oxide-semiconductor (CMOS) technology. With the extremely low noise levels of this sensor it is possible to observe spatial and temporal dark current quantization. Analysis of dark carrier emission timing confirms that carrier generation behaves as a Poisson process. The mean of this Poisson distribution is the only parameter needed to characterize a sensor, thus greatly reducing the required measurement and computational resources typically employed in device noise analysis. The impact of this new characterization method will be useful to a range of industrial and scientific applications requiring high accuracy in photoelectron counting, such as in particle detection or quantum sensing. The ability to observe single carrier emission in a QIS leads to a deeper understanding of the mechanism of dark current generation in state-of-the-art semiconductors, thereby promoting improvements in the development of device design and process technology.}, archive = {J_PRL}, author = {Joanna Krynski and Daniel McGrath and Alexandre Le Roch and Sarah Holloway and Lucrezia Migliorin and Cédric Virmontois and Vincent Goiffon}, doi = {10.1103/PhysRevLett.134.037001}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {037001}, shortjournal = {Phys. Rev. Lett.}, title = {Single-electron quantization of dark current in quanta image sensors}, volume = {134}, year = {2025}, }
• (2025). Spin noise spectroscopy of a single spin using single detected photons. PRL, 134(3), 036902. (www)

  @article{ , abstract = {Spin noise spectroscopy has become a widespread technique to extract information on spin dynamics in atomic and solid-state systems, in a potentially nonperturbative way. Here we experimentally demonstrate a new approach in spin noise spectroscopy, based on the detection of single photons. Because of the large spin-dependent polarization rotations provided by a deterministically coupled quantum dot-micropillar device, giant spin noise signals induced by a single-hole spin are extracted in the form of photon-photon cross-correlations. Ultimately, such a technique can be extended to an ultrafast regime probing mechanisms down to few tens of picoseconds.}, archive = {J_PRL}, author = {M. Gundín and P. Hilaire and C. Millet and E. Mehdi and C. Antón and A. Harouri and A. Lemaître and I. Sagnes and N. Somaschi and O. Krebs and P. Senellart and L. Lanco}, doi = {10.1103/PhysRevLett.134.036902}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036902}, shortjournal = {Phys. Rev. Lett.}, title = {Spin noise spectroscopy of a single spin using single detected photons}, volume = {134}, year = {2025}, }
• (2025). Valley-mediated singlet- and triplet-polaron interactions and quantum dynamics in a doped WSe2 monolayer. PRL, 134(3), 036901. (www)

  @article{ , abstract = {In doped transition metal dichalcogenides, optically created excitons (bound electron-hole pairs) can strongly interact with a Fermi sea of electrons to form Fermi polaron quasiparticles. When there are two distinct Fermi seas, as is the case in , there are two flavors of lowest-energy (attractive) polarons—singlet and triplet—where the exciton is coupled to the Fermi sea in the same or opposite valley, respectively. Using two-dimensional coherent electronic spectroscopy, we analyze how their quantum decoherence evolves with doping density and determine the condition under which stable Fermi polarons form. Because of the large oscillator strength associated with these resonances, intrinsic quantum dynamics of polarons as well as valley coherence between coupled singlet- and triplet polarons occur on subpicosecond timescales. Surprisingly, we find that a dark-to-bright state conversion process leads to a particularly long-lived singlet polaron valley polarization, persisting up to 200–800 ps. Valley coherence between the singlet- and triplet polaron is correlated with their energy fluctuations. Our finding provides valuable guidance for the electrical and optical control of spin and valley indexes in atomically thin semiconductors.}, archive = {J_PRL}, author = {Yue Ni and Di Huang and Danfu Liang and Albert Liu and Xiaohui Liu and Kevin Sampson and Zhida Liu and Jianmin Quan and Kenji Watanabe and Takashi Taniguchi and Dmitry K. Efimkin and Jesper Levinsen and Meera M. Parish and Xiaoqin Li}, doi = {10.1103/PhysRevLett.134.036901}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036901}, shortjournal = {Phys. Rev. Lett.}, title = {Valley-mediated singlet- and triplet-polaron interactions and quantum dynamics in a doped WSe2 monolayer}, volume = {134}, year = {2025}, }
• (2025). Enhanced strange metallicity due to hubbard-U coulomb repulsion. PRL, 134(3), 036502. (www)

  @article{ , abstract = {We solve a model of electrons with Hubbard- Coulomb repulsion and a random Yukawa coupling to a two-dimensional bosonic bath, using an extended dynamical mean field theory scheme. Our model exhibits a quantum critical point, at which the repulsive component of the electron interactions strongly enhances the effects of the quantum critical bosonic fluctuations on the electrons, leading to a breakdown of Fermi liquid physics and the formation of a strange metal with “Planckian” [ ] quasiparticle decay rates at low temperatures . Furthermore, the eventual Mott transition that occurs as the repulsion is increased seemingly bounds the maximum decay rate in the strange metal. Our results provide insight into low-temperature strange metallicity observed in proximity to a Mott transition, as is observed, for instance, in recent experiments on certain moiré materials.}, archive = {J_PRL}, author = {Andrew Hardy and Olivier Parcollet and Antoine Georges and Aavishkar A. Patel}, doi = {10.1103/PhysRevLett.134.036502}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036502}, shortjournal = {Phys. Rev. Lett.}, title = {Enhanced strange metallicity due to hubbard-U coulomb repulsion}, volume = {134}, year = {2025}, }
• (2025). Energy relaxation and dynamics in the correlated metal Sr2RuO4 via terahertz two-dimensional coherent spectroscopy. PRL, 134(3), 036501. (www)

  @article{ , abstract = {Discriminating the effects of different kinds of scattering in strongly interacting metals is crucial in their understanding. While momentum or current relaxation can be readily probed via dc resistivity or linear terahertz (THz) spectroscopy, discriminating other kinds of scattering can be more challenging. In this Letter, we argue that the nonlinear optical technique of THz 2D coherent spectroscopy measures the energy relaxation rate in strongly interacting metals. We apply the technique to the Fermi liquid S r 2 ⁢ R u O 4 and observe two energy relaxation channels: a fast process ( ∼ 0 . 1 T H z ) that we interpret as energy loss to the phonon system and a much slower relaxation ( ≲ 1 G H z ) that we interpret as the relaxation of nonequilibrium phonons. Both rates are at least an order of magnitude slower than the momentum relaxation rate. We show how energy relaxation provides a unique diagnostic into certain kinds of scattering and among other aspects allows a measure of the dimensionless electron-phonon coupling constant. Our observations reveal the versatility of nonlinear THz spectroscopy to measure the energy relaxation dynamics in correlated metals and also highlights the need for improved theoretical understanding of such processes in interacting metals.}, archive = {J_PRL}, author = {David Barbalas and Ralph Romero, III and Dipanjan Chaudhuri and Fahad Mahmood and Hari P. Nair and Nathaniel J. Schreiber and Darrell G. Schlom and K. M. Shen and N. P. Armitage}, doi = {10.1103/PhysRevLett.134.036501}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036501}, shortjournal = {Phys. Rev. Lett.}, title = {Energy relaxation and dynamics in the correlated metal Sr2RuO4 via terahertz two-dimensional coherent spectroscopy}, volume = {134}, year = {2025}, }
• (2025). Dynamical theory of angle-resolved electron energy loss and gain spectroscopies of phonons and magnons in transmission electron microscopy including multiple scattering effects. PRL, 134(3), 036402. (www)

  @article{ , abstract = {We present a method for computing angle-resolved electron energy loss and gain spectroscopies for phonon and magnon excitations in transmission electron microscopy. Fractional scattering intensities are derived from the temperature-dependent time autocorrelation of the auxiliary electron beam wave function. This method captures both single and multiple scattering processes, as well as dynamical diffraction effects, while remaining computationally efficient and easy to parallelize.}, archive = {J_PRL}, author = {José Ángel Castellanos-Reyes and Paul M. Zeiger and Ján Rusz}, doi = {10.1103/PhysRevLett.134.036402}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036402}, shortjournal = {Phys. Rev. Lett.}, title = {Dynamical theory of angle-resolved electron energy loss and gain spectroscopies of phonons and magnons in transmission electron microscopy including multiple scattering effects}, volume = {134}, year = {2025}, }
• (2025). Design of intrinsic transparent conductors from a synergetic effect of symmetry and spatial-distribution forbidden transitions. PRL, 134(3), 036401. (www)

  @article{ , abstract = {Intrinsic transparent conductors (ITCs) correspond to a unique class of TCs that do not need intentional doping. This character can provide ITCs significant advantages by avoiding severe “doping bottlenecks” and dopant scattering usually encountered in conventional transparent conducting oxides (TCOs). However, the realization of ITCs generally requires the minimization of photon absorption and reflection in metallic conductors, which is difficult due to the gapless nature of their band structures. Here, based on first-principles calculations, we illustrate a feasible strategy to design optical transparency in metallic conductors by a synergetic effect of symmetry and spatial-distribution forbidden transitions between their energy bands around the Fermi level. The validity of this design strategy is demonstrated in a zero-dimensional electride, which exhibits both electrical conductivity and optical transparency in the ultraviolet spectrum. More interestingly, we find that this transmittance range can be tuned to the visible spectrum region by chemical substitutions in with the elements that have either larger electronegativity or smaller atomic radius. By examining dozens of possible cation substitutions via high-throughput calculations, we identify several promising candidates that have the potential as ITCs.}, archive = {J_PRL}, author = {Gui Wang and Ying Ning Du and Pu Huang and Zheng Fang Qian and Peng Zhang and Su-Huai Wei}, doi = {10.1103/PhysRevLett.134.036401}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036401}, shortjournal = {Phys. Rev. Lett.}, title = {Design of intrinsic transparent conductors from a synergetic effect of symmetry and spatial-distribution forbidden transitions}, volume = {134}, year = {2025}, }
• (2025). Orbital pumping incorporating both orbital angular momentum and position. PRL, 134(3), 036305. (www)

  @article{ , abstract = {We develop a theory of adiabatic orbital pumping, highlighting qualitative differences from spin pumping. An oscillating magnetic field pumps not only orbital angular momentum current, but also orbital angular position current. The latter, which has no spin counterpart, underscores the incompleteness of existing orbital torque theories. Importantly, both types of orbital currents can be detected as transverse electric voltages, which contain considerable second-harmonic components unlike in spin pumping. Moreover, orbital currents can be pumped by lattice dynamics that carry phonon angular momentum, implying that orbital currents can, in turn, induce phonon angular momentum. Our Letter open up new possibilities for generating orbital currents and provides a broader understanding of the interplay between spin, orbital, and phonon dynamics.}, archive = {J_PRL}, author = {Seungyun Han and Hye-Won Ko and Jung Hyun Oh and Hyun-Woo Lee and Kyung-Jin Lee and Kyoung-Whan Kim}, doi = {10.1103/PhysRevLett.134.036305}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036305}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital pumping incorporating both orbital angular momentum and position}, volume = {134}, year = {2025}, }
• (2025). Quantum correction to the orbital hall effect. PRL, 134(3), 036304. (www)

  @article{ , abstract = {Evaluations of the orbital Hall effect (OHE) have retained only interband matrix elements of the position operator. Here, we evaluate the OHE including all matrix elements of the position operator, including the technically challenging intraband elements. We recover previous results and find quantum corrections due to the noncommutativity of the position and velocity operators and interband matrix elements of the orbital angular momentum. The quantum corrections dominate the OHE responses of the topological antiferromagnet CuMnAs and of massive Dirac fermions.}, archive = {J_PRL}, author = {Hong Liu and James H. Cullen and Daniel P. Arovas and Dimitrie Culcer}, doi = {10.1103/PhysRevLett.134.036304}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036304}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum correction to the orbital hall effect}, volume = {134}, year = {2025}, }
• (2025). Ionic conductivity in disordered media: Molecular flexibility as a new paradigm to enhance ion motion in glassy electrolytes. PRL, 134(3), 036303. (www)

  @article{ , abstract = {We investigate the role of molecular flexibility on the electrical transport properties of model electrolytes containing ions and an underlying disordered network structure with changing connectedness. Rather than focusing on the effect of ion content in a stoichiometric network former (e.g., ), we explore the possibility of increasing the ratio (flexibility index ) in order to reduce connectivity and to promote the occurrence of flexible modes and topological degrees of freedom in the network structure. At fixed ion content and below a certain threshold modifier composition , topological constraint counting indicates that a mean-field stress-to-flexible transition is expected for a flexibility index , and an ion hopping model predicts a substantial increase of conductivity once . Molecular dynamics simulations on a typical amorphous electrolyte, independently and quantitatively confirm the prediction as anomalous changes with are obtained, and these manifest by waterlike diffusivity anomalies, and a substantial increase of ionic conductivity upon moderate change of . The analysis disentangles contributions from mobility and the free carrier rate in the electrical transport, and finally suggests that molecular flexibility can serve as an efficient way for conductivity enhancement in all solid-state batteries using amorphous electrolytes.}, archive = {J_PRL}, author = {M. Micoulaut}, doi = {10.1103/PhysRevLett.134.036303}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036303}, shortjournal = {Phys. Rev. Lett.}, title = {Ionic conductivity in disordered media: Molecular flexibility as a new paradigm to enhance ion motion in glassy electrolytes}, volume = {134}, year = {2025}, }
• (2025). Giant tunneling magnetoresistance based on spin-valley-mismatched ferromagnetic metals. PRL, 134(3), 036302. (www)

  @article{ , abstract = {Half metals, which are amenable to perfect spin filtering, can be utilized for high-magnetoresistive devices. However, available half metals are very limited. Here, we demonstrate that materials with intrinsic spin-valley-mismatched (SVM) states can be used to block charge transport, resembling half metals and leading to giant tunneling magnetoresistance. As an example, by using first-principles transport calculations, we show that ferromagnetic , and are such spin-valley-mismatched metals, and giant magnetoresistance of more than 99% can be realized in spin-valve van der Waals (vdW) junctions using these metals as electrodes. Owing to the intrinsic mismatch of spin states, the central-layer materials for the vdW junctions can be arbitrary nonmagnetic materials, in principle. Our research provides clear physical insights into the mechanism for high magnetoresistance and opens new avenues for the search and design of high-magnetoresistance devices.}, archive = {J_PRL}, author = {Kun Yan and Li Cheng and Yizhi Hu and Junjie Gao and Xiaolong Zou and Xiaobin Chen}, doi = {10.1103/PhysRevLett.134.036302}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036302}, shortjournal = {Phys. Rev. Lett.}, title = {Giant tunneling magnetoresistance based on spin-valley-mismatched ferromagnetic metals}, volume = {134}, year = {2025}, }
• (2025). Switching spin filling sequence in a bilayer graphene quantum dot through trigonal warping. PRL, 134(3), 036301. (www)

  @article{ , abstract = {We demonstrate a switchable electron shell structure in a bilayer graphene quantum dot by manipulating the trigonal warping effect upon electrical gating. Under a small perpendicular electric field, the lowest shell is sequentially filled with two spin-up and two spin-down electrons of opposite valleys. When increasing the electric field, an additional threefold minivalley degeneracy is generated so that the shell can be filled with 12 electrons with the first (last) six electrons having the same spin polarization. The switched spin filling sequence demonstrates the possibility of using the trigonal warping effect to electrically access and manipulate the spin degree of freedom in bilayer graphene.}, archive = {J_PRL}, author = {Guo-Quan Qin and Fang-Ming Jing and Tian-Yue Hao and Shun-Li Jiang and Zhuo-Zhi Zhang and Gang Cao and Xiang-Xiang Song and Guo-Ping Guo}, doi = {10.1103/PhysRevLett.134.036301}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {036301}, shortjournal = {Phys. Rev. Lett.}, title = {Switching spin filling sequence in a bilayer graphene quantum dot through trigonal warping}, volume = {134}, year = {2025}, }
• (2025). Fast radio bursts as precursor radio emission from monster shocks. PRL, 134(3), 035201. (www)

  @article{ , abstract = {It has been proposed recently that the breaking of magnetohydrodynamics (MHD) waves in the inner magnetosphere of strongly magnetized neutron stars can power different types of high-energy transients. Motivated by these considerations, we study the steepening and dissipation of a strongly magnetized fast magnetosonic wave propagating in a declining background magnetic field, by means of particle-in-cell simulations that encompass MHD scales. Our analysis confirms the formation of a monster shock as , that dissipates about half of the fast magnetosonic wave energy. It also reveals, for the first time, the generation of a high-frequency precursor wave by the monster shock, carrying a fraction of of the total energy dissipated at the shock. The spectrum of the precursor wave exhibits several sharp harmonic peaks, with frequencies in the gigahertz band under conditions anticipated in magnetars. Such signals may appear as fast radio bursts.}, archive = {J_PRL}, author = {A. Vanthieghem and A. Levinson}, doi = {10.1103/PhysRevLett.134.035201}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {035201}, shortjournal = {Phys. Rev. Lett.}, title = {Fast radio bursts as precursor radio emission from monster shocks}, volume = {134}, year = {2025}, }
• (2025). Pellet rocket effect in magnetic confinement fusion plasmas. PRL, 134(3), 035101. (www)

  @article{ , abstract = {Pellets of frozen material traveling into a magnetically confined fusion plasma are accelerated by the so-called pellet rocket effect. The nonuniform plasma heats the pellet ablation cloud asymmetrically, producing pressure-driven, rocketlike propulsion of the pellet. We present a semianalytical model of this process by perturbing a spherically symmetric ablation model. Predicted pellet accelerations match experimental estimates in current tokamaks ( ). Projections for ITER high-confinement scenarios ( ) indicate significantly shorter pellet penetration than expected without this effect, which could limit the effectiveness of disruption mitigation.}, archive = {J_PRL}, author = {Nico J. Guth and Oskar Vallhagen and Per Helander and Istvan Pusztai and Sarah L. Newton and Tünde Fülöp}, doi = {10.1103/PhysRevLett.134.035101}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {035101}, shortjournal = {Phys. Rev. Lett.}, title = {Pellet rocket effect in magnetic confinement fusion plasmas}, volume = {134}, year = {2025}, }
• (2025). Exogenous–Endogenous surfactant interaction yields heterogeneous spreading in complex branching networks. PRL, 134(3), 034001. (www)

  @article{ , abstract = {Experiments have shown that surfactant introduced to a liquid-filled maze can find the solution path. We reveal how the maze-solving dynamics arise from interactions between the added surfactant and endogenous surfactant present at the liquid surface. We simulate the dynamics using a nonlinear model solved with a discrete mimetic scheme on a graph. Endogenous surfactant transforms local spreading into a nonlocal problem with an omniscient view of the maze geometry, key to the maze-solving dynamics. Our results offer insight into surfactant-driven transport in complex networks such as lung airways.}, archive = {J_PRL}, author = {Richard Mcnair and Fernando Temprano-Coleto and François J. Peaudecerf and Frédéric Gibou and Paolo Luzzatto-Fegiz and Oliver E. Jensen and Julien R. Landel}, doi = {10.1103/PhysRevLett.134.034001}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {034001}, shortjournal = {Phys. Rev. Lett.}, title = {Exogenous–Endogenous surfactant interaction yields heterogeneous spreading in complex branching networks}, volume = {134}, year = {2025}, }
• (2025). Realization of topology-controlled photonic cavities in a valley photonic crystal. PRL, 134(3), 033803. (www)

  @article{ , abstract = {We report the experimental realization of a new type of topology-controlled photonic cavities in valley photonic crystals by adopting judiciously oriented mirrors to localize the valley-polarized edge states along their propagation path. By using microwave frequency- and time-domain measurements, we directly observe the strong confinement of electromagnetic energy at the mirror surface due to the extended time delay required for the valley index flipping. Moreover, we experimentally demonstrate that both the degree of energy localization and quality factors of the topology-controlled photonic cavities are determined by the valley-flipping time which is controlled by the topology of the mirror. These results extend and complement the current design paradigm of topological photonic cavities.}, archive = {J_PRL}, author = {Bei Yan and Baoliang Liao and Fulong Shi and Xiang Xi and Yuan Cao and Kexin Xiang and Yan Meng and Linyun Yang and Zhenxiao Zhu and Jingming Chen and Xiao-Dong Chen and Gui-Geng Liu and Baile Zhang and Zhen Gao}, doi = {10.1103/PhysRevLett.134.033803}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {033803}, shortjournal = {Phys. Rev. Lett.}, title = {Realization of topology-controlled photonic cavities in a valley photonic crystal}, volume = {134}, year = {2025}, }
• (2025). Observation of copropagating chiral zero modes in magnetic photonic crystals. PRL, 134(3), 033802. (www)

  @article{ , abstract = {Topological singularities, such as Weyl points (WPs) and Dirac points, can give rise to unidirectional propagation channels known as chiral zero modes (CZMs) when subject to a magnetic field. CZMs, as distinct zeroth Landau levels (bulk modes) with high degeneracy, are responsible for intriguing phenomena like the chiral anomaly in quantum systems. The propagation direction of each CZM is determined by both the applied magnetic field and the topological charge of the singularity point. While counterpropagating CZMs have been observed in 2D and 3D systems, the realization of copropagating CZMs has remained elusive. Here, we present the first experimental observation of copropagating CZMs in magnetic photonic crystals hosting a single pair of ideal Weyl points. By manipulating the crystal’s structural configuration and applying a uniform bias magnetic field, we spatially alter the locations of the WPs, creating pseudo-magnetic fields of opposite directions for different WPs. This arrangement results in a pair of CZMs that possess the same group velocity and copropagate. Our work opens up new possibilities for the topological manipulation of wave propagation and may lead to advancements in optical waveguides, switches, and various other applications.}, archive = {J_PRL}, author = {Zhongfu Li and Shaojie Ma and Shuwei Li and Oubo You and Yachao Liu and Qingdong Yang and Yuanjiang Xiang and Peiheng Zhou and Shuang Zhang}, doi = {10.1103/PhysRevLett.134.033802}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {033802}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of copropagating chiral zero modes in magnetic photonic crystals}, volume = {134}, year = {2025}, }
• (2025). Multistable kuramoto splay states in a crystal of mode-locked laser pulses. PRL, 134(3), 033801. (www)

  @article{ , abstract = {We demonstrate the existence of coexisting frequency combs in a harmonically mode-locked laser that we link to the splay phases of the Kuramoto model with short range interactions. These splay states are multistable and the laser may wander between them under the influence of stochastic forces. Consequently, the many pulses circulating in the cavity are not necessarily coherent with each other. As these partially disordered states for the phase of the field still feature regular intensity pulses, we term them as incoherent crystals of optical pulses. We provide evidence that the notion of coherence should be interpreted by comparing the duration of the measurement time with the Kramers’ escape time of each splay state. Our theoretical results are confirmed experimentally by performing high resolution spectral measurements via a heterodyne technique of a passively mode-locked vertical external-cavity surface-emitting laser.}, archive = {J_PRL}, author = {T. G. Seidel and A. Bartolo and A. Garnache and M. Giudici and M. Marconi and S. V. Gurevich and J. Javaloyes}, doi = {10.1103/PhysRevLett.134.033801}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {033801}, shortjournal = {Phys. Rev. Lett.}, title = {Multistable kuramoto splay states in a crystal of mode-locked laser pulses}, volume = {134}, year = {2025}, }
• (2025). Probing rotational decoherence with a trapped-ion planar rotor. PRL, 134(3), 033601. (www)

  @article{ , abstract = {The quantum rotor is one of the simplest model systems in quantum mechanics, but only in recent years has theoretical work revealed general fundamental scaling laws for its decoherence. For example, a superposition of orientations decoheres at a rate proportional to the sine squared of the angle between them. Here, we observe scaling laws for rotational decoherence dynamics for the first time, using a diameter planar rotor composed of two Paul-trapped ions. We prepare the rotational motion of the ion crystal into superpositions of angular momentum with well-defined differences ranging from , and measure the rate of decoherence. We also tune the system-environment interaction strength by introducing resonant electric field noise. The observed scaling relationships for decoherence are in excellent agreement with recent theoretical work, and are directly relevant to the growing development of rotor-based quantum applications.}, archive = {J_PRL}, author = {Neil Glikin and Benjamin A. Stickler and Ryan Tollefsen and Sara Mouradian and Neha Yadav and Erik Urban and Klaus Hornberger and Hartmut Häffner}, doi = {10.1103/PhysRevLett.134.033601}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {033601}, shortjournal = {Phys. Rev. Lett.}, title = {Probing rotational decoherence with a trapped-ion planar rotor}, volume = {134}, year = {2025}, }
• (2025). Lattice light shift evaluations in a dual-ensemble yb optical lattice clock. PRL, 134(3), 033201. (www)

  @article{ , abstract = {In state-of-the-art optical lattice clocks, beyond-electric-dipole polarizability terms lead to a breakdown of magic wavelength trapping. In this Letter, we report a novel approach to evaluate lattice light shifts, specifically addressing recent discrepancies in the atomic multipolarizability term between experimental techniques and theoretical calculations. We combine imaging and multi-ensemble techniques to evaluate lattice light shift atomic coefficients, leveraging comparisons in a dual-ensemble lattice clock to rapidly evaluate differential frequency shifts. Further, we demonstrate application of a running wave field to probe both the multipolarizability and hyperpolarizability coefficients, establishing a new technique for future lattice light shift evaluations.}, archive = {J_PRL}, author = {Tobias Bothwell and Benjamin D. Hunt and Jacob L. Siegel and Youssef S. Hassan and Tanner Grogan and Takumi Kobayashi and Kurt Gibble and Sergey G. Porsev and Marianna S. Safronova and Roger C. Brown and Kyle Beloy and Andrew D. Ludlow}, doi = {10.1103/PhysRevLett.134.033201}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {033201}, shortjournal = {Phys. Rev. Lett.}, title = {Lattice light shift evaluations in a dual-ensemble yb optical lattice clock}, volume = {134}, year = {2025}, }
• (2025). Experimental evidence for double intermolecular coulombic decay in bio-relevant molecular dimers. PRL, 134(3), 033001. (www)

  @article{ , abstract = {We report the experimental observation of double intermolecular Coulombic decay (dICD) and reveal its potential for radiation biology in some prototypical molecular dimers consisting of benzene, pyridine, and water. In dICD, the inner-shell vacancy is filled by an electron from an outer shell and the energy released is transferred to doubly ionize the neighboring molecule with the emission of two low-energy electrons. The system further relaxes by a three-body Coulomb explosion process, e.g., C H + 3 + C 5 ⁢ H + 3 + C 6 ⁢ H + 6 for benzene dimer. Through multicoincidence momentum imaging, we find that dICD is an efficient relaxation pathway for the Auger-accessible inner-shell ionization states in molecular complexes. Moreover, this ultrafast decay mechanism causes a direct breaking of the aromatic rings, which is observed to be a general phenomenon occurring in biological systems and thus can play an important role in radiation biology.}, archive = {J_PRL}, author = {Xintai Hao and Xiaorui Xue and Jiaqi Zhou and Xinyu Zhang and Xiaokai Li and Qingrui Zeng and Qibo Ma and Yongtao Zhao and Chuncheng Wang and Sizuo Luo and Dajun Ding and Xueguang Ren}, doi = {10.1103/PhysRevLett.134.033001}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {033001}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental evidence for double intermolecular coulombic decay in bio-relevant molecular dimers}, volume = {134}, year = {2025}, }
• (2025). Revisiting the helium isotope-shift puzzle with improved uncertainties from nuclear structure corrections. PRL, 134(3), 032502. (www)

  @article{ , abstract = {Measurements of the difference between the squared charge radii of the helion ( nucleus) and the particle ( nucleus) have been characterized by longstanding tensions recently spotlighted in the discrepancy of the extractions from ordinary atoms versus those from muonic atoms [Karsten Schuhmann et al. , arXiv:2305.11679 ]. Here, we present a novel analysis of uncertainties in nuclear structure corrections that must be supplied by theory to enable the extraction of the difference in radii from spectroscopic experiments. We use modern Bayesian inference techniques to quantify uncertainties stemming from the truncation of the chiral effective field theory expansion of the nuclear force for both muonic and ordinary atoms. With the new nuclear structure input, the helium isotope-shift puzzle cannot be explained, rather, it is reinforced to a discrepancy.}, archive = {J_PRL}, author = {Simone Salvatore Li Muli and Thomas R. Richardson and Sonia Bacca}, doi = {10.1103/PhysRevLett.134.032502}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {032502}, shortjournal = {Phys. Rev. Lett.}, title = {Revisiting the helium isotope-shift puzzle with improved uncertainties from nuclear structure corrections}, volume = {134}, year = {2025}, }
• (2025). Spin-triplet pairing in heavy nuclei is stable against deformation. PRL, 134(3), 032501. (www)

  @article{ , abstract = {Any experimental evidence of nucleons paired in spin-triplet states will confirm the existence of an exotic phase of nuclear systems. This type of nuclear superfluidity has been hypothesized in heavy nuclei, where the antagonizing spin-orbit effects are damped, and there it oftentimes coexists with traditional spin-singlet pairing, leading to the possibility of mixed-spin pairing. Realistic nuclear deformation, not considered in such studies, could make-or-break these proposals, since its effect on triplet pairing, and the competition (and coexistence) of the two superfluid phases, was expected to be crucial. We report on a thorough study on the effect of deformation on triplet, singlet, and mixed-spin pairing in the relevant region of the nuclear chart. We find that, at low isospin asymmetries, spin-triplet pairing is enhanced by deformation, while below the proton-drip line, the novel superfluid phase survives alongside the usual spin-singlet pairing. These results suggest that spin-triplet superfluidity exists in realistic nuclei and can be probed in the lab.}, archive = {J_PRL}, author = {Georgios Palkanoglou and Michael Stuck and Alexandros Gezerlis}, doi = {10.1103/PhysRevLett.134.032501}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {032501}, shortjournal = {Phys. Rev. Lett.}, title = {Spin-triplet pairing in heavy nuclei is stable against deformation}, volume = {134}, year = {2025}, }
• (2025). Observation of exotic j/ψϕ resonant structure in diffractive processes in proton-proton collisions. PRL, 134(3), 031902. (www)

  @article{ , abstract = {The first study of J / ψ ϕ production in diffractive processes in proton-proton collisions is presented. The study is based on an LHCb dataset recorded at center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5 fb − 1 . The data disfavor a nonresonant J / ψ ϕ production but are consistent with a resonant model including several resonant states observed previously only in B + → J / ψ ϕ K + decays. The χ c 0 ( 4500 ) state is observed with a significance over 6 σ and the χ c 1 ( 4274 ) is confirmed with a significance of more than 4 σ .}, archive = {J_PRL}, author = {LHCb Collaboration and R. Aaij and A. S. W. Abdelmotteleb and C. Abellan Beteta and F. Abudinén and T. Ackernley and A. A. Adefisoye and B. Adeva and M. Adinolfi and P. Adlarson and C. Agapopoulou and C. A. Aidala and Z. Ajaltouni and S. Akar and K. Akiba and P. Albicocco and J. Albrecht and F. Alessio and M. Alexander and Z. Aliouche and P. Alvarez Cartelle and R. Amalric and S. Amato and J. L. Amey and Y. Amhis and L. An and L. Anderlini and M. Andersson and A. Andreianov and P. Andreola and M. Andreotti and D. Andreou and A. Anelli and D. Ao and F. Archilli and M. Argenton and S. Arguedas Cuendis and A. Artamonov and M. Artuso and E. Aslanides and M. Atzeni and B. Audurier and D. Bacher and I. Bachiller Perea and S. Bachmann and M. Bachmayer and J. J. Back and P. Baladron Rodriguez and V. Balagura and W. Baldini and J. Baptista de Souza Leite and M. Barbetti and I. R. Barbosa and R. J. Barlow and S. Barsuk and W. Barter and M. Bartolini and J. Bartz and F. Baryshnikov and J. M. Basels and G. Bassi and B. Batsukh and A. Battig and A. Bay and A. Beck and M. Becker and F. Bedeschi and I. B. Bediaga and A. Beiter and S. Belin and V. Bellee and K. Belous and I. Belov and I. Belyaev and G. Benane and G. Bencivenni and E. Ben-Haim and A. Berezhnoy and R. Bernet and S. Bernet Andres and C. Bertella and A. Bertolin and C. Betancourt and F. Betti and J. Bex and Ia. Bezshyiko and J. Bhom and M. S. Bieker and N. V. Biesuz and P. Billoir and A. Biolchini and M. Birch and F. C. R. Bishop and A. Bitadze and A. Bizzeti and T. Blake and F. Blanc and J. E. Blank and S. Blusk and V. Bocharnikov and J. A. Boelhauve and O. Boente Garcia and T. Boettcher and A. Bohare and A. Boldyrev and C. S. Bolognani and R. Bolzonella and N. Bondar and F. Borgato and S. Borghi and M. Borsato and J. T. Borsuk and S. A. Bouchiba and T. J. V. Bowcock and A. Boyer and C. Bozzi and M. J. Bradley and A. Brea Rodriguez and N. Breer and J. Brodzicka and A. Brossa Gonzalo and J. Brown and D. Brundu and E. Buchanan and A. Buonaura and L. Buonincontri and A. T. Burke and C. Burr and A. Bursche and A. Butkevich and J. S. Butter and J. Buytaert and W. Byczynski and S. Cadeddu and H. Cai and R. Calabrese and L. Calefice and S. Cali and M. Calvi and M. Calvo Gomez and J. I. Cambon Bouzas and P. Campana and D. H. Campora Perez and A. F. Campoverde Quezada and S. Capelli and L. Capriotti and R. Caravaca-Mora and A. Carbone and L. Carcedo Salgado and R. Cardinale and A. Cardini and P. Carniti and L. Carus and A. Casais Vidal and R. Caspary and G. Casse and J. Castro Godinez and M. Cattaneo and G. Cavallero and V. Cavallini and S. Celani and J. Cerasoli and D. Cervenkov and S. Cesare and A. J. Chadwick and I. Chahrour and M. Charles and Ph. Charpentier and C. A. Chavez Barajas and M. Chefdeville and C. Chen and S. Chen and Z. Chen and A. Chernov and S. Chernyshenko and V. Chobanova and S. Cholak and M. Chrzaszcz and A. Chubykin and V. Chulikov and P. Ciambrone and X. Cid Vidal and G. Ciezarek and P. Cifra and P. E. L. Clarke and M. Clemencic and H. V. Cliff and J. Closier and C. Cocha Toapaxi and V. Coco and J. Cogan and E. Cogneras and L. Cojocariu and P. Collins and T. Colombo and A. Comerma-Montells and L. Congedo and A. Contu and N. Cooke and I. Corredoira and A. Correia and G. Corti and J. J. Cottee Meldrum and B. Couturier and D. C. Craik and M. Cruz Torres and E. Curras Rivera and R. Currie and C. L. Da Silva and S. Dadabaev and L. Dai and X. Dai and E. Dall’Occo and J. Dalseno and C. D’Ambrosio and J. Daniel and A. Danilina and P. d’Argent and A. Davidson and J. E. Davies and A. Davis and O. De Aguiar Francisco and C. De Angelis and F. De Benedetti and J. de Boer and K. De Bruyn and S. De Capua and M. De Cian and U. De Freitas Carneiro Da Graca and E. De Lucia and J. M. De Miranda and L. De Paula and M. De Serio and D. De Simone and P. De Simone and F. De Vellis and J. A. de Vries and F. Debernardis and D. Decamp and V. Dedu and L. Del Buono and B. Delaney and H.-P. Dembinski and J. Deng and V. Denysenko and O. Deschamps and F. Dettori and B. Dey and P. Di Nezza and I. Diachkov and S. Didenko and S. Ding and L. Dittmann and V. Dobishuk and A. D. Docheva and A. Dolmatov and C. Dong and A. M. Donohoe and F. Dordei and A. C. dos Reis and A. D. Dowling and A. G. Downes and W. Duan and P. Duda and M. W. Dudek and L. Dufour and V. Duk and P. Durante and M. M. Duras and J. M. Durham and O. D. Durmus and A. Dziurda and A. Dzyuba and S. Easo and E. Eckstein and U. Egede and A. Egorychev and V. Egorychev and S. Eisenhardt and E. Ejopu and S. Ek-In and L. Eklund and M. Elashri and J. Ellbracht and S. Ely and A. Ene and E. Epple and S. Escher and J. Eschle and S. Esen and T. Evans and F. Fabiano and L. N. Falcao and Y. Fan and B. Fang and L. Fantini and M. Faria and K. Farmer and D. Fazzini and L. Felkowski and M. Feng and M. Feo and M. Fernandez Gomez and A. D. Fernez and F. Ferrari and F. Ferreira Rodrigues and S. Ferreres Sole and M. Ferrillo and M. Ferro-Luzzi and S. Filippov and R. A. Fini and M. Fiorini and K. M. Fischer and D. S. Fitzgerald and C. Fitzpatrick and F. Fleuret and M. Fontana and L. F. Foreman and R. Forty and D. Foulds-Holt and M. Franco Sevilla and M. Frank and E. Franzoso and G. Frau and C. Frei and D. A. Friday and J. Fu and Q. Fuehring and Y. Fujii and T. Fulghesu and E. Gabriel and G. Galati and M. D. Galati and A. Gallas Torreira and D. Galli and S. Gambetta and M. Gandelman and P. Gandini and H. Gao and R. Gao and Y. Gao and M. Garau and L. M. Garcia Martin and P. Garcia Moreno and J. García Pardiñas and K. G. Garg and L. Garrido and C. Gaspar and R. E. Geertsema and L. L. Gerken and E. Gersabeck and M. Gersabeck and T. Gershon and Z. Ghorbanimoghaddam and L. Giambastiani and F. I. Giasemis and V. Gibson and H. K. Giemza and A. L. Gilman and M. Giovannetti and A. Gioventù and P. Gironella Gironell and C. Giugliano and M. A. Giza and E. L. Gkougkousis and F. C. Glaser and V. V. Gligorov and C. Göbel and E. Golobardes and D. Golubkov and A. Golutvin and A. Gomes and S. Gomez Fernandez and F. Goncalves Abrantes and M. Goncerz and G. Gong and J. A. Gooding and I. V. Gorelov and C. Gotti and J. P. Grabowski and L. A. Granado Cardoso and E. Graugés and E. Graverini and L. Grazette and G. Graziani and A. T. Grecu and L. M. Greeven and N. A. Grieser and L. Grillo and S. Gromov and C. Gu and M. Guarise and M. Guittiere and V. Guliaeva and P. A. Günther and A.-K. Guseinov and E. Gushchin and Y. Guz and T. Gys and K. Habermann and T. Hadavizadeh and C. Hadjivasiliou and G. Haefeli and C. Haen and J. Haimberger and M. Hajheidari and M. M. Halvorsen and P. M. Hamilton and J. Hammerich and Q. Han and X. Han and S. Hansmann-Menzemer and L. Hao and N. Harnew and T. Harrison and M. Hartmann and J. He and K. Heijhoff and F. Hemmer and C. Henderson and R. D. L. Henderson and A. M. Hennequin and K. Hennessy and L. Henry and J. Herd and P. Herrero Gascon and J. Heuel and A. Hicheur and G. Hijano Mendizabal and D. Hill and S. E. Hollitt and J. Horswill and R. Hou and Y. Hou and N. Howarth and J. Hu and W. Hu and X. Hu and W. Huang and W. Hulsbergen and R. J. Hunter and M. Hushchyn and D. Hutchcroft and D. Ilin and P. Ilten and A. Inglessi and A. Iniukhin and A. Ishteev and K. Ivshin and R. Jacobsson and H. Jage and S. J. Jaimes Elles and S. Jakobsen and E. Jans and B. K. Jashal and A. Jawahery and V. Jevtic and E. Jiang and X. Jiang and Y. Jiang and Y. J. Jiang and M. John and D. Johnson and C. R. Jones and T. P. Jones and S. Joshi and B. Jost and N. Jurik and I. Juszczak and D. Kaminaris and S. Kandybei and Y. Kang and M. Karacson and D. Karpenkov and A. Kauniskangas and J. W. Kautz and F. Keizer and M. Kenzie and T. Ketel and B. Khanji and A. Kharisova and S. Kholodenko and G. Khreich and T. Kirn and V. S. Kirsebom and O. Kitouni and S. Klaver and N. Kleijne and K. Klimaszewski and M. R. Kmiec and S. Koliiev and L. Kolk and A. Konoplyannikov and P. Kopciewicz and P. Koppenburg and M. Korolev and I. Kostiuk and O. Kot and S. Kotriakhova and A. Kozachuk and P. Kravchenko and L. Kravchuk and M. Kreps and S. Kretzschmar and P. Krokovny and W. Krupa and W. Krzemien and J. Kubat and S. Kubis and W. Kucewicz and M. Kucharczyk and V. Kudryavtsev and E. Kulikova and A. Kupsc and B. K. Kutsenko and D. Lacarrere and A. Lai and A. Lampis and D. Lancierini and C. Landesa Gomez and J. J. Lane and R. Lane and C. Langenbruch and J. Langer and O. Lantwin and T. Latham and F. Lazzari and C. Lazzeroni and R. Le Gac and R. Lefèvre and A. Leflat and S. Legotin and M. Lehuraux and E. Lemos Cid and O. Leroy and T. Lesiak and B. Leverington and A. Li and H. Li and K. Li and L. Li and P. Li and P.-R. Li and S. Li and T. Li and Y. Li and Z. Li and Z. Lian and X. Liang and S. Libralon and C. Lin and T. Lin and R. Lindner and V. Lisovskyi and R. Litvinov and F. L. Liu and G. Liu and K. Liu and Q. Liu and S. Liu and Y. Liu and Y. L. Liu and A. Lobo Salvia and A. Loi and J. Lomba Castro and T. Long and J. H. Lopes and A. Lopez Huertas and S. López Soliño and G. H. Lovell and C. Lucarelli and D. Lucchesi and S. Luchuk and M. Lucio Martinez and V. Lukashenko and Y. Luo and A. Lupato and E. Luppi and K. Lynch and X.-R. Lyu and G. M. Ma and R. Ma and S. Maccolini and F. Machefert and F. Maciuc and B. Mack and I. Mackay and L. M. Mackey and L. R. Madhan Mohan and M. M. Madurai and A. Maevskiy and D. Magdalinski and D. Maisuzenko and M. W. Majewski and J. J. Malczewski and S. Malde and B. Malecki and L. Malentacca and A. Malinin and T. Maltsev and G. Manca and G. Mancinelli and C. Mancuso and R. Manera Escalero and D. Manuzzi and D. Marangotto and J. F. Marchand and R. Marchevski and U. Marconi and S. Mariani and C. Marin Benito and J. Marks and A. M. Marshall and P. J. Marshall and G. Martelli and G. Martellotti and L. Martinazzoli and M. Martinelli and D. Martinez Santos and F. Martinez Vidal and A. Massafferri and M. Materok and R. Matev and A. Mathad and V. Matiunin and C. Matteuzzi and K. R. Mattioli and A. Mauri and E. Maurice and J. Mauricio and P. Mayencourt and M. Mazurek and M. McCann and L. Mcconnell and T. H. McGrath and N. T. McHugh and A. McNab and R. McNulty and B. Meadows and G. Meier and D. Melnychuk and M. Merk and A. Merli and L. Meyer Garcia and D. Miao and H. Miao and M. Mikhasenko and D. A. Milanes and A. Minotti and E. Minucci and T. Miralles and B. Mitreska and D. S. Mitzel and A. Modak and A. Mödden and R. A. Mohammed and R. D. Moise and S. Mokhnenko and T. Mombächer and M. Monk and S. Monteil and A. Morcillo Gomez and G. Morello and M. J. Morello and M. P. Morgenthaler and A. B. Morris and A. G. Morris and R. Mountain and H. Mu and Z. M. Mu and E. Muhammad and F. Muheim and M. Mulder and K. Müller and F. Muñoz-Rojas and R. Murta and P. Naik and T. Nakada and R. Nandakumar and T. Nanut and I. Nasteva and M. Needham and N. Neri and S. Neubert and N. Neufeld and P. Neustroev and J. Nicolini and D. Nicotra and E. M. Niel and N. Nikitin and P. Nogga and N. S. Nolte and C. Normand and J. Novoa Fernandez and G. Nowak and C. Nunez and H. N. Nur and A. Oblakowska-Mucha and V. Obraztsov and T. Oeser and S. Okamura and A. Okhotnikov and R. Oldeman and F. Oliva and M. Olocco and C. J. G. Onderwater and R. H. O’Neil and J. M. Otalora Goicochea and P. Owen and A. Oyanguren and O. Ozcelik and K. O. Padeken and B. Pagare and P. R. Pais and T. Pajero and A. Palano and M. Palutan and G. Panshin and L. Paolucci and A. Papanestis and M. Pappagallo and L. L. Pappalardo and C. Pappenheimer and C. Parkes and B. Passalacqua and G. Passaleva and D. Passaro and A. Pastore and M. Patel and J. Patoc and C. Patrignani and C. J. Pawley and A. Pellegrino and M. Pepe Altarelli and S. Perazzini and D. Pereima and A. Pereiro Castro and P. Perret and A. Perro and K. Petridis and A. Petrolini and S. Petrucci and J. P. Pfaller and H. Pham and L. Pica and M. Piccini and B. Pietrzyk and G. Pietrzyk and D. Pinci and F. Pisani and M. Pizzichemi and V. Placinta and M. Plo Casasus and F. Polci and M. Poli Lener and A. Poluektov and N. Polukhina and I. Polyakov and E. Polycarpo and S. Ponce and D. Popov and S. Poslavskii and K. Prasanth and C. Prouve and V. Pugatch and G. Punzi and W. Qian and N. Qin and S. Qu and R. Quagliani and N. V. Raab and R. I. Rabadan Trejo and J. H. Rademacker and M. Rama and M. Ramírez García and M. Ramos Pernas and M. S. Rangel and F. Ratnikov and G. Raven and M. Rebollo De Miguel and F. Redi and J. Reich and F. Reiss and Z. Ren and P. K. Resmi and R. Ribatti and G. R. Ricart and D. Riccardi and S. Ricciardi and K. Richardson and M. Richardson-Slipper and K. Rinnert and P. Robbe and G. Robertson and E. Rodrigues and E. Rodriguez Fernandez and J. A. Rodriguez Lopez and E. Rodriguez Rodriguez and A. Rogovskiy and D. L. Rolf and P. Roloff and V. Romanovskiy and M. Romero Lamas and A. Romero Vidal and G. Romolini and F. Ronchetti and M. Rotondo and S. R. Roy and M. S. Rudolph and T. Ruf and M. Ruiz Diaz and R. A. Ruiz Fernandez and J. Ruiz Vidal and A. Ryzhikov and J. Ryzka and J. J. Saavedra-Arias and J. J. Saborido Silva and R. Sadek and N. Sagidova and D. Sahoo and N. Sahoo and B. Saitta and M. Salomoni and C. Sanchez Gras and I. Sanderswood and R. Santacesaria and C. Santamarina Rios and M. Santimaria and L. Santoro and E. Santovetti and A. Saputi and D. Saranin and G. Sarpis and M. Sarpis and A. Sarti and C. Satriano and A. Satta and M. Saur and D. Savrina and H. Sazak and L. G. Scantlebury Smead and A. Scarabotto and S. Schael and S. Scherl and A. M. Schertz and M. Schiller and H. Schindler and M. Schmelling and B. Schmidt and S. Schmitt and H. Schmitz and O. Schneider and A. Schopper and N. Schulte and S. Schulte and M. H. Schune and R. Schwemmer and G. Schwering and B. Sciascia and A. Sciuccati and S. Sellam and A. Semennikov and T. Senger and M. Senghi Soares and A. Sergi and N. Serra and L. Sestini and A. Seuthe and Y. Shang and D. M. Shangase and M. Shapkin and R. S. Sharma and I. Shchemerov and L. Shchutska and T. Shears and L. Shekhtman and Z. Shen and S. Sheng and V. Shevchenko and B. Shi and E. B. Shields and Y. Shimizu and E. Shmanin and R. Shorkin and J. D. Shupperd and R. Silva Coutinho and G. Simi and S. Simone and N. Skidmore and T. Skwarnicki and M. W. Slater and J. C. Smallwood and E. Smith and K. Smith and M. Smith and A. Snoch and L. Soares Lavra and M. D. Sokoloff and F. J. P. Soler and A. Solomin and A. Solovev and I. Solovyev and R. Song and Y. Song and Y. S. Song and F. L. Souza De Almeida and B. Souza De Paula and E. Spadaro Norella and E. Spedicato and J. G. Speer and E. Spiridenkov and P. Spradlin and V. Sriskaran and F. Stagni and M. Stahl and S. Stahl and S. Stanislaus and E. N. Stein and O. Steinkamp and O. Stenyakin and H. Stevens and D. Strekalina and Y. Su and F. Suljik and J. Sun and L. Sun and Y. Sun and W. Sutcliffe and P. N. Swallow and F. Swystun and A. Szabelski and T. Szumlak and Y. Tan and S. Taneja and M. D. Tat and A. Terentev and F. Terzuoli and F. Teubert and E. Thomas and D. J. D. Thompson and H. Tilquin and V. Tisserand and S. T’Jampens and M. Tobin and L. Tomassetti and G. Tonani and X. Tong and D. Torres Machado and L. Toscano and D. Y. Tou and C. Trippl and G. Tuci and N. Tuning and L. H. Uecker and A. Ukleja and D. J. Unverzagt and E. Ursov and A. Usachov and A. Ustyuzhanin and U. Uwer and V. Vagnoni and A. Valassi and G. Valenti and N. Valls Canudas and H. Van Hecke and E. van Herwijnen and C. B. Van Hulse and R. Van Laak and M. van Veghel and R. Vazquez Gomez and P. Vazquez Regueiro and C. Vázquez Sierra and S. Vecchi and J. J. Velthuis and M. Veltri and A. Venkateswaran and M. Vesterinen and M. Vieites Diaz and X. Vilasis-Cardona and E. Vilella Figueras and A. Villa and P. Vincent and F. C. Volle and D. vom Bruch and V. Vorobyev and N. Voropaev and K. Vos and G. Vouters and C. Vrahas and J. Wagner and J. Walsh and E. J. Walton and G. Wan and C. Wang and G. Wang and J. Wang and M. Wang and N. W. Wang and R. Wang and X. Wang and X. W. Wang and Y. Wang and Z. Wang and J. A. Ward and M. Waterlaat and N. K. Watson and D. Websdale and Y. Wei and B. D. C. Westhenry and D. J. White and M. Whitehead and A. R. Wiederhold and D. Wiedner and G. Wilkinson and M. K. Wilkinson and M. Williams and M. R. J. Williams and R. Williams and F. F. Wilson and W. Wislicki and M. Witek and L. Witola and C. P. Wong and G. Wormser and S. A. Wotton and H. Wu and J. Wu and Y. Wu and K. Wyllie and S. Xian and Z. Xiang and Y. Xie and A. Xu and J. Xu and L. Xu and M. Xu and Z. Xu and D. Yang and S. Yang and X. Yang and Y. Yang and Z. Yang and V. Yeroshenko and H. Yeung and H. Yin and C. Y. Yu and J. Yu and X. Yuan and E. Zaffaroni and M. Zavertyaev and M. Zdybal and M. Zeng and C. Zhang and D. Zhang and J. Zhang and L. Zhang and S. Zhang and Y. Zhang and Y. Z. Zhang and Y. Zhao and A. Zharkova and A. Zhelezov and X. Z. Zheng and Y. Zheng and T. Zhou and X. Zhou and Y. Zhou and V. Zhovkovska and L. Z. Zhu and X. Zhu and V. Zhukov and J. Zhuo and Q. Zou and D. Zuliani and G. Zunica}, doi = {10.1103/PhysRevLett.134.031902}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031902}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of exotic j/ψϕ resonant structure in diffractive processes in proton-proton collisions}, volume = {134}, year = {2025}, }
• (2025). Complete next-to-leading order QCD corrections to ZZ production in gluon fusion. PRL, 134(3), 031901. (www)

  @article{ , abstract = {We calculate the complete next-to-leading order (NLO) QCD corrections to loop-induced g g → Z Z production including full top-quark mass effects. The two-loop virtual corrections are obtained by combining analytic results for the massless, Higgs-mediated, and one-loop factorizable contributions with numerically computed amplitudes containing the top-quark mass. We show that the choice of subtraction scheme for the virtual contribution impacts the precision with which the virtual contribution must be evaluated in order to obtain sufficiently precise phenomenological predictions. For direct production through a massive top-quark loop, we observe that the relative NLO corrections are large. The direct massive and Higgs-mediated contributions individually increase relative to the massless production at high diboson invariant mass, but interfere destructively with each other. At the Large Hadron Collider, the NLO corrections to the gluon channel give a sizable contribution to the p p → Z Z + X cross section at N 3 LO .}, archive = {J_PRL}, author = {Bakul Agarwal and Stephen Jones and Matthias Kerner and Andreas von Manteuffel}, doi = {10.1103/PhysRevLett.134.031901}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031901}, shortjournal = {Phys. Rev. Lett.}, title = {Complete next-to-leading order QCD corrections to ZZ production in gluon fusion}, volume = {134}, year = {2025}, }
• (2025). Symmetric mass generation with four SU(2) doublet fermions. PRL, 134(3), 031602. (www)

  @article{ , abstract = {We study a single exactly massless staggered fermion in the fundamental representation of an SU(2) gauge group. We utilize an nHYP-smeared fermion action supplemented with additional heavy Pauli-Villars fields that serve to decrease lattice artifacts. The phase diagram exhibits a clear two-phase structure with a conformal phase at weak coupling and a novel new phase, the symmetric mass generation (SMG) phase, appearing at strong coupling. The SMG phase is confining with all states gapped and chiral symmetry unbroken. Our finite size scaling analysis provides strong evidence that the phase transition between these two phases is continuous, which would allow for the existence of a continuum SMG phase. Furthermore, the renormalization group flows are consistent with a β function that vanishes quadratically at the new fixed point, suggesting that the N f = 4 flavor SU(2) gauge theory lies at the opening of the conformal window.}, archive = {J_PRL}, author = {Nouman Butt and Simon Catterall and Anna Hasenfratz}, doi = {10.1103/PhysRevLett.134.031602}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031602}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetric mass generation with four SU(2) doublet fermions}, volume = {134}, year = {2025}, }
• (2025). Hidden zeros are equivalent to enhanced ultraviolet scaling, and lead to unique amplitudes in tr(ϕ3) theory. PRL, 134(3), 031601. (www)

  @article{ , abstract = {We investigate the hidden amplitude zeros which describe a nontrivial vanishing of scattering amplitudes on special external kinematics. We first prove that every type of hidden zero is equivalent to what we call a “subset” enhanced scaling under Britto-Cachazo-Feng-Witten shifts for any rational function built from planar Lorentz invariants X i j = ( p i + p i + 1 + ⋯ + p j − 1 ) 2 . This directly applies to Tr ( ϕ 3 ) , nonlinear sigma models, or Yang-Mills-scalar amplitudes, revealing a novel type of enhanced UV scaling in these theories. We also use this observation to prove the conjecture that Tr ( ϕ 3 ) amplitudes are uniquely fixed by the zeros, up to an overall normalization, when assuming an ordered and local propagator structure and trivial numerators. In this context, unitarity (residue factorization) may be viewed as a consequence of the zeros. For Yang-Mills theory, we conjecture the zeros, combined with the Bern-Carrasco-Johansson color-kinematic duality in the form of amplitude relations, uniquely fix the ⌊ n / 2 ⌋ distinct polarization structures of n -point gluon amplitudes. Our approach opens a new avenue for understanding previous similar uniqueness results, and also extending them beyond tree level for the first time.}, archive = {J_PRL}, author = {Laurentiu Rodina}, doi = {10.1103/PhysRevLett.134.031601}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031601}, shortjournal = {Phys. Rev. Lett.}, title = {Hidden zeros are equivalent to enhanced ultraviolet scaling, and lead to unique amplitudes in tr(ϕ3) theory}, volume = {134}, year = {2025}, }
• (2025). Testing mirror symmetry in the universe with LIGO-virgo black-hole mergers. PRL, 134(3), 031402. (www)

  @article{ , abstract = {Certain precessing black-hole mergers produce gravitational waves with net circular polarization, understood as an imbalance between right- and left-handed amplitudes. According to the cosmological principle, such emission must average to zero across all binary mergers in our Universe to preserve mirror-reflection symmetry at very large scales. We present a new independent gravitational-wave test of this hypothesis. Using a novel observable based on the Chern-Pontryagin pseudoscalar, we measure the emission of net circular polarization across 47 black-hole mergers recently analyzed by [T. Islam et al. , arXiv:2309.14473 .] with a state-of-the art model for precessing black-hole mergers in general relativity. The average value obtained is consistent with zero. Remarkably, however, we find that at least 82% of the analyzed sources must have produced net circular polarization. Of these, GW200129 shows strong evidence for mirror asymmetry, with a Bayes factor of 12.6 or, equivalently, 93.1% probability. We obtain consistent (although stronger) results of 97.5% and 94.3%, respectively, using public results on this event from [M. Hannam et al. , Nature (London) 610 , 652 (2022) .] and performing our own parameter inference. This finding further implies evidence of astrophysical sources that can spontaneously emit circularly polarized photons by quantum effects. Forthcoming black-hole merger detections will enable stronger constraints on large-scale mirror asymmetry and the cosmological principle.}, archive = {J_PRL}, author = {Juan Calderón Bustillo and Adrian del Rio and Nicolas Sanchis-Gual and Koustav Chandra and Samson H. W. Leong}, doi = {10.1103/PhysRevLett.134.031402}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031402}, shortjournal = {Phys. Rev. Lett.}, title = {Testing mirror symmetry in the universe with LIGO-virgo black-hole mergers}, volume = {134}, year = {2025}, }
• (2025). Optimal reconstruction of the hellings and downs correlation. PRL, 134(3), 031401. (www)

  @article{ , abstract = {Pulsar timing arrays (PTAs) detect gravitational waves (GWs) via the correlations they create in the arrival times of pulses from different pulsars. The mean correlation, a function of the angle between the directions to two pulsars, was predicted in 1983 by Hellings and Downs (HD). Observation of this angular pattern is crucial evidence that GWs are present, so PTAs “reconstruct the HD curve” by estimating the correlation using pulsar pairs separated by similar angles. Several studies have examined the amount by which this curve is expected to differ from the HD mean. The variance arises because (a) a finite set of pulsars at specific sky locations is used, (b) the GW sources interfere, and (c) the data are contaminated by noise. Here, for a Gaussian ensemble of sources, we predict that variance by constructing an optimal estimator of the HD correlation, taking into account the pulsar sky locations and the frequency distribution of the GWs and the pulsar noise. The variance is a ratio: the numerator depends upon the pulsar sky locations, and the denominator is the (effective) number of frequency bins for which the GW signal dominates the noise. In effect, after suitable combination, each such frequency bin gives an independent estimate of the HD correlation.}, archive = {J_PRL}, author = {Bruce Allen and Joseph D. Romano}, doi = {10.1103/PhysRevLett.134.031401}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031401}, shortjournal = {Phys. Rev. Lett.}, title = {Optimal reconstruction of the hellings and downs correlation}, volume = {134}, year = {2025}, }
• (2025). Ultralight dark matter search with space-time separated atomic clocks and cavities. PRL, 134(3), 031001. (www)

  @article{ , abstract = {We devise and demonstrate a method to search for nongravitational couplings of ultralight dark matter to standard model particles using space-time separated atomic clocks and cavity-stabilized lasers. By making use of space-time separated sensors, which probe different values of an oscillating dark matter field, we can search for couplings that cancel in typical local experiments. This provides sensitivity to both the temporal and spatial fluctuations of the field. We demonstrate this method using existing data from a frequency comparison of lasers stabilized to two optical cavities connected via a 2220 km fiber link [Schioppo et al. , Nat. Commun. 13 , 212 (2022) ], and from the atomic clocks on board the global positioning system satellites. Our analysis results in constraints on the coupling of scalar dark matter to electrons, for masses between and . These are the first constraints on alone in this mass range.}, archive = {J_PRL}, author = {Melina Filzinger and Ashlee R. Caddell and Dhruv Jani and Martin Steinel and Leonardo Giani and Nils Huntemann and Benjamin M. Roberts}, doi = {10.1103/PhysRevLett.134.031001}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {031001}, shortjournal = {Phys. Rev. Lett.}, title = {Ultralight dark matter search with space-time separated atomic clocks and cavities}, volume = {134}, year = {2025}, }
• (2025). Path percolation in quantum communication networks. PRL, 134(3), 030803. (www)

  @article{ , abstract = {In a quantum communication network, links represent entanglement between qubits located at different nodes. Even if two nodes are not directly linked by shared entanglement, they can still communicate via routing protocols. However, in contrast to classical communication, each quantum communication event removes all participating links along the routed path, disrupting the quantum communication network. Here, we propose a simple model, where randomly selected pairs of nodes communicate through the shortest paths. Each time such a path is used, all participating links are eliminated, leading to a correlated percolation process that we call “path percolation.” We study path percolation both numerically and analytically and present the phase diagram of the steady states as a function of the rate at which new links are being added to the network. As a key result, the steady state is found to be independent of the initial network topologies when new links are added randomly between disconnected components. We close by discussing extensions of path percolation and link replenishment, along with their potential applications.}, archive = {J_PRL}, author = {Xiangyi Meng and Bingjie Hao and Balázs Ráth and István A. Kovács}, doi = {10.1103/PhysRevLett.134.030803}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {030803}, shortjournal = {Phys. Rev. Lett.}, title = {Path percolation in quantum communication networks}, volume = {134}, year = {2025}, }
• (2025). Privacy in networks of quantum sensors. PRL, 134(3), 030802. (www)

  @article{ , abstract = {We treat privacy in a network of quantum sensors where accessible information is limited to specific functions of the network parameters, and all other information remains private. We develop an analysis of privacy in terms of a manipulation of the quantum Fisher information matrix, and find the optimal state achieving maximum privacy in the estimation of linear combination of the unknown parameters in a network of quantum sensors. We also discuss the effect of uncorrelated noise on the privacy of the network. Moreover, we illustrate our results with an example where the goal is to estimate the average value of the unknown parameters in the network. In this example, we also introduce the notion of quasiprivacy ( privacy), quantifying how close the state is to being private.}, archive = {J_PRL}, author = {Majid Hassani and Santiago Scheiner and Matteo G. A. Paris and Damian Markham}, doi = {10.1103/PhysRevLett.134.030802}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {030802}, shortjournal = {Phys. Rev. Lett.}, title = {Privacy in networks of quantum sensors}, volume = {134}, year = {2025}, }
• (2025). Optimizing quantum measurements by partitioning multisets of observables. PRL, 134(3), 030801. (www)

  @article{ , abstract = {Quantum tomography approaches typically consider a set of observables that we wish to measure, designing a measurement scheme that measures each of the observables and then repeats the measurements as many times as necessary. We show that instead of considering only the simple set of observables, one should consider a multiset of the observables taking into account the required repetitions, to minimize the number of measurements. This leads to a graph theoretic multicoloring problem. We show that the multiset method offers at most quadratic improvement but it is achievable. Furthermore, despite the NP-hard optimal coloring problem, the multiset approach with greedy coloring algorithms already offers asymptotically quadratic improvement in test cases.}, archive = {J_PRL}, author = {O. Veltheim and E. Keski-Vakkuri}, doi = {10.1103/PhysRevLett.134.030801}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {030801}, shortjournal = {Phys. Rev. Lett.}, title = {Optimizing quantum measurements by partitioning multisets of observables}, volume = {134}, year = {2025}, }
• (2025). Universal work statistics in long-range interacting quantum systems. PRL, 134(3), 030402. (www)

  @article{ , abstract = {We determine the conditions under which the presence of long-range interactions reduce the energy losses due to defect generation during nonadiabatic evolution, crucial for enhancing the power to efficiency ratio of quantum thermal devices. In order to do so, we investigate the response of long-range systems to diverse external drivings, emphasizing their robustness against dynamic excitation in comparison to generic local systems. This phenomenon is demonstrated through the study of the quantum work statistics, revealing insights into energy transfer efficiency and dynamical quantum criticality. Our results demonstrate the benefits of including a long-range interacting medium for quantum thermodynamics application, highlighting the potential to optimize finite-time quantum thermal cycles. Thanks to the effective dimension approach our findings can be drawn in full generality and, then, specified to different experimentally relevant scenarios.}, archive = {J_PRL}, author = {Andrea Solfanelli and Nicolò Defenu}, doi = {10.1103/PhysRevLett.134.030402}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {030402}, shortjournal = {Phys. Rev. Lett.}, title = {Universal work statistics in long-range interacting quantum systems}, volume = {134}, year = {2025}, }
• (2025). Krylov subspace methods for quantum dynamics with time-dependent generators. PRL, 134(3), 030401. (www)

  @article{ , abstract = {Krylov subspace methods in quantum dynamics identify the minimal subspace in which a process unfolds. To date, their use is restricted to time evolutions governed by time-independent generators. We introduce a generalization valid for driven quantum systems governed by a time-dependent Hamiltonian that maps the evolution to a diffusion problem in a one-dimensional lattice with nearest-neighbor hopping probabilities that are inhomogeneous and time dependent. This representation is used to establish a novel class of fundamental limits to the quantum speed of evolution and operator growth. We also discuss generalizations of the algorithm, adapted to discretized time evolutions and periodic Hamiltonians, with applications to many-body systems.}, archive = {J_PRL}, author = {Kazutaka Takahashi and Adolfo del Campo}, doi = {10.1103/PhysRevLett.134.030401}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {030401}, shortjournal = {Phys. Rev. Lett.}, title = {Krylov subspace methods for quantum dynamics with time-dependent generators}, volume = {134}, year = {2025}, }
• (2025). Revealing hidden physical nonclassicality with non-negative polynomials. PRL, 134(3), 030201. (www)

  @article{ , abstract = {Understanding quantum phenomena that go beyond classical concepts is a focus of modern quantum physics. Here, we show how the theory of non-negative polynomials emerging around Hilbert’s 17th problem, can be used to optimally exploit data capturing the nonclassical nature of light. Specifically, we show that non-negative polynomials can reveal nonclassicality in data even when it is hidden from standard detection methods up to now. Moreover, the abstract language of non-negative polynomials also leads to a unified mathematical approach to nonclassicality for light and spin systems, allowing us to map methods for one to the other. Conversely, the physical problems arising also inspire several mathematical insights into characterization of non-negative polynomials.}, archive = {J_PRL}, author = {Ties-A. Ohst and Benjamin Yadin and Birte Ostermann and Timo de Wolff and Otfried Gühne and Hai-Chau Nguyen}, doi = {10.1103/PhysRevLett.134.030201}, journal = {Physical Review Letters}, month = {1}, number = {3}, pages = {030201}, shortjournal = {Phys. Rev. Lett.}, title = {Revealing hidden physical nonclassicality with non-negative polynomials}, volume = {134}, year = {2025}, }
• (2025). Critical avalanches in excitation-inhibition balanced networks reconcile response reliability with sensitivity for optimal neural representation. PRL, 134(2), 028401. (www)

  @article{ , abstract = {Neural criticality has emerged as a unified framework that reconciles diverse multiscale neuronal dynamics such as the irregular firing of individual neurons, sparse synchrony in neuronal populations, and the emergence of scale-free avalanches. However, the functional role of neuronal criticality remains ambiguous. Here, we investigate the neural dynamics and representations in response to external signals in excitation-inhibition balanced networks. We reveal that, in contrast with the case for the traditional critical branching model, the critical state of the balanced network simultaneously achieves maximal response sensitivity, maximal response reliability, and the optimal representation of external signals due to the presence of reliable avalanches induced by external signals. We further demonstrate that heterogeneity in inhibitory connections is a mechanism underlying the reliable critical avalanches and optimal representation. Our study addresses a longstanding challenge concerning the functional significance of neuronal criticality, namely the intricate coexistence of reliability and sensitivity.}, archive = {J_PRL}, author = {Zhuda Yang and Junhao Liang and Changsong Zhou}, doi = {10.1103/PhysRevLett.134.028401}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {028401}, shortjournal = {Phys. Rev. Lett.}, title = {Critical avalanches in excitation-inhibition balanced networks reconcile response reliability with sensitivity for optimal neural representation}, volume = {134}, year = {2025}, }
• (2025). Unified flow rule of undeveloped and fully developed dense granular flows down rough inclines. PRL, 134(2), 028201. (www)

  @article{ , abstract = {We report on chute measurements of the free-surface velocity in dense flows of spheres and diverse sands and spheres-sand mixtures down rough inclines. These and previous measurements are inconsistent with standard flow rules, in which the Froude number scales linearly with or , where is the dynamic friction coefficient, the flow thickness, and its smallest value that permits a steady, uniform dense flow state at a given inclination angle . This is because the characteristic length a flow needs to fully develop can exceed the chute or travel length and because neither rule is universal for fully developed flows across granular materials. We use a dimensional analysis motivated by a recent unification of sediment transport to derive a flow rule that solves both problems in accordance with our and previous measurements: , with and .}, archive = {J_PRL}, author = {Yanbin Wu and Thomas Pähtz and Zixiao Guo and Lu Jing and Zhao Duan and Zhiguo He}, doi = {10.1103/PhysRevLett.134.028201}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {028201}, shortjournal = {Phys. Rev. Lett.}, title = {Unified flow rule of undeveloped and fully developed dense granular flows down rough inclines}, volume = {134}, year = {2025}, }
• (2025). Smooth exact gradient descent learning in spiking neural networks. PRL, 134(2), 027301. (www)

  @article{ , abstract = {Gradient descent prevails in artificial neural network training, but seems inept for spiking neural networks as small parameter changes can cause sudden, disruptive appearances and disappearances of spikes. Here, we demonstrate exact gradient descent based on continuously changing spiking dynamics. These are generated by neuron models whose spikes vanish and appear at the end of a trial, where it cannot influence subsequent dynamics. This also enables gradient-based spike addition and removal. We illustrate our scheme with various tasks and setups, including recurrent and deep, initially silent networks.}, archive = {J_PRL}, author = {Christian Klos and Raoul-Martin Memmesheimer}, doi = {10.1103/PhysRevLett.134.027301}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {027301}, shortjournal = {Phys. Rev. Lett.}, title = {Smooth exact gradient descent learning in spiking neural networks}, volume = {134}, year = {2025}, }
• (2025). Asymmetric simple exclusion process on the percolation cluster: Waiting time distribution in side branches. PRL, 134(2), 027102. (www)

  @article{ , abstract = {As the simplest model of transport of interacting particles in a disordered medium, we consider the asymmetric simple exclusion process (ASEP) in which particles with hard-core interactions perform biased random walks, on the supercritical percolation cluster. In this process, the long time trajectory of a marked particle consists of steps on the backbone, punctuated by time spent in side branches. We study the probability distribution in the steady state of the waiting time of a randomly chosen particle, in a side branch since its last step along the backbone. Exact numerical evaluation of this on a single side branch of length to 9 shows that for large fields, the probability distribution of has multiple well separated peaks. We extend this result to a regular comb, and to the ASEP on the percolation cluster. We show that in the steady state, the fractional number of particles that have been in the same side branch for a time interval greater than varies as for large , where depends only on the bias field. However, these long timescales are not reflected in the eigenvalue spectrum of the Markov evolution matrix. The system shows dynamical heterogeneity, with particles segregating into pockets of high and low mobilities.}, archive = {J_PRL}, author = {Chandrashekar Iyer and Mustansir Barma and Hunnervir Singh and Deepak Dhar}, doi = {10.1103/PhysRevLett.134.027102}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {027102}, shortjournal = {Phys. Rev. Lett.}, title = {Asymmetric simple exclusion process on the percolation cluster: Waiting time distribution in side branches}, volume = {134}, year = {2025}, }
• (2025). Minimal model for carnot efficiency at maximum power. PRL, 134(2), 027101. (www)

  @article{ , abstract = {Carnot efficiency sets a fundamental upper bound on the heat engine efficiency, attainable in the quasistatic limit, albeit at the cost of completely sacrificing power output. Here, we present a minimal heat engine model that can attain Carnot efficiency while achieving maximum power output. We unveil the potential of intrinsic divergent physical quantities within the working substance, such as degeneracy, as promising thermodynamic resources to break through the universal power-efficiency trade-off imposed by nonequilibrium thermodynamics for conventional heat engines. Our findings provide novel insights into the collective advantage in harnessing energy of many-body interacting systems.}, archive = {J_PRL}, author = {Shiling Liang (梁师翎) and Yu-Han Ma and Daniel Maria Busiello and Paolo De Los Rios}, doi = {10.1103/PhysRevLett.134.027101}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {027101}, shortjournal = {Phys. Rev. Lett.}, title = {Minimal model for carnot efficiency at maximum power}, volume = {134}, year = {2025}, }
• (2025). Observation of nonreciprocal diffraction of surface acoustic wave. PRL, 134(2), 027001. (www)

  @article{ , abstract = {The rectification phenomenon caused by the simultaneous breaking of time-reversal and spatial inversion symmetries has been extended to a wide range of (quasi)particles and waves; however, nonreciprocal diffraction, which is the imbalance of upward and downward deflections, was previously observed only for photons and remained to be extended to other (quasi)particles. In this Letter, we present evidence of the nonreciprocal diffraction of a surface acoustic wave (SAW) utilizing a magnetoelastic grating on a SAW device. Asymmetric diffraction intensities were observed when the ferromagnetic resonance was acoustically excited. Based on a theoretical model, we attribute the microscopic origin of this phenomenon to the resonant scattering involving ferromagnetic resonance excitations. The novel property may pave an avenue to further development of SAW devices for various purposes, including microwave communications and quantum engineering applications.}, archive = {J_PRL}, author = {Y. Nii and K. Yamamoto and M. Kanno and S. Maekawa and Y. Onose}, doi = {10.1103/PhysRevLett.134.027001}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {027001}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of nonreciprocal diffraction of surface acoustic wave}, volume = {134}, year = {2025}, }
• (2025). Twist-angle-dependent valley polarization of intralayer moiré excitons in van der waals superlattices. PRL, 134(2), 026904. (www)

  @article{ , abstract = {Twistronics, which utilizes the moiré potential to induce exotic excitations in twisted material systems, has garnered significant attention in recent years. In this Letter, using the Bethe-Salpeter calculations based on a continuum model of electronic structures, we explore the optical characteristics of intralayer moiré excitons in twisted bilayer transition metal dichalcogenide heterostructures. We find the Coulomb exchange interactions strongly influence these excitons and the degree of valley polarization and that the splitting between spin-singlet and spin-triplet moiré excitons can be effectively controlled by varying the twist angle. Specifically, intralayer bright spin-singlet moiré excitons confined in a twisted heterostructure can achieve valley polarization levels as high as 90% at small twist angles, which holds promise for future applications in valleytronics. These findings underscore the twist angle as a novel parameter for manipulating the optical properties of moiré excitons, thereby establishing moiré semiconductors as a promising platform for investigating many-body physics in solid-state systems.}, archive = {J_PRL}, author = {Renqi Wang and Kai Chang and Wenhui Duan and Yong Xu and Peizhe Tang}, doi = {10.1103/PhysRevLett.134.026904}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026904}, shortjournal = {Phys. Rev. Lett.}, title = {Twist-angle-dependent valley polarization of intralayer moiré excitons in van der waals superlattices}, volume = {134}, year = {2025}, }
• (2025). Multiple carrier generation at an exceptionally low energy threshold. PRL, 134(2), 026903. (www)

  @article{ , abstract = {Multiple carrier generation (MCG), a process wherein two or more carriers are generated from a single high-energy absorbed photon, holds immense promise for quantum sensing, metrology, low-threshold lasers, and photovoltaics. Despite its potential, MCG has faced obstacles such as low efficiency and a high threshold photon energy at least twice the band gap ( ) of the semiconductor, limiting its application only to a class of materials with low . Here, we present a new approach that overcomes this limitation by leveraging carrier-donor scattering to excite secondary electrons from donor states strategically positioned below the conduction band. Our method relies on strong Coulomb interaction, reduced dielectric screening, slow hot carrier cooling, and strictly follows the energy conservation rules. We experimentally demonstrated this idea in a model system of monolayer (1L) by exploiting electron-donating chalcogen vacancy states. We observed an exceptionally low MCG threshold of for the first time in 1L . Remarkably, the quantum yield can be further increased to by increasing the photon energy to , representing a substantial advancement over existing methods. Our findings extend the horizon of MCG into next-generation high-performance optoelectronic devices with an on-demand operating spectral range spanning from infrared to ultraviolet.}, archive = {J_PRL}, author = {Riyanka Karmakar and Pravrati Taank and Debjit Ghoshal and Pushpendra Yadav and Dipendranath Mandal and Megha Shrivastava and Amit Agarwal and Matthew C. Beard and Elisa M. Miller and K. V. Adarsh}, doi = {10.1103/PhysRevLett.134.026903}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026903}, shortjournal = {Phys. Rev. Lett.}, title = {Multiple carrier generation at an exceptionally low energy threshold}, volume = {134}, year = {2025}, }
• (2025). Strategy for direct detection of chiral phonons with phase-structured free electrons. PRL, 134(2), 026902. (www)

  @article{ , abstract = {Chiral phonons possessing valley pseudoangular momentum (PAM) underlie a diversity of quantum phenomena of fundamental and applied importance, but are challenging to probe directly. We show that deficiencies of typical momentum-resolved electron energy loss measurements that make it impossible to distinguish the PAM of chiral phonons can be overcome by introducing pinwheel free electron states with well-defined PAM. Transitions between such states generate 2D periodic arrays of in-plane field vortices with polarization textures tailored to selectively couple to desired chiral mode symmetries.}, archive = {J_PRL}, author = {Marc R. Bourgeois and Andrew W. Rossi and David J. Masiello}, doi = {10.1103/PhysRevLett.134.026902}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026902}, shortjournal = {Phys. Rev. Lett.}, title = {Strategy for direct detection of chiral phonons with phase-structured free electrons}, volume = {134}, year = {2025}, }
• (2025). Ultrafast optical control of rashba interactions in a TMDC heterostructure. PRL, 134(2), 026901. (www)

  @article{ , abstract = {We investigate spin relaxation dynamics of interlayer excitons in a heterostructure induced by the Rashba effect. In such a system, Rashba interactions arise from an out-of-plane electric field due to photogenerated interlayer excitons inducing a phonon-assisted intravalley spin relaxation. We develop a theoretical description based on a microscopic approach to quantify the magnitude of Rashba interactions and test these predictions via time-resolved Kerr rotation measurements. In agreement with the calculations, we find that the Rashba-induced intravalley spin mixing becomes the dominating spin relaxation channel above . Our work identifies a previously unexplored spin-depolarization channel in heterostructures which can be used for ultrafast spin manipulation.}, archive = {J_PRL}, author = {Henry Mittenzwey and Abhijeet M. Kumar and Raghav Dhingra and Kenji Watanabe and Takashi Taniguchi and Cornelius Gahl and Kirill I. Bolotin and Malte Selig and Andreas Knorr}, doi = {10.1103/PhysRevLett.134.026901}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026901}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrafast optical control of rashba interactions in a TMDC heterostructure}, volume = {134}, year = {2025}, }
• (2025). Anomalous spin and orbital hall phenomena in antiferromagnetic systems. PRL, 134(2), 026702. (www)

  @article{ , abstract = {We investigate anomalous spin and orbital Hall phenomena in antiferromagnetic materials via orbital pumping experiments. Conducting spin and orbital pumping experiments on heterostructures, we unexpectedly observe strong spin and orbital anomalous signals in an out-of-plane configuration. We report a sevenfold increase in the signal of the anomalous inverse orbital Hall effect compared to conventional effects. Our study suggests expanding the orbital Hall angle ( ) to a rank 3 tensor, akin to the spin Hall angle ( ), to explain the anomalous inverse orbital Hall effect. This work pioneers converting spin-orbital currents into charge currents, advancing the spin-orbitronics domain in antiferromagnetic materials.}, archive = {J_PRL}, author = {J. E. Abrão and E. Santos and J. L. Costa and J. G. S. Santos and J. B. S. Mendes and A. Azevedo}, doi = {10.1103/PhysRevLett.134.026702}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026702}, shortjournal = {Phys. Rev. Lett.}, title = {Anomalous spin and orbital hall phenomena in antiferromagnetic systems}, volume = {134}, year = {2025}, }
• (2025). Magnon spin transport through atomic ferrimagnetic domain walls. PRL, 134(2), 026701. (www)

  @article{ , abstract = {It is a well-established notion that the spin of a magnon should be flipped when it passes through a 180° domain wall (DW) in both ferromagnets and antiferromagnets, while the magnon spin transport through ferrimagnetic DW is still elusive. In this Letter, we report that the magnon preserves its spin after the transmission through an atomically sharp DW in ferrimagnets due to the intriguing interband magnon scattering at the domain interface. This finding may provide significant insight to resolve the puzzling insensitivity of magnon spin diffusion to the 180° ferrimagnetic DWs observed by recent experiments. Our results reveal the unique role of ferrimagnetic DWs in manipulating the magnon spin and may facilitate the design of novel magnonic devices based on ferrimagnets.}, archive = {J_PRL}, author = {Zhaozhuo Zeng and Peng Yan}, doi = {10.1103/PhysRevLett.134.026701}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026701}, shortjournal = {Phys. Rev. Lett.}, title = {Magnon spin transport through atomic ferrimagnetic domain walls}, volume = {134}, year = {2025}, }
• (2025). Fermionic isometric tensor network states in two dimensions. PRL, 134(2), 026502. (www)

  @article{ , abstract = {We generalize isometric tensor network states to fermionic systems, paving the way for efficient adaptations of 1D tensor network algorithms to 2D fermionic systems. As the first application of this formalism, we developed and benchmarked a time-evolving block-decimation (TEBD) algorithm for real-time and imaginary-time evolution. The imaginary-time evolution produces ground-state energies for gapped systems, systems with a Dirac point, and systems with gapless edge modes to good accuracy. The real-time TEBD captures the scattering of two fermions and the chiral edge dynamics on the boundary of a Chern insulator.}, archive = {J_PRL}, author = {Zhehao Dai and Yantao Wu and Taige Wang and Michael P. Zaletel}, doi = {10.1103/PhysRevLett.134.026502}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026502}, shortjournal = {Phys. Rev. Lett.}, title = {Fermionic isometric tensor network states in two dimensions}, volume = {134}, year = {2025}, }
• (2025). Flat and tunable moir\'e phonons in twisted transition-metal dichalcogenides. PRL, 134(2), 026501. (www)

  @article{ , abstract = {Displacement fields are one of the main tuning knobs employed to engineer flat electronic band dispersions in twisted van der Waals multilayers. Here, we show that electric fields can also be used to tune the phonon dispersion of moiré superlattices formed by noncentrosymmetric materials, focusing on twisted transition metal dichalcogenide homobilayers. This effect arises from the intertwining between the local stacking configuration and the formation of polar domains within the moiré supercell. For small twist angles, increasing the electric field leads to a universal moiré phonon spectrum characterized by a substantially softened longitudinal acoustic phason mode and a flat optical phonon mode, both of which cause a significant enhancement in the vibrational density of states. The phasons also acquire a prominent chiral character, displaying a nonzero angular momentum spread across the Brillouin zone. We discuss how the tunability of the moiré phonon spectra may affect electronic properties, focusing on the recently discovered phenomenon of van der Waals ferroelectricity.}, archive = {J_PRL}, author = {Alejandro Ramos-Alonso and Benjamin Remez and Daniel Bennett and Rafael M. Fernandes and Héctor Ochoa}, doi = {10.1103/PhysRevLett.134.026501}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026501}, shortjournal = {Phys. Rev. Lett.}, title = {Flat and tunable moir\'e phonons in twisted transition-metal dichalcogenides}, volume = {134}, year = {2025}, }
• (2025). Symmetry breaking in the superionic phase of silver iodide. PRL, 134(2), 026306. (www)

  @article{ , abstract = {In the superionic phase of silver iodide, we observe a distorted tetragonal structure characterized by symmetry breaking in the cation distribution. This phase competes with the well known bcc phase with a symmetric cation distribution, at an energetic cost of only a few . The small energy difference suggests that these competing structures may both be thermally accessible near the superionic transition temperature. We also find that the distribution of silver ions depends on the low-temperature parent polymorph, with memory persisting in the superionic phase on the nanosecond timescales accessible in our simulations. Furthermore, simulations on the order of 100 ns reveal that even at temperatures where the bcc phase is stable, significant fluctuations toward the tetragonal lattice structure remain. Our results are consistent with many “anomalous” experimental observations and offer a molecular mechanism for the “memory effect” in silver iodide.}, archive = {J_PRL}, author = {Amir Hajibabaei and William J. Baldwin and Gábor Csányi and Stephen J. Cox}, doi = {10.1103/PhysRevLett.134.026306}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026306}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry breaking in the superionic phase of silver iodide}, volume = {134}, year = {2025}, }
• (2025). Giant third-order nonlinearity induced by the quantum metric quadrupole in few-layer ${\mathrm{WTe}}_{2}$. PRL, 134(2), 026305. (www)

  @article{ , abstract = {The quantum geometric properties of topological materials underpin many exotic physical phenomena and applications. Quantum nonlinearity has emerged as a powerful probe for revealing these properties. The Berry curvature dipole in nonmagnetic materials and the quantum metric dipole in antiferromagnets have been explored by studying the second-order nonlinear Hall effect. Although the quadrupole moment of the quantum geometric tensor is theoretically predicted to induce higher-order quantum nonlinearity, the quantum metric quadrupole remains experimentally unexplored. Here, we report the quantum metric quadrupole induced third-order nonlinear longitudinal electrical response in few-layer WTe 2 , persisting up to room temperature. Angle-resolved third-harmonic current-voltage characteristics are found consistent with the intrinsic crystal symmetry of WTe 2 . Through temperature variation and scaling analysis, we identify the quantum metric quadrupole as the physical origin of the observed third-order longitudinal nonlinearity. Additionally, we determine the angle dependence of the quantum metric quadrupole, establishing third-order nonlinearity as an efficient method for revealing the quantum metric structure.}, archive = {J_PRL}, author = {Xing-Yu Liu and An-Qi Wang and Dong Li and Tong-Yang Zhao and Xin Liao and Zhi-Min Liao}, doi = {10.1103/PhysRevLett.134.026305}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026305}, shortjournal = {Phys. Rev. Lett.}, title = {Giant third-order nonlinearity induced by the quantum metric quadrupole in few-layer ${\mathrm{WTe}}_{2}$}, volume = {134}, year = {2025}, }
• (2025). Quantum nonlinear acoustic hall effect and inverse acoustic faraday effect in dirac insulators. PRL, 134(2), 026304. (www)

  @article{ , abstract = {We propose to realize the quantum nonlinear Hall effect and the inverse Faraday effect through the acoustic wave in a time-reversal invariant but inversion broken Dirac insulator. We focus on the acoustic frequency much lower than the Dirac gap such that the interband transition is suppressed and these effects arise solely from the intrinsic valley-contrasting band topology. The corresponding acoustoelectric conductivity and magnetoacoustic susceptibility are both proportional to the quantized valley Chern number and independent of the quasiparticle lifetime. The linear and nonlinear components of the longitudinal and transverse topological currents can be tuned by adjusting the polarization and propagation directions of the surface acoustic wave. The static magnetization generated by a circularly polarized acoustic wave scales linearly with the acoustic frequency as well as the strain-induced charge density. Our results unveil a quantized nonlinear topological acoustoelectric response of gapped Dirac materials, like hexagonal boron nitride and transition-metal dichalcogenide, paving the way toward room-temperature acoustoelectric devices due to their large band gaps.}, archive = {J_PRL}, author = {Ying Su and Alexander V. Balatsky and Shi-Zeng Lin}, doi = {10.1103/PhysRevLett.134.026304}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026304}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum nonlinear acoustic hall effect and inverse acoustic faraday effect in dirac insulators}, volume = {134}, year = {2025}, }
• (2025). Orbital diffusion, polarization, and swapping in centrosymmetric metals. PRL, 134(2), 026303. (www)

  @article{ , abstract = {We propose a general theory of charge, spin, and orbital diffusion based on Keldysh formalism. Our findings indicate that the diffusivity of orbital angular momentum in metals is much lower than that of spin or charge due to the strong orbital intermixing in crystals. Furthermore, our theory introduces the concept of “spin-orbit polarization” by which a pure orbital (spin) current induces a longitudinal spin (orbital) current, a process as efficient as spin polarization in ferromagnets. Finally, we find that orbital currents undergo momentum swapping, even in the absence of spin-orbit coupling. This theory establishes several key parameters for orbital transport of direct importance to experiments.}, archive = {J_PRL}, author = {Xiaobai Ning and A. Pezo and Kyoung-Whan Kim and Weisheng Zhao and Kyung-Jin Lee and Aurélien Manchon}, doi = {10.1103/PhysRevLett.134.026303}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026303}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital diffusion, polarization, and swapping in centrosymmetric metals}, volume = {134}, year = {2025}, }
• (2025). Temperature dependence of electron viscosity in superballistic GaAs point contacts. PRL, 134(2), 026302. (www)

  @article{ , abstract = {Hydrodynamic description of collective electron motion turns out to be fruitful, since it provides a reliable physical concept that allows engineering the electron-electron interaction. We experimentally study the relation between two fundamental quantities—the electron viscosity and the Fermi quasiparticle lifetime—beyond the applicability limit of the Fermi liquid theory. We use point contact (PC) geometry to study electron transport and observe superballistic PC conductance, which is a signature of the electron viscosity. At high enough temperatures, the viscosity-lifetime relation is shown to diverge from the theoretically predicted one and turns out to be nontrivial. In addition, we study these phenomena in PCs freely suspended over a substrate, i.e., under the unique experimental conditions of enhanced electron-electron interaction. Suspension is found to reduce the electron viscosity in the whole temperature range, which makes the suspended structures a promising test bed for studying hydrodynamic effects in solids.}, archive = {J_PRL}, author = {Daniil I. Sarypov and Dmitriy A. Pokhabov and Arthur G. Pogosov and Evgeny Yu. Zhdanov and Andrey A. Shevyrin and Askhat K. Bakarov and Alexander A. Shklyaev}, doi = {10.1103/PhysRevLett.134.026302}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026302}, shortjournal = {Phys. Rev. Lett.}, title = {Temperature dependence of electron viscosity in superballistic GaAs point contacts}, volume = {134}, year = {2025}, }
• (2025). Planar hall effect in quasi-two-dimensional materials. PRL, 134(2), 026301. (www)

  @article{ , abstract = {The planar Hall effect in 3D systems is an effective probe for their Berry curvature, topology, and electronic properties. However, the Berry curvature-induced conventional planar Hall effect is forbidden in 2D systems as the out-of-plane Berry curvature cannot couple to the band velocity of the electrons moving in the 2D plane. Here, we demonstrate a unique 2D planar Hall effect (2DPHE) originating from the hidden planar components of the Berry curvature and orbital magnetic moment in quasi-2D materials. We identify all planar band geometric contributions to 2DPHE and classify their crystalline symmetry restrictions. Using gated bilayer graphene as an example, we show that in addition to capturing the hidden band geometric effects, 2DPHE is also sensitive to the Lifshitz transitions. Our Letter motivates further exploration of hidden planar band geometry-induced 2DPHE and related transport phenomena for innovative applications.}, archive = {J_PRL}, author = {Koushik Ghorai and Sunit Das and Harsh Varshney and Amit Agarwal}, doi = {10.1103/PhysRevLett.134.026301}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026301}, shortjournal = {Phys. Rev. Lett.}, title = {Planar hall effect in quasi-two-dimensional materials}, volume = {134}, year = {2025}, }
• (2025). Superconducting meron phase in locally noncentrosymmetric superconductors. PRL, 134(2), 026002. (www)

  @article{ , abstract = {The theory of superconducting parity transition is extended by incorporating the vortex degree of freedom. We employ the bilayer Rashba model representing locally noncentrosymmetric layered superconductors and derive the Ginzburg-Landau free energy functional. This formulation reveals parity transition, where the even-parity superconducting state changes to the odd-parity one upon increasing the magnetic field under the vortex states. The phase diagram of is quantitatively reproduced and a novel superconducting state with a meron (half-skyrmion) lattice pseudospin texture is predicted.}, archive = {J_PRL}, author = {Akihiro Minamide and Youichi Yanase}, doi = {10.1103/PhysRevLett.134.026002}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026002}, shortjournal = {Phys. Rev. Lett.}, title = {Superconducting meron phase in locally noncentrosymmetric superconductors}, volume = {134}, year = {2025}, }
• (2025). Nonlinear superconducting magnetoelectric effect. PRL, 134(2), 026001. (www)

  @article{ , abstract = {Supercurrent flow can induce a nonvanishing spin magnetization in noncentrosymmetric superconductors with spin-orbit interaction. Often known as the nondissipative magnetoelectric effect, these are most commonly found at linear order in supercurrent flow. Here, we propose that a nonlinear superconducting magnetoelectric (NSM) effect can naturally manifest in magnet-superconductor heterostructures. In such platforms, NSM manifests as the spin polarization generated as a second-order response to a driving supercurrent. Strikingly, we find NSM survives centrosymmetry and is the leading-order magnetic response in a variety of magnetic materials that include both collinear magnets (e.g., -wave planar altermagnet thin film-superconductor) as well as noncollinear magnets (e.g., kagome-superconductor systems). This renders NSM a powerful electric and nondissipative means of controlling magnetization in magnet-superconductor heterostructures, a promising platform for superconducting spintronics.}, archive = {J_PRL}, author = {Jin-Xin Hu and Oles Matsyshyn and Justin C. W. Song}, doi = {10.1103/PhysRevLett.134.026001}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {026001}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear superconducting magnetoelectric effect}, volume = {134}, year = {2025}, }
• (2025). Excitation of alfvénic modes via electromagnetic turbulence in wendelstein 7-X. PRL, 134(2), 025103. (www)

  @article{ , abstract = {In this Letter, we demonstrate by comparison of computer simulations and experimental results that excitation of turbulence-driven electromagnetic secondary instabilities can serve as a paradigm to explain the observed activity of otherwise stable modes in fusion devices. In particular, we discuss the excitation of Alfvén eigenmodes in electron cyclotron heated plasmas in the Wendelstein 7-X (W7-X) stellarator. In more than 700 experimental programs of W7-X Operational Phase 1.2b (from which 25 were selected and discussed in this paper), poloidal magnetic fluctuation measurements with a clear Alfvénic nature are seen to correlate with turbulence density fluctuations. In response, we perform nonlinear, global, gyrokinetic, electromagnetic simulations using profiles consistent with the experimental conditions. The results agree remarkably well with the measurements and reveal excitation of zonal flow activity and long wavelength Alfvénic modes by ion temperature gradient turbulence. Integer ratios between the primary and secondary growth rates suggest an excitation mechanism similar to the forced-driven excitation of zonal flow by Alfvén eigenmodes.}, archive = {J_PRL}, author = {Jörg Riemann and Sara Vaz Mendes and Kian Rahbarnia and Ralf Kleiber and Christoph Slaby and Axel Könies and Matthias Borchardt and Alexey Mishchenko and Henning Thomsen and Charlotte Büschel and Adrian von Stechow and the Wendelstein 7-X Team and Jan-Peter Bähner and Søren Kjer Hansen and Eric Edlund}, doi = {10.1103/PhysRevLett.134.025103}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {025103}, shortjournal = {Phys. Rev. Lett.}, title = {Excitation of alfvénic modes via electromagnetic turbulence in wendelstein 7-X}, volume = {134}, year = {2025}, }
• (2025). Optical imaging of laser-driven fast electron weibel-like filamentation in overcritical density plasma. PRL, 134(2), 025102. (www)

  @article{ , abstract = {We report on the measurement of filamented transport of laser-generated fast electron beams in near-critical density plasma. A relativistic intensity long-wave-infrared laser irradiated a hydrodynamically shaped helium gas flow at an electron density , generating a large flux of fast electrons that propagated beyond the critical surface. The beam-to-background electron density ratio was sufficiently high to drive growth of Weibel-like filamentation, which was measured by optical probing to extend up to with radii . Particle-in-cell simulations reproduce the main features of the filamentation generation, suggesting that collisionless processes are dominant in these interactions. Expansion of the filaments after formation infers a fast electron heated plasma temperature in the overcritical density plasma.}, archive = {J_PRL}, author = {N. P. Dover and O. Tresca and N. Cook and O. C. Ettlinger and R. J. Kingham and C. Maharjan and M. N. Polyanskiy and P. Shkolnikov and I. Pogorelsky and Z. Najmudin}, doi = {10.1103/PhysRevLett.134.025102}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {025102}, shortjournal = {Phys. Rev. Lett.}, title = {Optical imaging of laser-driven fast electron weibel-like filamentation in overcritical density plasma}, volume = {134}, year = {2025}, }
• (2025). All-optical blast-wave control of laser wakefield acceleration in a near-critical plasma. PRL, 134(2), 025101. (www)

  @article{ , abstract = {We propose a novel method for changing the length of laser wakefield electron acceleration in a gas jet using a cylindrical blast-wave created by a perpendicularly focused nanosecond laser pulse. The shock front modifies the wake significantly and stops interaction between the laser pulse and accelerated electron bunch, allowing one to directly control the interaction length and avoid dephasing. It also improves the electron beam quality through the plasma lensing effect between the two shock fronts. We demonstrated both experimentally and numerically how this approach can be used to form a quasimonoenergetic electron bunch with controlled energy and improved divergence as well as tracking changes in the bunch parameters during acceleration.}, archive = {J_PRL}, author = {I. Tsymbalov and D. Gorlova and K. Ivanov and E. Starodubtseva and R. Volkov and I. Tsygvintsev and Yu. Kochetkov and Ph. Korneev and A. Polonski and A. Savel’ev}, doi = {10.1103/PhysRevLett.134.025101}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {025101}, shortjournal = {Phys. Rev. Lett.}, title = {All-optical blast-wave control of laser wakefield acceleration in a near-critical plasma}, volume = {134}, year = {2025}, }
• (2025). Enabling all-to-circular polarization up-conversion by nonlinear chiral metasurfaces with rotational symmetry. PRL, 134(2), 023804. (www)

  @article{ , abstract = {We introduce a stacking strategy to design nonlinear chiral metasurfaces with high rotational symmetry, enabling degenerate quasi-bound-in-the-continuum resonances of absolute chirality. This symmetry allows for converting a circularly polarized pump into a circularly polarized nonlinear signal. Consequently, our rotation-symmetric bilayered metasurface design, tailored to respond solely to one specific circular polarization, can up-convert a linear or arbitrary polarized pump into circularly polarized nonlinear signals. The intensity ratios of these signals scale as the fourth (second) power of the chiral resonance amplitude for the second (third) harmonic.}, archive = {J_PRL}, author = {Dmitrii Gromyko and Jun Siang Loh and Jiangang Feng and Cheng-Wei Qiu and Lin Wu}, doi = {10.1103/PhysRevLett.134.023804}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023804}, shortjournal = {Phys. Rev. Lett.}, title = {Enabling all-to-circular polarization up-conversion by nonlinear chiral metasurfaces with rotational symmetry}, volume = {134}, year = {2025}, }
• (2025). Metasurface polarization optics: Phase manipulation for arbitrary polarization conversion condition. PRL, 134(2), 023803. (www)

  @article{ , abstract = {Metasurface polarization optics have attracted considerable attention due to their ability to manipulate independently the wave fronts of different polarization channels with subwavelength scale. Previous methods mainly focused on the condition of complete polarization conversion, restricting the application range of metasurface polarization multiplexing. Here, we proposed a generalized framework of phase manipulation for the metasurface polarization optics, which can realize independent phase control and arbitrary energy distribution of different polarization channels for the arbitrary polarization conversion efficiency. Based on this principle, we experimentally demonstrate tripolarization-channel wave-front control for the arbitrary polarization state (elliptical, circular, and linear). The arbitrary energy distribution of different polarization channels has been achieved via varying the polarization conversion efficiency. The proposed framework significantly improves the performance of metasurface in the polarization multiplexing and energy distribution, and expands the application scope of metasurface in the polarization optics.}, archive = {J_PRL}, author = {Siqi Li and Chen Chen and Guoxi Wang and Suyang Ge and Jiaqi Zhao and Xianshun Ming and Wei Zhao and Tao Li and Wenfu Zhang}, doi = {10.1103/PhysRevLett.134.023803}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023803}, shortjournal = {Phys. Rev. Lett.}, title = {Metasurface polarization optics: Phase manipulation for arbitrary polarization conversion condition}, volume = {134}, year = {2025}, }
• (2025). Hybridized soliton lasing in coupled semiconductor lasers. PRL, 134(2), 023802. (www)

  @article{ , abstract = {Coupling is an essential mechanism that drives complexity in natural systems, transforming single, noninteracting elements into intricate networks with rich physical properties. Here, we demonstrate a chip-scale coupled laser system that exhibits complex optical states impossible to achieve in an uncoupled system. We show that a pair of coupled semiconductor ring lasers spontaneously forms a frequency comb consisting of the hybridized modes of its coupled cavity, exhibiting a large number of phase-locked tones that anticross with one another. Experimental coherent waveform reconstruction reveals that the hybridized frequency comb manifests itself as pairs of bright and dark picosecond-long solitons circulating simultaneously. The dark and bright solitons exit the coupled cavity at the same time, leading to breathing bright solitons temporally overlapped with their dark soliton counterparts—a state inaccessible for a single, free-running laser. Our results demonstrate that the rules that govern allowable states of light can be broken by simply coupling elements together, paving the way for the design of more complex networks of coupled on-chip lasers.}, archive = {J_PRL}, author = {Theodore P. Letsou and Dmitry Kazakov and Pawan Ratra and Lorenzo L. Columbo and Massimo Brambilla and Franco Prati and Cristina Rimoldi and Sandro Dal Cin and Nikola Opačak and Henry O. Everitt and Marco Piccardo and Benedikt Schwarz and Federico Capasso}, doi = {10.1103/PhysRevLett.134.023802}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023802}, shortjournal = {Phys. Rev. Lett.}, title = {Hybridized soliton lasing in coupled semiconductor lasers}, volume = {134}, year = {2025}, }
• (2025). Diagnosis for band topology under crystal symmetries based on bulk measurements. PRL, 134(2), 023801. (www)

  @article{ , abstract = {Topological gapped crystalline materials are a class of topological materials characterized by invariants protected by spatial symmetries, allowing for the emergence of robust boundary states. The band topology of gapped materials with crystal symmetries can be theoretically labeled by symmetry-indicator invariants, such as the Fu-Kane parity criterion for inversion-symmetric topological gapped materials. Here, we propose an approach to measuring these invariants and diagnosing topological gapped crystalline materials, which is experimentally validated in two-dimensional photonic crystals with finite size. Notably, this diagnosis approach relies exclusively on the measured field distribution within the bulk region, without necessitating the energy band diagram possessing complete band gaps, even in the absence of in-gap states in real materials. Our study provides an approach for measuring symmetry-indicator invariants and paves the way for experimentally diagnosing various gapped topological phases originating from crystalline symmetries.}, archive = {J_PRL}, author = {Shiyin Jia and Shiqi Li and Junzheng Hu and Renwen Huang and Jing Li and Biye Xie and Peng Zhan and Zhenlin Wang}, doi = {10.1103/PhysRevLett.134.023801}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023801}, shortjournal = {Phys. Rev. Lett.}, title = {Diagnosis for band topology under crystal symmetries based on bulk measurements}, volume = {134}, year = {2025}, }
• (2025). Quantum state transfer via a multimode resonator. PRL, 134(2), 023602. (www)

  @article{ , abstract = {Large-scale fault-tolerant superconducting quantum computation needs rapid quantum communication to network qubits fabricated on different chips and long-range couplers to implement efficient quantum error correction codes. Quantum channels used for these purposes are best modeled by multimode resonators, which lie between single-mode cavities and waveguides with a continuum of modes. In this Letter, we propose a non-Markovian formalism for quantum state transfer using coupling strengths comparable to the channel’s free spectral range ( g ∼ Δ FSR ). Our scheme merges features of both the stimulated-Raman-adiabatic-passage-based methods for single-mode cavities and the pitch-and-catch protocol for long waveguides, integrating their advantages of low loss and high speed. It is immune to thermal channel occupations if using harmonic resonators for the sender and receiver.}, archive = {J_PRL}, author = {Yang He and Yu-Xiang Zhang}, doi = {10.1103/PhysRevLett.134.023602}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023602}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum state transfer via a multimode resonator}, volume = {134}, year = {2025}, }
• (2025). Coherence of an electronic two-level system under continuous charge sensing by a quantum dot detector. PRL, 134(2), 023601. (www)

  @article{ , abstract = {We investigate experimentally the quantum coherence of an electronic two-level system in a double quantum dot under continuous charge detection. The charge state of the two-level system is monitored by a capacitively coupled single quantum dot detector that imposes a backaction effect on the system. The measured backaction is well described by an additional decoherence rate, approximately linearly proportional to the detector electron tunneling rate. We provide a model for the decoherence rate arising due to level detuning fluctuations induced by detector charge fluctuations. The theory predicts a factor of 2 lower decoherence rates than observed in the experiment, suggesting the need for a more elaborate theory accounting for additional sources of decoherence.}, archive = {J_PRL}, author = {Subhomoy Haldar and Morten Munk and Harald Havir and Waqar Khan and Sebastian Lehmann and Claes Thelander and Kimberly A. Dick and Peter Samuelsson and Patrick P. Potts and Ville F. Maisi}, doi = {10.1103/PhysRevLett.134.023601}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023601}, shortjournal = {Phys. Rev. Lett.}, title = {Coherence of an electronic two-level system under continuous charge sensing by a quantum dot detector}, volume = {134}, year = {2025}, }
• (2025). Observation of relaxation stages in a nonequilibrium closed quantum system: Decaying turbulence in a trapped superfluid. PRL, 134(2), 023401. (www)

  @article{ , abstract = {The dynamics of nonequilibrium closed quantum systems and their route to thermalization are of fundamental interest to several fields, from cosmology to particle physics. However, a comprehensive description of nonequilibrium phenomena still presents a significant challenge. In this work, we report the observation of distinct stages during the relaxation of the decaying turbulence in trapped Bose-Einstein condensates. Our findings show a direct particle cascade from low to high momenta, a consequence of the energy injection in the system, exhibiting a characteristic universal scaling. This stage is followed by an inverse particle cascade responsible for repopulating the previously depleted condensate. Both cascades can be explained through self-similar solutions provided by wave turbulence theory. These findings provide important insights into the relaxation stages of out-of-equilibrium quantum many-body systems.}, archive = {J_PRL}, author = {M. A. Moreno-Armijos and A. R. Fritsch and A. D. García-Orozco and S. Sab and G. Telles and Y. Zhu and L. Madeira and S. Nazarenko and V. I. Yukalov and V. S. Bagnato}, doi = {10.1103/PhysRevLett.134.023401}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023401}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of relaxation stages in a nonequilibrium closed quantum system: Decaying turbulence in a trapped superfluid}, volume = {134}, year = {2025}, }
• (2025). $^{115}{\mathrm{In}}^{+}\text{\ensuremath{-}}^{172}{\mathrm{Yb}}^{+}$ coulomb crystal clock with $2.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}18}$ systematic uncertainty. PRL, 134(2), 023201. (www)

  @article{ , abstract = {We present a scalable mixed-species Coulomb crystal clock based on the S 0 1 ↔ P 3 0 transition in In + 115 . Yb + 172 ions are cotrapped and used for sympathetic cooling. Reproducible interrogation conditions for mixed-species Coulomb crystals are ensured by a conditional preparation sequence with permutation control. We demonstrate clock operation with a 1 In + − 3 Yb + crystal, achieving a relative systematic uncertainty of 2.5 × 10 − 18 and a relative frequency instability of 1.6 × 10 − 15 / τ / 1 s . We report on absolute frequency measurements with an uncertainty of 1.3 × 10 − 16 and optical frequency comparisons with clocks based on Yb + 171 ( E 3 ) and Sr 87 . With a fractional uncertainty of 4.4 × 10 − 18 , the former is—to our knowledge—the most accurate frequency ratio value reported to date. For the In + 115 / Sr 87 ratio, we improve upon the best previous measurement by more than an order of magnitude. We also demonstrate operation with four In + 115 clock ions, which reduces the instability to 9.2 × 10 − 16 / τ / 1 s .}, archive = {J_PRL}, author = {H. N. Hausser and J. Keller and T. Nordmann and N. M. Bhatt and J. Kiethe and H. Liu and I. M. Richter and M. von Boehn and J. Rahm and S. Weyers and E. Benkler and B. Lipphardt and S. Dörscher and K. Stahl and J. Klose and C. Lisdat and M. Filzinger and N. Huntemann and E. Peik and T. E. Mehlstäubler}, doi = {10.1103/PhysRevLett.134.023201}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {023201}, shortjournal = {Phys. Rev. Lett.}, title = {$^{115}{\mathrm{In}}^{+}\text{\ensuremath{-}}^{172}{\mathrm{Yb}}^{+}$ coulomb crystal clock with $2.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}18}$ systematic uncertainty}, volume = {134}, year = {2025}, }
• (2025). Gamma decay of the $^{154}\mathrm{Sm}$ isovector giant dipole resonance: Smekal-raman scattering as a novel probe of nuclear ground-state deformation. PRL, 134(2), 022503. (www)

  @article{ , abstract = {γ decays of the isovector giant dipole resonance (IVGDR) of the deformed nucleus Sm 154 were measured using 2 1 + -Smekal-Raman and elastic scattering of linearly polarized, quasimonochromatic photon beams. The two scattering processes were disentangled through their distinct angular distributions. Their branching ratio and cross sections were determined at six excitation energies covering the Sm 154 IVGDR. Both agree with the predictions of the geometrical model for the IVGDR and confirm γ decay as an observable sensitive to the structure of the resonance. Consequently, the data place strong constraints on the nuclear shape, including the degree of triaxiality. The derived Sm 154 shape parameters β = 0.2925 ( 25 ) and γ = 5.0 ( 15 ) ° agree well with other measurements and recent Monte Carlo shell-model calculations.}, archive = {J_PRL}, author = {J. Kleemann and N. Pietralla and U. Friman-Gayer and J. Isaak and O. Papst and K. Prifti and V. Werner and A. D. Ayangeakaa and T. Beck and G. Colò and M. L. Cortés and S. W. Finch and M. Fulghieri and D. Gribble and K. E. Ide and X. K.-H. James and R. V. F. Janssens and S. R. Johnson and P. Koseoglou and Krishichayan and D. Savran and W. Tornow}, doi = {10.1103/PhysRevLett.134.022503}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {022503}, shortjournal = {Phys. Rev. Lett.}, title = {Gamma decay of the $^{154}\mathrm{Sm}$ isovector giant dipole resonance: Smekal-raman scattering as a novel probe of nuclear ground-state deformation}, volume = {134}, year = {2025}, }
• (2025). First identification of excited states in $^{78}\mathrm{Zr}$ and implications for isospin nonconserving forces in nuclei. PRL, 134(2), 022502. (www)

  @article{ , abstract = {At a fundamental level, the interactions between protons and protons, protons and neutrons, and neutrons and neutrons are not identical. Such isospin nonconserving interactions emerge when comparing the excitation energy of analog states in triplet nuclei. Here, we extend such an analysis to the , triplet system—the heaviest system for which such complete data exists—and find strong disagreement with contemporary theory. This was achieved by pioneering the technique of recoil- tagging to identify excited states in . We also established a half-life of and extended the band in to .}, archive = {J_PRL}, author = {G. L. Zimba and P. Ruotsalainen and D. G. Jenkins and W. Satuła and J. Uusitalo and R. Wadsworth and X. Pereira Lopez and K. Auranen and A. D. Briscoe and B. Cederwall and S. Chen and G. de Angelis and M. Doncel and A. Ertoprak and T. Grahn and P. T. Greenlees and A. Illana and H. Joukainen and R. Julin and H. Jutila and J. Keatings and J. Louko and M. Luoma and A. M. Plaza and J. Sarén and B. S. Nara Singh and J. Ojala and J. Pakarinen and P. Rahkila and J. Romero and A. Sood and A. Stott and C. Sullivan and H. Tann and A. Tolosa Delgado}, doi = {10.1103/PhysRevLett.134.022502}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {022502}, shortjournal = {Phys. Rev. Lett.}, title = {First identification of excited states in $^{78}\mathrm{Zr}$ and implications for isospin nonconserving forces in nuclei}, volume = {134}, year = {2025}, }
• (2025). Stepping into the sea of instability: The new sub-$\mathrm{\ensuremath{\mu}}\mathrm{s}$ superheavy nucleus $^{252}\mathrm{Rf}$. PRL, 134(2), 022501. (www)

  @article{ , abstract = {We report the discovery of the new isotope Rf 252 . With its extremely short half-life of 60 − 30 + 90 ns , it expands the range of half-lives of the known superheavy nuclei by about 2 orders of magnitude. This nucleus was synthesized in its high- K isomeric state, for which we measured a half-life of 13 − 3 + 4 μ s . Our results confirm a smooth onset of decreasing ground-state spontaneous fission half-lives in the neutron-deficient Rf isotopes toward the isotopic border of 10 − 14 s , which is the time needed to form an atomic shell. Our findings set a new benchmark for further exploration of phenomena associated with high- K states and inverted fission stability in the heaviest nuclei.}, archive = {J_PRL}, author = {J. Khuyagbaatar and P. Mosat and J. Ballof and R. A. Cantemir and Ch. E. Düllmann and K. Hermainski and F. P. Heßberger and E. Jäger and B. Kindler and J. Krier and N. Kurz and S. Löchner and B. Lommel and B. Schausten and Y. Wei and P. Wieczorek and A. Yakushev}, doi = {10.1103/PhysRevLett.134.022501}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {022501}, shortjournal = {Phys. Rev. Lett.}, title = {Stepping into the sea of instability: The new sub-$\mathrm{\ensuremath{\mu}}\mathrm{s}$ superheavy nucleus $^{252}\mathrm{Rf}$}, volume = {134}, year = {2025}, }
• (2025). Probing strangeness hadronization with event-by-event production of multistrange hadrons. PRL, 134(2), 022303. (www)

  @article{ , abstract = {This Letter presents the first measurement of event-by-event fluctuations of the net number (difference between the particle and antiparticle multiplicities) of multistrange hadrons and and its correlation with the net-kaon number using the data collected by the ALICE Collaboration in pp, p-Pb, and Pb-Pb collisions at a center-of-mass energy per nucleon pair . The statistical hadronization model with a correlation over three units of rapidity between hadrons having the same and opposite strangeness content successfully describes the results. On the other hand, string-fragmentation models that mainly correlate strange hadrons with opposite strange quark content over a small rapidity range fail to describe the data.}, archive = {J_PRL}, author = {ALICE Collaboration and S. Acharya and D. Adamová and A. Agarwal and G. Aglieri Rinella and L. Aglietta and M. Agnello and N. Agrawal and Z. Ahammed and S. Ahmad and S. U. Ahn and I. Ahuja and A. Akindinov and V. Akishina and M. Al-Turany and D. Aleksandrov and B. Alessandro and H. M. Alfanda and R. Alfaro Molina and B. Ali and A. Alici and N. Alizadehvandchali and A. Alkin and J. Alme and G. Alocco and T. Alt and A. R. Altamura and I. Altsybeev and J. R. Alvarado and C. O. R. Alvarez and M. N. Anaam and C. Andrei and N. Andreou and A. Andronic and E. Andronov and V. Anguelov and F. Antinori and P. Antonioli and N. Apadula and L. Aphecetche and H. Appelshäuser and C. Arata and S. Arcelli and M. Aresti and R. Arnaldi and J. G. M. C. A. Arneiro and I. C. Arsene and M. Arslandok and A. Augustinus and R. Averbeck and D. Averyanov and M. D. Azmi and H. Baba and A. Badalà and J. Bae and Y. W. Baek and X. Bai and R. Bailhache and Y. Bailung and R. Bala and A. Balbino and A. Baldisseri and B. Balis and D. Banerjee and Z. Banoo and V. Barbasova and F. Barile and L. Barioglio and M. Barlou and B. Barman and G. G. Barnaföldi and L. S. Barnby and E. Barreau and V. Barret and L. Barreto and C. Bartels and K. Barth and E. Bartsch and N. Bastid and S. Basu and G. Batigne and D. Battistini and B. Batyunya and D. Bauri and J. L. Bazo Alba and I. G. Bearden and C. Beattie and P. Becht and D. Behera and I. Belikov and A. D. C. Bell Hechavarria and F. Bellini and R. Bellwied and S. Belokurova and L. G. E. Beltran and Y. A. V. Beltran and G. Bencedi and A. Bensaoula and S. Beole and Y. Berdnikov and A. Berdnikova and L. Bergmann and M. G. Besoiu and L. Betev and P. P. Bhaduri and A. Bhasin and B. Bhattacharjee and L. Bianchi and N. Bianchi and J. Bielčík and J. Bielčíková and A. P. Bigot and A. Bilandzic and G. Biro and S. Biswas and N. Bize and J. T. Blair and D. Blau and M. B. Blidaru and N. Bluhme and C. Blume and G. Boca and F. Bock and T. Bodova and J. Bok and L. Boldizsár and M. Bombara and P. M. Bond and G. Bonomi and H. Borel and A. Borissov and A. G. Borquez Carcamo and H. Bossi and E. Botta and Y. E. M. Bouziani and L. Bratrud and P. Braun-Munzinger and M. Bregant and M. Broz and G. E. Bruno and V. D. Buchakchiev and M. D. Buckland and D. Budnikov and H. Buesching and S. Bufalino and P. Buhler and N. Burmasov and Z. Buthelezi and A. Bylinkin and S. A. Bysiak and J. C. Cabanillas Noris and M. F. T. Cabrera and M. Cai and H. Caines and A. Caliva and E. Calvo Villar and J. M. M. Camacho and P. Camerini and F. D. M. Canedo and S. L. Cantway and M. Carabas and A. A. Carballo and F. Carnesecchi and R. Caron and L. A. D. Carvalho and J. Castillo Castellanos and M. Castoldi and F. Catalano and S. Cattaruzzi and C. Ceballos Sanchez and R. Cerri and I. Chakaberia and P. Chakraborty and S. Chandra and S. Chapeland and M. Chartier and S. Chattopadhay and S. Chattopadhyay and M. Chen and T. Cheng and C. Cheshkov and V. Chibante Barroso and D. D. Chinellato and E. S. Chizzali and J. Cho and S. Cho and P. Chochula and Z. A. Chochulska and D. Choudhury and P. Christakoglou and C. H. Christensen and P. Christiansen and T. Chujo and M. Ciacco and C. Cicalo and M. R. Ciupek and G. Clai and F. Colamaria and J. S. Colburn and D. Colella and M. Colocci and M. Concas and G. Conesa Balbastre and Z. Conesa del Valle and G. Contin and J. G. Contreras and M. L. Coquet and P. Cortese and M. R. Cosentino and F. Costa and S. Costanza and C. Cot and J. Crkovská and P. Crochet and R. Cruz-Torres and P. Cui and M. M. Czarnynoga and A. Dainese and G. Dange and M. C. Danisch and A. Danu and P. Das and S. Das and A. R. Dash and S. Dash and A. De Caro and G. de Cataldo and J. de Cuveland and A. De Falco and D. De Gruttola and N. De Marco and C. De Martin and S. De Pasquale and R. Deb and R. Del Grande and L. Dello Stritto and W. Deng and K. C. Devereaux and P. Dhankher and D. Di Bari and A. Di Mauro and B. Diab and R. A. Diaz and T. Dietel and Y. Ding and J. Ditzel and R. Divià and Ø. Djuvsland and U. Dmitrieva and A. Dobrin and B. Dönigus and J. M. Dubinski and A. Dubla and P. Dupieux and N. Dzalaiova and T. M. Eder and R. J. Ehlers and F. Eisenhut and R. Ejima and D. Elia and B. Erazmus and F. Ercolessi and B. Espagnon and G. Eulisse and D. Evans and S. Evdokimov and L. Fabbietti and M. Faggin and J. Faivre and F. Fan and W. Fan and A. Fantoni and M. Fasel and A. Feliciello and G. Feofilov and A. Fernández Téllez and L. Ferrandi and M. B. Ferrer and A. Ferrero and C. Ferrero and A. Ferretti and V. J. G. Feuillard and V. Filova and D. Finogeev and F. M. Fionda and E. Flatland and F. Flor and A. N. Flores and S. Foertsch and I. Fokin and S. Fokin and U. Follo and E. Fragiacomo and E. Frajna and U. Fuchs and N. Funicello and C. Furget and A. Furs and T. Fusayasu and J. J. Gaardhøje and M. Gagliardi and A. M. Gago and T. Gahlaut and C. D. Galvan and D. R. Gangadharan and P. Ganoti and C. Garabatos and J. M. Garcia and T. García Chávez and E. Garcia-Solis and C. Gargiulo and P. Gasik and H. M. Gaur and A. Gautam and M. B. Gay Ducati and M. Germain and R. A. Gernhaeuser and C. Ghosh and M. Giacalone and G. Gioachin and S. K. Giri and P. Giubellino and P. Giubilato and A. M. C. Glaenzer and P. Glässel and E. Glimos and D. J. Q. Goh and V. Gonzalez and P. Gordeev and M. Gorgon and K. Goswami and S. Gotovac and V. Grabski and L. K. Graczykowski and E. Grecka and A. Grelli and C. Grigoras and V. Grigoriev and S. Grigoryan and F. Grosa and J. F. Grosse-Oetringhaus and R. Grosso and D. Grund and N. A. Grunwald and G. G. Guardiano and R. Guernane and M. Guilbaud and K. Gulbrandsen and J. J. W. K. Gumprecht and T. Gündem and T. Gunji and W. Guo and A. Gupta and R. Gupta and K. Gwizdziel and L. Gyulai and C. Hadjidakis and F. U. Haider and S. Haidlova and M. Haldar and H. Hamagaki and A. Hamdi and Y. Han and B. G. Hanley and R. Hannigan and J. Hansen and M. R. Haque and J. W. Harris and A. Harton and M. V. Hartung and H. Hassan and D. Hatzifotiadou and P. Hauer and L. B. Havener and E. Hellbär and H. Helstrup and M. Hemmer and T. Herman and S. G. Hernandez and G. Herrera Corral and S. Herrmann and K. F. Hetland and B. Heybeck and H. Hillemanns and B. Hippolyte and F. W. Hoffmann and B. Hofman and G. H. Hong and M. Horst and A. Horzyk and Y. Hou and P. Hristov and P. Huhn and L. M. Huhta and T. J. Humanic and A. Hutson and D. Hutter and M. C. Hwang and R. Ilkaev and M. Inaba and G. M. Innocenti and M. Ippolitov and A. Isakov and T. Isidori and M. S. Islam and S. Iurchenko and M. Ivanov and V. Ivanov and K. E. Iversen and M. Jablonski and B. Jacak and N. Jacazio and P. M. Jacobs and S. Jadlovska and J. Jadlovsky and S. Jaelani and C. Jahnke and M. J. Jakubowska and M. A. Janik and T. Janson and S. Ji and S. Jia and A. A. P. Jimenez and F. Jonas and D. M. Jones and J. M. Jowett and J. Jung and M. Jung and A. Junique and A. Jusko and J. Kaewjai and P. Kalinak and A. Kalweit and A. Karasu Uysal and D. Karatovic and N. Karatzenis and O. Karavichev and T. Karavicheva and E. Karpechev and M. J. Karwowska and U. Kebschull and R. Keidel and M. Keil and B. Ketzer and S. S. Khade and A. M. Khan and S. Khan and A. Khanzadeev and Y. Kharlov and A. Khatun and A. Khuntia and Z. Khuranova and B. Kileng and B. Kim and C. Kim and D. J. Kim and E. J. Kim and J. Kim and M. Kim and S. Kim and T. Kim and K. Kimura and A. Kirkova and S. Kirsch and I. Kisel and S. Kiselev and A. Kisiel and J. P. Kitowski and J. L. Klay and J. Klein and S. Klein and C. Klein-Bösing and M. Kleiner and T. Klemenz and A. Kluge and C. Kobdaj and R. Kohara and T. Kollegger and A. Kondratyev and N. Kondratyeva and J. Konig and S. A. Konigstorfer and P. J. Konopka and G. Kornakov and M. Korwieser and S. D. Koryciak and C. Koster and A. Kotliarov and N. Kovacic and V. Kovalenko and M. Kowalski and V. Kozhuharov and I. Králik and A. Kravčáková and L. Krcal and M. Krivda and F. Krizek and K. Krizkova Gajdosova and C. Krug and M. Krüger and D. M. Krupova and E. Kryshen and V. Kučera and C. Kuhn and P. G. Kuijer and T. Kumaoka and D. Kumar and L. Kumar and N. Kumar and S. Kumar and S. Kundu and P. Kurashvili and A. Kurepin and A. B. Kurepin and A. Kuryakin and S. Kushpil and V. Kuskov and M. Kutyla and A. Kuznetsov and M. J. Kweon and Y. Kwon and S. L. La Pointe and P. La Rocca and A. Lakrathok and M. Lamanna and A. R. Landou and R. Langoy and P. Larionov and E. Laudi and L. Lautner and R. A. N. Laveaga and R. Lavicka and R. Lea and H. Lee and I. Legrand and G. Legras and J. Lehrbach and A. M. Lejeune and T. M. Lelek and R. C. Lemmon and I. León Monzón and M. M. Lesch and E. D. Lesser and P. Lévai and M. Li and X. Li and B. E. Liang-gilman and J. Lien and R. Lietava and I. Likmeta and B. Lim and S. H. Lim and V. Lindenstruth and A. Lindner and C. Lippmann and D. H. Liu and J. Liu and G. S. S. Liveraro and I. M. Lofnes and C. Loizides and S. Lokos and J. Lömker and X. Lopez and E. López Torres and C. Lotteau and P. Lu and F. V. Lugo and J. R. Luhder and M. Lunardon and G. Luparello and Y. G. Ma and M. Mager and A. Maire and E. M. Majerz and M. V. Makariev and M. Malaev and G. Malfattore and N. M. Malik and Q. W. Malik and S. K. Malik and L. Malinina and D. Mallick and N. Mallick and G. Mandaglio and S. K. Mandal and A. Manea and V. Manko and F. Manso and V. Manzari and Y. Mao and R. W. Marcjan and G. V. Margagliotti and A. Margotti and A. Marín and C. Markert and P. Martinengo and M. I. Martínez and G. Martínez García and M. P. P. Martins and S. Masciocchi and M. Masera and A. Masoni and L. Massacrier and O. Massen and A. Mastroserio and O. Matonoha and S. Mattiazzo and A. Matyja and A. L. Mazuecos and F. Mazzaschi and M. Mazzilli and J. E. Mdhluli and Y. Melikyan and M. Melo and A. Menchaca-Rocha and J. E. M. Mendez and E. Meninno and A. S. Menon and M. W. Menzel and M. Meres and Y. Miake and L. Micheletti and D. L. Mihaylov and K. Mikhaylov and N. Minafra and D. Miśkowiec and A. Modak and B. Mohanty and M. Mohisin Khan and M. A. Molander and S. Monira and C. Mordasini and D. A. Moreira De Godoy and I. Morozov and A. Morsch and T. Mrnjavac and V. Muccifora and S. Muhuri and J. D. Mulligan and A. Mulliri and M. G. Munhoz and R. H. Munzer and H. Murakami and S. Murray and L. Musa and J. Musinsky and J. W. Myrcha and B. Naik and A. I. Nambrath and B. K. Nandi and R. Nania and E. Nappi and A. F. Nassirpour and A. Nath and S. Nath and C. Nattrass and M. N. Naydenov and A. Neagu and A. Negru and E. Nekrasova and L. Nellen and R. Nepeivoda and S. Nese and G. Neskovic and N. Nicassio and B. S. Nielsen and E. G. Nielsen and S. Nikolaev and S. Nikulin and V. Nikulin and F. Noferini and S. Noh and P. Nomokonov and J. Norman and N. Novitzky and P. Nowakowski and A. Nyanin and J. Nystrand and S. Oh and A. Ohlson and V. A. Okorokov and J. Oleniacz and A. Onnerstad and C. Oppedisano and A. Ortiz Velasquez and J. Otwinowski and M. Oya and K. Oyama and Y. Pachmayer and S. Padhan and D. Pagano and G. Paić and S. Paisano-Guzmán and A. Palasciano and S. Panebianco and C. Pantouvakis and H. Park and J. Park and J. E. Parkkila and Y. Patley and R. N. Patra and B. Paul and H. Pei and T. Peitzmann and X. Peng and M. Pennisi and S. Perciballi and D. Peresunko and G. M. Perez and Y. Pestov and M. T. Petersen and V. Petrov and M. Petrovici and S. Piano and M. Pikna and P. Pillot and O. Pinazza and L. Pinsky and C. Pinto and S. Pisano and M. Płoskoń and M. Planinic and F. Pliquett and D. K. Plociennik and M. G. Poghosyan and B. Polichtchouk and S. Politano and N. Poljak and A. Pop and S. Porteboeuf-Houssais and V. Pozdniakov and I. Y. Pozos and K. K. Pradhan and S. K. Prasad and S. Prasad and R. Preghenella and F. Prino and C. A. Pruneau and I. Pshenichnov and M. Puccio and S. Pucillo and S. Qiu and L. Quaglia and S. Ragoni and A. Rai and A. Rakotozafindrabe and L. Ramello and F. Rami and M. Rasa and S. S. Räsänen and R. Rath and M. P. Rauch and I. Ravasenga and K. F. Read and C. Reckziegel and A. R. Redelbach and K. Redlich and C. A. Reetz and H. D. Regules-Medel and A. Rehman and F. Reidt and H. A. Reme-Ness and Z. Rescakova and K. Reygers and A. Riabov and V. Riabov and R. Ricci and M. Richter and A. A. Riedel and W. Riegler and A. G. Riffero and M. Rignanese and C. Ripoli and C. Ristea and M. V. Rodriguez and M. Rodríguez Cahuantzi and S. A. Rodríguez Ramírez and K. Røed and R. Rogalev and E. Rogochaya and T. S. Rogoschinski and D. Rohr and D. Röhrich and S. Rojas Torres and P. S. Rokita and G. Romanenko and F. Ronchetti and E. D. Rosas and K. Roslon and A. Rossi and A. Roy and S. Roy and N. Rubini and J. A. Rudolph and D. Ruggiano and R. Rui and P. G. Russek and R. Russo and A. Rustamov and E. Ryabinkin and Y. Ryabov and A. Rybicki and J. Ryu and W. Rzesa and B. Sabiu and S. Sadovsky and J. Saetre and K. Šafařík and S. K. Saha and S. Saha and B. Sahoo and R. Sahoo and S. Sahoo and D. Sahu and P. K. Sahu and J. Saini and K. Sajdakova and S. Sakai and M. P. Salvan and S. Sambyal and D. Samitz and I. Sanna and T. B. Saramela and D. Sarkar and P. Sarma and V. Sarritzu and V. M. Sarti and M. H. P. Sas and S. Sawan and E. Scapparone and J. Schambach and H. S. Scheid and C. Schiaua and R. Schicker and F. Schlepper and A. Schmah and C. Schmidt and H. R. Schmidt and M. O. Schmidt and M. Schmidt and N. V. Schmidt and A. R. Schmier and R. Schotter and A. Schröter and J. Schukraft and K. Schweda and G. Scioli and E. Scomparin and J. E. Seger and Y. Sekiguchi and D. Sekihata and M. Selina and I. Selyuzhenkov and S. Senyukov and J. J. Seo and D. Serebryakov and L. Serkin and L. Šerkšnytė and A. Sevcenco and T. J. Shaba and A. Shabetai and R. Shahoyan and A. Shangaraev and B. Sharma and D. Sharma and H. Sharma and M. Sharma and S. Sharma and U. Sharma and A. Shatat and O. Sheibani and K. Shigaki and M. Shimomura and J. Shin and S. Shirinkin and Q. Shou and Y. Sibiriak and S. Siddhanta and T. Siemiarczuk and T. F. Silva and D. Silvermyr and T. Simantathammakul and R. Simeonov and B. Singh and K. Singh and R. Singh and S. Singh and V. K. Singh and V. Singhal and T. Sinha and B. Sitar and M. Sitta and T. B. Skaali and G. Skorodumovs and N. Smirnov and R. J. M. Snellings and E. H. Solheim and J. Song and C. Sonnabend and J. M. Sonneveld and F. Soramel and A. B. Soto-hernandez and R. Spijkers and I. Sputowska and J. Staa and J. Stachel and I. Stan and P. J. Steffanic and S. F. Stiefelmaier and D. Stocco and I. Storehaug and N. J. Strangmann and P. Stratmann and S. Strazzi and A. Sturniolo and C. P. Stylianidis and A. A. P. Suaide and C. Suire and M. Sukhanov and M. Suljic and R. Sultanov and V. Sumberia and S. Sumowidagdo and I. Szarka and M. Szymkowski and S. F. Taghavi and G. Taillepied and J. Takahashi and G. J. Tambave and S. Tang and Z. Tang and J. D. Tapia Takaki and N. Tapus and L. A. Tarasovicova and M. G. Tarzila and G. F. Tassielli and A. Tauro and A. Tavira García and G. Tejeda Muñoz and A. Telesca and L. Terlizzi and C. Terrevoli and S. Thakur and D. Thomas and A. Tikhonov and N. Tiltmann and A. R. Timmins and M. Tkacik and T. Tkacik and A. Toia and R. Tokumoto and S. Tomassini and K. Tomohiro and N. Topilskaya and M. Toppi and V. V. Torres and A. G. Torres Ramos and A. Trifiró and T. Triloki and A. S. Triolo and S. Tripathy and T. Tripathy and V. Trubnikov and W. H. Trzaska and T. P. Trzcinski and C. Tsolanta and R. Tu and A. Tumkin and R. Turrisi and T. S. Tveter and K. Ullaland and B. Ulukutlu and A. Uras and M. Urioni and G. L. Usai and M. Vala and N. Valle and L. V. R. van Doremalen and M. van Leeuwen and C. A. van Veen and R. J. G. van Weelden and P. Vande Vyvre and D. Varga and Z. Varga and P. Vargas Torres and M. Vasileiou and A. Vasiliev and O. Vázquez Doce and O. Vazquez Rueda and V. Vechernin and E. Vercellin and S. Vergara Limón and R. Verma and L. Vermunt and R. Vértesi and M. Verweij and L. Vickovic and Z. Vilakazi and O. Villalobos Baillie and A. Villani and A. Vinogradov and T. Virgili and M. M. O. Virta and A. Vodopyanov and B. Volkel and M. A. Völkl and S. A. Voloshin and G. Volpe and B. von Haller and I. Vorobyev and N. Vozniuk and J. Vrláková and J. Wan and C. Wang and D. Wang and Y. Wang and A. Wegrzynek and F. T. Weiglhofer and S. C. Wenzel and J. P. Wessels and J. Wiechula and J. Wikne and G. Wilk and J. Wilkinson and G. A. Willems and B. Windelband and M. Winn and J. R. Wright and W. Wu and Y. Wu and Z. Xiong and R. Xu and A. Yadav and A. K. Yadav and Y. Yamaguchi and S. Yang and S. Yano and E. R. Yeats and Z. Yin and I.-K. Yoo and J. H. Yoon and H. Yu and S. Yuan and A. Yuncu and V. Zaccolo and C. Zampolli and M. Zang and F. Zanone and N. Zardoshti and A. Zarochentsev and P. Závada and N. Zaviyalov and M. Zhalov and B. Zhang and C. Zhang and L. Zhang and M. Zhang and S. Zhang and X. Zhang and Y. Zhang and Z. Zhang and M. Zhao and V. Zherebchevskii and Y. Zhi and D. Zhou and Y. Zhou and J. Zhu and S. Zhu and Y. Zhu and S. C. Zugravel and N. Zurlo}, doi = {10.1103/PhysRevLett.134.022303}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {022303}, shortjournal = {Phys. Rev. Lett.}, title = {Probing strangeness hadronization with event-by-event production of multistrange hadrons}, volume = {134}, year = {2025}, }
• (2025). Disentangling centrality bias and final-state effects in the production of high-${p}_{T}$ neutral pions using direct photon in $d+\mathrm{Au}$ collisions at $\sqrt{{s}_{NN}}=200\text{ }\text{ }\mathrm{GeV}$. PRL, 134(2), 022302. (www)

  @article{ , abstract = {PHENIX presents a simultaneous measurement of the production of direct and in collisions at over a range of 7.5 to for different event samples selected by event activity, i.e., charged-particle multiplicity detected at forward rapidity. Direct-photon yields are used to empirically estimate the contribution of hard-scattering processes in the different event samples. Using this estimate, the average nuclear-modification factor, is , consistent with unity for minimum-bias (MB) collisions. For event classes with low and moderate event activity, is consistent with the MB value within 5% uncertainty. This result confirms that the previously observed enhancement of high- production found in small-system collisions with low event activity is a result of a bias in interpreting event activity within the Glauber framework. In contrast, for the top 5% of events with the highest event activity, is suppressed by 20% relative to the MB value with a significance of , which may be due to final-state effects. This suppression corresponds to a shift of at .}, archive = {J_PRL}, author = {N. J. Abdulameer and U. Acharya and C. Aidala and Y. Akiba and M. Alfred and K. Aoki and N. Apadula and C. Ayuso and V. Babintsev and V. Babintsev and K. N. Barish and S. Bathe and A. Bazilevsky and R. Belmont and A. Berdnikov and Y. Berdnikov and L. Bichon and B. Blankenship and D. S. Blau and M. Boer and J. S. Bok and V. Borisov and M. L. Brooks and J. Bryslawskyj and V. Bumazhnov and C. Butler and S. Campbell and V. Canoa Roman and M. Chiu and M. Connors and R. Corliss and Y. Corrales Morales and M. Csanád and T. Csörgő and L. D. Liu and T. W. Danley and M. S. Daugherity and G. David and C. T. Dean and K. DeBlasio and K. Dehmelt and A. Denisov and A. Deshpande and E. J. Desmond and V. Doomra and J. H. Do and A. Drees and K. A. Drees and M. Dumancic and J. M. Durham and A. Durum and T. Elder and A. Enokizono and R. Esha and B. Fadem and W. Fan and N. Feege and M. Finger, Jr. and M. Finger and D. Firak and D. Fitzgerald and S. L. Fokin and J. E. Frantz and A. Franz and A. D. Frawley and Y. Fukuda and C. Gal and P. Garg and H. Ge and M. Giles and Y. Goto and N. Grau and S. V. Greene and T. Gunji and T. Hachiya and J. S. Haggerty and K. I. Hahn and S. Y. Han and M. Harvey and S. Hasegawa and T. O. S. Haseler and T. K. Hemmick and X. He and K. Hill and A. Hodges and K. Homma and B. Hong and T. Hoshino and N. Hotvedt and J. Huang and J. Imrek and M. Inaba and D. Isenhower and Y. Ito and D. Ivanishchev and B. V. Jacak and Z. Ji and B. M. Johnson and V. Jorjadze and D. Jouan and D. S. Jumper and J. H. Kang and D. Kapukchyan and S. Karthas and A. V. Kazantsev and V. Khachatryan and A. Khanzadeev and A. Khatiwada and C. Kim and D. J. Kim and E.-J. Kim and M. Kim and M. H. Kim and T. Kim and D. Kincses and A. Kingan and E. Kistenev and T. Koblesky and D. Kotov and L. Kovacs and S. Kudo and B. Kurgyis and K. Kurita and J. G. Lajoie and E. O. Lallow and D. Larionova and A. Lebedev and S. H. Lee and M. J. Leitch and Y. H. Leung and N. A. Lewis and S. H. Lim and M. X. Liu and X. Li and V.-R. Loggins and D. A. Loomis and D. Lynch and S. Lökös and T. Majoros and M. Makek and M. Malaev and V. I. Manko and E. Mannel and H. Masuda and M. McCumber and D. McGlinchey and A. C. Mignerey and D. E. Mihalik and A. Milov and D. K. Mishra and J. T. Mitchell and M. Mitrankova and Iu. Mitrankov and G. Mitsuka and M. M. Mondal and T. Moon and D. P. Morrison and S. I. Morrow and A. Muhammad and B. Mulilo and T. Murakami and J. Murata and K. Nagai and K. Nagashima and T. Nagashima and J. L. Nagle and M. I. Nagy and I. Nakagawa and H. Nakagomi and K. Nakano and C. Nattrass and S. Nelson and R. Nouicer and N. Novitzky and R. Novotny and T. Novák and G. Nukazuka and A. S. Nyanin and E. O’Brien and C. A. Ogilvie and J. Oh and J. D. Orjuela Koop and M. Orosz and J. D. Osborn and A. Oskarsson and K. Ozawa and V. Pantuev and V. Papavassiliou and J. S. Park and S. Park and M. Patel and S. F. Pate and W. Peng and D. V. Perepelitsa and G. D. N. Perera and C. E. PerezLara and R. Petti and M. Phipps and C. Pinkenburg and M. Potekhin and A. Pun and M. L. Purschke and P. V. Radzevich and N. Ramasubramanian and K. F. Read and V. Riabov and Y. Riabov and D. Richford and T. Rinn and M. Rosati and Z. Rowan and J. Runchey and T. Sakaguchi and H. Sako and V. Samsonov and M. Sarsour and K. Sato and S. Sato and B. Schaefer and B. K. Schmoll and R. Seidl and A. Sen and R. Seto and A. Sexton and D. Sharma and I. Shein and M. Shibata and T.-A. Shibata and K. Shigaki and M. Shimomura and Z. Shi and C. L. Silva and D. Silvermyr and M. Slunečka and K. L. Smith and S. P. Sorensen and I. V. Sourikova and P. W. Stankus and S. P. Stoll and T. Sugitate and A. Sukhanov and Z. Sun and S. Syed and R. Takahama and A. Takeda and K. Tanida and M. J. Tannenbaum and S. Tarafdar and A. Taranenko and G. Tarnai and R. Tieulent and A. Timilsina and T. Todoroki and M. Tomášek and C. L. Towell and R. S. Towell and I. Tserruya and Y. Ueda and B. Ujvari and H. W. van Hecke and S. Vazquez-Carson and J. Velkovska and M. Virius and V. Vrba and X. R. Wang and Z. Wang and Y. Watanabe and C. P. Wong and C. Xu and Q. Xu and Y. L. Yamaguchi and A. Yanovich and P. Yin and I. Yoon and J. H. Yoo and I. E. Yushmanov and H. Yu and W. A. Zajc and L. Zou}, doi = {10.1103/PhysRevLett.134.022302}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {022302}, shortjournal = {Phys. Rev. Lett.}, title = {Disentangling centrality bias and final-state effects in the production of high-${p}_{T}$ neutral pions using direct photon in $d+\mathrm{Au}$ collisions at $\sqrt{{s}_{NN}}=200\text{ }\text{ }\mathrm{GeV}$}, volume = {134}, year = {2025}, }
• (2025). Deciphering hypertriton and antihypertriton spins from their global polarizations in heavy-ion collisions. PRL, 134(2), 022301. (www)

  @article{ , abstract = {Understanding the properties of hypernuclei is crucial for constraining the nature of hyperon-nucleon ( ) interactions, which plays a key role in determining the inner structure of compact stars. The lightest hypernuclei and antihypernuclei are the hypertriton ( ), which consists of a pair of nucleons and a hyperon, and its antinucleus ( ). Significant knowledge has recently been acquired regarding the mass, lifetime, and binding energy of . However, its exact spin, whether or , remains undetermined in both experimental and theoretical studies. Here, we present a novel method of using the hypertriton global polarization in heavy-ion collisions to decipher not only its total spin but also its internal spin structure. This method is based on the finding that its three different spin structures exhibit distinct beam energy dependence of its global polarization when it is produced in these collisions from the coalescence of proton, neutron and . Future observations of the hypertriton and antihypertriton global polarizations thus provide the opportunity to unveil the spin structures of hypertriton and antihypertriton and their production mechanisms in heavy-ion collisions.}, archive = {J_PRL}, author = {Kai-Jia Sun and Dai-Neng Liu and Yun-Peng Zheng and Jin-Hui Chen and Che Ming Ko and Yu-Gang Ma}, doi = {10.1103/PhysRevLett.134.022301}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {022301}, shortjournal = {Phys. Rev. Lett.}, title = {Deciphering hypertriton and antihypertriton spins from their global polarizations in heavy-ion collisions}, volume = {134}, year = {2025}, }
• (2025). Observation of Λc+→Λa0(980)+ and evidence for Σ(1380)+ in Λc+→Λπ+η. PRL, 134(2), 021901. (www)

  @article{ , abstract = {Based on of annihilation data collected at center-of-mass energies from 4.600 to 4.843 GeV with the BESIII detector at the BEPCII collider, a partial wave analysis of is performed, and branching fractions and decay asymmetry parameters of intermediate processes are determined. The process is observed for the first time, and evidence for the pentaquark candidate decaying into is found with statistical significance larger than with mass and width fixed to theoretical predictions. The branching fraction product is determined to be , which is larger than theoretical calculations by 1–2 orders of magnitude. Here the third (external) systematic is from . Finally, we precisely obtain the absolute branching fraction .}, archive = {J_PRL}, author = {BESIII Collaboration and M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and J. F. Chang and G. R. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and J. J. Lane and P. Larin and L. Lavezzi and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. Z. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. Ma and Y. M. Ma and F. E. Maas and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and P. Patteri and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and H. C. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and N. Y. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. C. Xu and Z. P. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. X. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. D. Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and Z. Z. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and S. Q. Zhu and T. J. Zhu and W. D. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.021901}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {021901}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of Λc+→Λa0(980)+ and evidence for Σ(1380)+ in Λc+→Λπ+η}, volume = {134}, year = {2025}, }
• (2025). First direct search for light dark matter using the NEON experiment at a nuclear reactor. PRL, 134(2), 021802. (www)

  @article{ , abstract = {We report new results from the neutrino elastic scattering observation with NaI (NEON) experiment in the search for light dark matter (LDM) using 2636 kg · days of NaI(Tl) exposure. The experiment employs an array of NaI(Tl) crystals with a total mass of 16.7 kg, located 23.7 m away from a 2.8 GW thermal power nuclear reactor. We investigated LDM produced by the invisible decay of dark photons, a well-motivated mechanism generated by high-flux photons during reactor operation. The energy spectra collected during reactor-on and reactor-off periods were compared within the LDM signal region of 1–10 keV. No signal consistent with LDM interaction with electrons was observed, allowing us to set 90% confidence level exclusion limits on the dark matter-electron scattering cross section ( σ e ) across dark matter masses ranging from 1 to 1000 keV / c 2 . Our results set a 90% confidence level upper limit of σ e = 3.17 × 10 − 35 cm 2 for a dark matter mass of 100 keV / c 2 , marking the best laboratory result in this mass range. Additionally, our search extends the coverage of LDM below 100 keV / c 2 for the first time, assuming the specific invisible decay of dark photons.}, archive = {J_PRL}, author = {J. J. Choi and C. Ha and E. J. Jeon and J. Y. Kim and K. W. Kim and S. H. Kim and S. K. Kim and Y. D. Kim and Y. J. Ko and Y. J. Ko and B. C. Koh and S. H. Lee and I. S. Lee and H. Lee and H. S. Lee and J. S. Lee and Y. M. Oh and B. J. Park}, doi = {10.1103/PhysRevLett.134.021802}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {021802}, shortjournal = {Phys. Rev. Lett.}, title = {First direct search for light dark matter using the NEON experiment at a nuclear reactor}, volume = {134}, year = {2025}, }
• (2025). Distinguishing dirac from majorana heavy neutrino at future lepton colliders. PRL, 134(2), 021801. (www)

  @article{ , abstract = {We propose to identify whether a sterile neutrino is Dirac-type or Majorana-type by counting the peak of the rapidity distribution at lepton colliders. Our method requires only one charged-lepton tagging, and the nature of sterile neutrinos can be pinned down once they are confirmed.}, archive = {J_PRL}, author = {Qing-Hong Cao and Kun Cheng and Yandong Liu}, doi = {10.1103/PhysRevLett.134.021801}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {021801}, shortjournal = {Phys. Rev. Lett.}, title = {Distinguishing dirac from majorana heavy neutrino at future lepton colliders}, volume = {134}, year = {2025}, }
• (2025). Quantized axial charge of staggered fermions and the chiral anomaly. PRL, 134(2), 021601. (www)

  @article{ , abstract = {In the ultralocal lattice Hamiltonian for staggered fermions with a finite-dimensional Hilbert space, there are two conserved, integer-valued charges that flow in the continuum limit to the vector and axial charges of a massless Dirac fermion with a perturbative anomaly. Each of the two lattice charges generates an ordinary U(1) global symmetry that acts locally on operators and can be gauged individually. Interestingly, they do not commute on a finite lattice and generate the Onsager algebra, but their commutator goes to zero in the continuum limit. The chiral anomaly is matched by this non-Abelian algebra, which is consistent with the Nielsen-Ninomiya theorem. We further prove that the presence of these two conserved lattice charges forces the low-energy phase to be gapless, reminiscent of the consequence from perturbative anomalies of continuous global symmetries in continuum field theory. Upon bosonization, these two charges lead to two exact U(1) symmetries in the XX model that flow to the momentum and winding symmetries in the free boson conformal field theory.}, archive = {J_PRL}, author = {Arkya Chatterjee and Salvatore D. Pace and Shu-Heng Shao}, doi = {10.1103/PhysRevLett.134.021601}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {021601}, shortjournal = {Phys. Rev. Lett.}, title = {Quantized axial charge of staggered fermions and the chiral anomaly}, volume = {134}, year = {2025}, }
• (2025). Inference of the mass composition of cosmic rays with energies from ${10}^{18.5}$ to ${10}^{20}\text{ }\text{ }\mathrm{eV}$ using the pierre auger observatory and deep learning. PRL, 134(2), 021001. (www)

  @article{ , abstract = {We present measurements of the atmospheric depth of the shower maximum X max , inferred for the first time on an event-by-event level using the surface detector of the Pierre Auger Observatory. Using deep learning, we were able to extend measurements of the X max distributions up to energies of 100 EeV ( 10 20 eV ), not yet revealed by current measurements, providing new insights into the mass composition of cosmic rays at extreme energies. Gaining a 10-fold increase in statistics compared to the fluorescence detector data, we find evidence that the rate of change of the average X max with the logarithm of energy features three breaks at 6.5 ± 0.6 ( stat ) ± 1 ( syst ) EeV , 11 ± 2 ( stat ) ± 1 ( syst ) EeV , and 31 ± 5 ( stat ) ± 3 ( syst ) EeV , in the vicinity to the three prominent features (ankle, instep, suppression) of the cosmic-ray flux. The energy evolution of the mean and standard deviation of the measured X max distributions indicates that the mass composition becomes increasingly heavier and purer, thus being incompatible with a large fraction of light nuclei between 50 and 100 EeV.}, archive = {J_PRL}, author = {A. Abdul Halim and P. Abreu and M. Aglietta and I. Allekotte and K. Almeida Cheminant and A. Almela and R. Aloisio and J. Alvarez-Muñiz and J. Ammerman Yebra and J. Ammerman Yebra and G. A. Anastasi and L. Anchordoqui and B. Andrada and L. Andrade Dourado and S. Andringa and L. Apollonio and C. Aramo and P. R. Araújo Ferreira and E. Arnone and J. C. Arteaga Velázquez and P. Assis and G. Avila and E. Avocone and A. Bakalova and F. Barbato and A. Bartz Mocellin and C. Berat and M. E. Bertaina and G. Bhatta and M. Bianciotto and P. L. Biermann and V. Binet and K. Bismark and T. Bister and J. Biteau and J. Blazek and C. Bleve and J. Blümer and M. Boháčová and D. Boncioli and C. Bonifazi and L. Bonneau Arbeletche and N. Borodai and J. Brack and P. G. Brichetto Orchera and F. L. Briechle and A. Bueno and S. Buitink and M. Buscemi and M. Büsken and A. Bwembya and K. S. Caballero-Mora and S. Cabana-Freire and L. Caccianiga and F. Campuzano and R. Caruso and A. Castellina and F. Catalani and G. Cataldi and L. Cazon and M. Cerda and B. Čermáková and A. Cermenati and J. A. Chinellato and J. Chudoba and L. Chytka and R. W. Clay and A. C. Cobos Cerutti and R. Colalillo and M. R. Coluccia and R. Conceição and A. Condorelli and G. Consolati and M. Conte and F. Convenga and D. Correia dos Santos and P. J. Costa and C. E. Covault and M. Cristinziani and C. S. Cruz Sanchez and S. Dasso and K. Daumiller and B. R. Dawson and R. M. de Almeida and B. de Errico and J. de Jesús and S. J. de Jong and J. R. T. de Mello Neto and I. De Mitri and J. de Oliveira and D. de Oliveira Franco and F. de Palma and V. de Souza and E. De Vito and A. Del Popolo and O. Deligny and N. Denner and L. Deval and A. di Matteo and J. A. do and M. Dobre and C. Dobrigkeit and J. C. D’Olivo and L. M. Domingues Mendes and Q. Dorosti and J. C. dos Anjos and R. C. dos Anjos and J. Ebr and F. Ellwanger and M. Emam and R. Engel and I. Epicoco and M. Erdmann and A. Etchegoyen and C. Evoli and H. Falcke and G. Farrar and A. C. Fauth and T. Fehler and F. Feldbusch and F. Fenu and A. Fernandes and B. Fick and J. M. Figueira and P. Filip and A. Filipčič and T. Fitoussi and B. Flaggs and T. Fodran and T. Fujii and A. Fuster and C. Galea and B. García and C. Gaudu and A. Gherghel-Lascu and P. L. Ghia and U. Giaccari and J. Glombitza and F. Gobbi and F. Gollan and G. Golup and M. Gómez Berisso and P. F. Gómez Vitale and J. P. Gongora and J. M. González and N. González and D. Góra and A. Gorgi and M. Gottowik and F. Guarino and G. P. Guedes and E. Guido and L. Gülzow and S. Hahn and P. Hamal and M. R. Hampel and P. Hansen and D. Harari and V. M. Harvey and A. Haungs and T. Hebbeker and C. Hojvat and J. R. Hörandel and P. Horvath and M. Hrabovský and T. Huege and A. Insolia and P. G. Isar and P. Janecek and V. Jilek and J. A. Johnsen and J. Jurysek and K.-H. Kampert and B. Keilhauer and A. Khakurdikar and V. V. Kizakke Covilakam and H. O. Klages and M. Kleifges and F. Knapp and J. Köhler and F. Krieger and N. Kunka and B. L. Lago and N. Langner and M. A. Leigui de Oliveira and Y. Lema-Capeans and A. Letessier-Selvon and I. Lhenry-Yvon and L. Lopes and L. Lu and Q. Luce and J. P. Lundquist and A. Machado Payeras and M. Majercakova and D. Mandat and B. C. Manning and P. Mantsch and F. M. Mariani and A. G. Mariazzi and I. C. Mariş and G. Marsella and D. Martello and S. Martinelli and O. Martínez Bravo and M. A. Martins and H.-J. Mathes and J. Matthews and G. Matthiae and E. Mayotte and S. Mayotte and P. O. Mazur and G. Medina-Tanco and J. Meinert and D. Melo and A. Menshikov and C. Merx and S. Michal and M. I. Micheletti and L. Miramonti and S. Mollerach and F. Montanet and L. Morejon and K. Mulrey and R. Mussa and W. M. Namasaka and S. Negi and L. Nellen and K. Nguyen and G. Nicora and M. Niechciol and D. Nitz and D. Nosek and V. Novotny and L. Nožka and A. Nucita and L. A. Núñez and C. Oliveira and M. Palatka and J. Pallotta and S. Panja and G. Parente and T. Paulsen and J. Pawlowsky and M. Pech and J. Pȩkala and R. Pelayo and V. Pelgrims and L. A. S. Pereira and E. E. Pereira Martins and C. Pérez Bertolli and L. Perrone and S. Petrera and C. Petrucci and T. Pierog and M. Pimenta and M. Platino and B. Pont and M. Pothast and M. Pourmohammad Shahvar and P. Privitera and M. Prouza and S. Querchfeld and J. Rautenberg and D. Ravignani and J. V. Reginatto Akim and M. Reininghaus and A. Reuzki and J. Ridky and F. Riehn and M. Risse and V. Rizi and W. Rodrigues de Carvalho and E. Rodriguez and J. Rodriguez Rojo and M. J. Roncoroni and S. Rossoni and M. Roth and E. Roulet and A. C. Rovero and A. Saftoiu and M. Saharan and F. Salamida and H. Salazar and G. Salina and J. D. Sanabria Gomez and F. Sánchez and E. M. Santos and E. Santos and F. Sarazin and R. Sarmento and R. Sato and P. Savina and C. M. Schäfer and V. Scherini and H. Schieler and M. Schimassek and M. Schimp and D. Schmidt and O. Scholten and H. Schoorlemmer and P. Schovánek and F. G. Schröder and J. Schulte and T. Schulz and S. J. Sciutto and M. Scornavacche and A. Sedoski and A. Segreto and S. Sehgal and S. U. Shivashankara and G. Sigl and K. Simkova and F. Simon and R. Smau and R. Šmída and P. Sommers and R. Squartini and M. Stadelmaier and S. Stanič and J. Stasielak and P. Stassi and S. Strähnz and M. Straub and T. Suomijärvi and A. D. Supanitsky and Z. Svozilikova and Z. Szadkowski and F. Tairli and A. Tapia and C. Taricco and C. Timmermans and O. Tkachenko and P. Tobiska and C. J. Todero Peixoto and B. Tomé and Z. Torrès and A. Travaini and P. Travnicek and M. Tueros and M. Unger and R. Uzeiroska and L. Vaclavek and M. Vacula and J. F. Valdés Galicia and L. Valore and E. Varela and V. Vašíčková and A. Vásquez-Ramírez and D. Veberič and I. D. Vergara Quispe and V. Verzi and J. Vicha and J. Vink and S. Vorobiov and C. Watanabe and A. A. Watson and A. Weindl and L. Wiencke and H. Wilczyński and D. Wittkowski and B. Wundheiler and B. Yue and A. Yushkov and O. Zapparrata and E. Zas and D. Zavrtanik and M. Zavrtanik}, doi = {10.1103/PhysRevLett.134.021001}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {021001}, shortjournal = {Phys. Rev. Lett.}, title = {Inference of the mass composition of cosmic rays with energies from ${10}^{18.5}$ to ${10}^{20}\text{ }\text{ }\mathrm{eV}$ using the pierre auger observatory and deep learning}, volume = {134}, year = {2025}, }
• (2025). Fundamental limit on the power of entanglement assistance in quantum communication. PRL, 134(2), 020802. (www)

  @article{ , abstract = {The optimal rate of reliable communication over a quantum channel can be enhanced by preshared entanglement. Whereas the enhancement may be unbounded in infinite-dimensional settings even when the input power is constrained, a long-standing conjecture asserts that the ratio between the entanglement-assisted and unassisted classical capacities is bounded in finite-dimensional settings [Bennett et al. , IEEE Trans. Inf. Theory 48 , 2637 (2002) ]. In this Letter, we prove this conjecture by showing that their ratio is upper bounded by , where is the input dimension of the channel. An application to quantum communication with noisy encoders and decoders is given.}, archive = {J_PRL}, author = {Lasse H. Wolff and Paula Belzig and Matthias Christandl and Bergfinnur Durhuus and Marco Tomamichel}, doi = {10.1103/PhysRevLett.134.020802}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020802}, shortjournal = {Phys. Rev. Lett.}, title = {Fundamental limit on the power of entanglement assistance in quantum communication}, volume = {134}, year = {2025}, }
• (2025). Long-range $ZZ$ interaction via resonator-induced phase in superconducting qubits. PRL, 134(2), 020801. (www)

  @article{ , abstract = {Superconducting quantum computing emerges as one of the leading candidates for achieving quantum advantage. However, a prevailing challenge is the coding overhead due to limited quantum connectivity, constrained by nearest-neighbor coupling among superconducting qubits. Here, we propose a novel multimode coupling scheme using three resonators driven by two microwaves, based on the resonator-induced phase gate, to extend the interaction distance between qubits. We demonstrate a controlled-Z ( cz ) gate fidelity exceeding 99.9% within 160 ns at a free spectral range (FSR) of 1.4 GHz, and by optimizing driving pulses, we further reduce the residual photon to nearly within 100 ns at a FSR of 0.2 GHz. These facilitate the long-range cz gate over separations reaching submeters, thus significantly enhancing qubit connectivity and making a practical step toward the scalable integration and modularization of quantum processors. Specifically, our approach supports the implementation of quantum error correction codes requiring high connectivity, such as low-density parity check codes that pave the way to achieving fault-tolerant quantum computing.}, archive = {J_PRL}, author = {Xiang Deng and Wen Zheng and Xudong Liao and Haoyu Zhou and Yangyang Ge and Jie Zhao and Dong Lan and Xinsheng Tan and Yu Zhang and Shaoxiong Li and Yang Yu}, doi = {10.1103/PhysRevLett.134.020801}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020801}, shortjournal = {Phys. Rev. Lett.}, title = {Long-range $ZZ$ interaction via resonator-induced phase in superconducting qubits}, volume = {134}, year = {2025}, }
• (2025). Pauli noise learning for mid-circuit measurements. PRL, 134(2), 020602. (www)

  @article{ , abstract = {Current benchmarks for midcircuit measurements (MCMs) are limited in scalability or the types of error they can quantify, necessitating new techniques for quantifying MCM performance. Here, we introduce a theory for learning stochastic Pauli noise in MCMs and use it to create MCM cycle benchmarking, a scalable method for benchmarking MCMs. MCM cycle benchmarking extracts detailed information about the rates of errors in randomly compiled layers of MCMs and Clifford gates, and we demonstrate how its results can be used to quantify correlated errors during MCMs on current quantum hardware. Our method can be integrated with existing Pauli noise learning techniques to scalably characterize the errors in wide classes of circuits containing MCMs.}, archive = {J_PRL}, author = {Jordan Hines and Timothy Proctor}, doi = {10.1103/PhysRevLett.134.020602}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020602}, shortjournal = {Phys. Rev. Lett.}, title = {Pauli noise learning for mid-circuit measurements}, volume = {134}, year = {2025}, }
• (2025). Non-markovian feedback for optimized quantum error correction. PRL, 134(2), 020601. (www)

  @article{ , abstract = {Bosonic codes allow the encoding of a logical qubit in a single component device, utilizing the infinitely large Hilbert space of a harmonic oscillator. In particular, the Gottesman-Kitaev-Preskill code has recently been demonstrated to be correctable well beyond the break-even point of the best passive encoding in the same system. Current approaches to quantum error correction (QEC) for this system are based on protocols that use feedback, but the response is based only on the latest measurement outcome. In our work, we use the recently proposed feedback-GRAPE (gradient-ascent pulse engineering with feedback) method to train a recurrent neural network that provides a QEC scheme based on memory, responding in a non-Markovian way to the full history of previous measurement outcomes, optimizing all subsequent unitary operations. This approach significantly outperforms current strategies and paves the way for more powerful measurement-based QEC protocols.}, archive = {J_PRL}, author = {Matteo Puviani and Sangkha Borah and Remmy Zen and Jan Olle and Florian Marquardt}, doi = {10.1103/PhysRevLett.134.020601}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020601}, shortjournal = {Phys. Rev. Lett.}, title = {Non-markovian feedback for optimized quantum error correction}, volume = {134}, year = {2025}, }
• (2025). Semiclassical limit of resonance states in chaotic scattering. PRL, 134(2), 020404. (www)

  @article{ , abstract = {Resonance states in quantum chaotic scattering systems have a multifractal structure that depends on their decay rate. We show how classical dynamics describes this structure for all decay rates in the semiclassical limit. This result for chaotic scattering systems corresponds to the well-established quantum ergodicity for closed chaotic systems. Specifically, we generalize Ulam’s matrix approximation of the Perron-Frobenius operator, giving rise to conditionally invariant measures of various decay rates. There are many matrix approximations leading to the same decay rate and we conjecture a criterion for selecting the one relevant for resonance states. Numerically, we demonstrate that resonance states in the semiclassical limit converge to the selected measure. Example systems are a dielectric cavity, the three-disk scattering system, and open quantum maps.}, archive = {J_PRL}, author = {Roland Ketzmerick and Florian Lorenz and Jan Robert Schmidt}, doi = {10.1103/PhysRevLett.134.020404}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020404}, shortjournal = {Phys. Rev. Lett.}, title = {Semiclassical limit of resonance states in chaotic scattering}, volume = {134}, year = {2025}, }
• (2025). Protect measurement-induced phase transition from noise. PRL, 134(2), 020403. (www)

  @article{ , abstract = {Scrambling dynamics induced by random unitary gates can protect information from low-rate measurements, which underpins the phenomenon known as the measurement-induced phase transition (MIPT). However, typical decoherence noise disrupts the volume-law phase, complicating the observation of the MIPT on noisy intermediate-scale quantum devices. Here, we demonstrate that incorporating quantum-enhanced operations can effectively protect the MIPT from environmental noise, thereby enabling its detection in experiment. The transition is characterized by conditional entanglement entropy, which is associated with a statistical mechanics model wherein noise and quantum-enhanced operations act as competing external random fields. When the net external field is zero, a ferromagnetic-paramagnetic phase transition is expected, resulting in the MIPT. This zero-field condition also ensures an average apparatus-environment symmetry, making conditional entanglement entropy a valid probe of entanglement and establishing the transition as a genuine entanglement phase transition. Additionally, we provide numerical results that demonstrate the MIPT in a ( )-dimensional quantum circuit under dephasing noise. We also propose a method to estimate the noise rate, enabling the zero-field condition to be achieved experimentally and ensuring the feasibility of our protocol. Our result serves as a concrete example of the power of quantum enhancement in combating noise.}, archive = {J_PRL}, author = {Dongheng Qian and Jing Wang}, doi = {10.1103/PhysRevLett.134.020403}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020403}, shortjournal = {Phys. Rev. Lett.}, title = {Protect measurement-induced phase transition from noise}, volume = {134}, year = {2025}, }
• (2025). Thermal area law in long-range interacting systems. PRL, 134(2), 020402. (www)

  @article{ , abstract = {The area law of the bipartite information measure characterizes one of the most fundamental aspects of quantum many-body physics. In thermal equilibrium, the area law for the mutual information universally holds at arbitrary temperatures as long as the systems have short-range interactions. In systems with power-law decaying interactions, r − α ( r : distance), conditions for the thermal area law are elusive. In this Letter, we aim to clarify the optimal condition α > α c such that the thermal area law universally holds. A standard approach to considering the conditions is to focus on the magnitude of the boundary interaction between two subsystems. However, we find here that the thermal area law is more robust than this conventional argument suggests. We show the optimal threshold for the thermal area law by α c = ( D + 1 ) / 2 ( D : the spatial dimension of the lattice), assuming a power-law decay of the clustering for the bipartite correlations. Remarkably, this condition encompasses even the thermodynamically unstable regimes α < D . We verify this condition numerically, finding that it is qualitatively accurate for both integrable and nonintegrable systems. Unconditional proof of the thermal area law is possible by developing the power-law clustering theorem for α > D above a threshold temperature. Furthermore, the numerical calculation for the logarithmic negativity shows that the same criterion α > ( D + 1 ) / 2 applies to the thermal area law for quantum entanglement.}, archive = {J_PRL}, author = {Donghoon Kim and Tomotaka Kuwahara and Keiji Saito}, doi = {10.1103/PhysRevLett.134.020402}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020402}, shortjournal = {Phys. Rev. Lett.}, title = {Thermal area law in long-range interacting systems}, volume = {134}, year = {2025}, }
• (2025). Role of quantum coherence in kinetic uncertainty relations. PRL, 134(2), 020401. (www)

  @article{ , abstract = {The kinetic uncertainty relation (KUR) bounds the signal-to-noise ratio of stochastic currents in terms of the number of transitions per unit time, known as the dynamical activity. This bound was derived in a classical context and can be violated in the quantum regime due to coherent effects. However, the precise connection between KUR violations and quantum coherence has so far remained elusive, despite significant investigation. In this Letter, we solve this problem by deriving a modified bound that exactly pinpoints how, and when, coherence might lead to KUR violations. Our bound is sensitive to the specific kind of unraveling of the quantum master equation. It, therefore, allows one to compare quantum jumps and quantum diffusion, and understand, in each case, how quantum coherence affects fluctuations. We illustrate our result on a double quantum dot, where the electron current is monitored either by electron jump detection or with continuous diffusive charge measurement.}, archive = {J_PRL}, author = {Kacper Prech and Patrick P. Potts and Gabriel T. Landi}, doi = {10.1103/PhysRevLett.134.020401}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020401}, shortjournal = {Phys. Rev. Lett.}, title = {Role of quantum coherence in kinetic uncertainty relations}, volume = {134}, year = {2025}, }
• (2025). Limits to velocity of signal propagation in many-body systems: A quantum information perspective. PRL, 134(2), 020201. (www)

  @article{ , abstract = {The Lieb-Robinson bound (LRB) states that the range and strength of interactions between the constituents of a complex many-body system impose upper limits to how fast the signal can propagate. It manifests in a light conelike growth of correlation function connecting two distant subsystems. Here, we employ the techniques of quantum information to demonstrate that the LRB can be determined from local measurements performed on a single qubit that is connected to a many-body system. This formulation provides an operational recipe for estimating the LRB in complex systems, replacing the measurement of the correlation function with simple single-particle manipulations. We demonstrate the potency of this approach by deriving the upper limit to the speed of signal propagation in the spin chain.}, archive = {J_PRL}, author = {Piotr Wysocki and Jan Chwedeńczuk}, doi = {10.1103/PhysRevLett.134.020201}, journal = {Physical Review Letters}, month = {1}, number = {2}, pages = {020201}, shortjournal = {Phys. Rev. Lett.}, title = {Limits to velocity of signal propagation in many-body systems: A quantum information perspective}, volume = {134}, year = {2025}, }
• (2025). Passive defect driven morphogenesis in nematic membranes. PRL, 134(1), 018402. (www)

  @article{ , abstract = {Orientational order is a common feature of many biological and synthetic materials. Topological defects are discontinuities in this order that are often coupled to geometric features of the materials. Here, we study the equilibrium shapes of fluid membranes featuring a + 1 topological defect as a model for morphogenesis. We show, through simulation and analytic calculation, that the membrane can spontaneously deform toward a conical shape with a defect at its apex. We show that the relative stability of the deformation is controlled by the balance of the elastic parameters. When boundary constraints are introduced, we observe three distinct modes of deformation. These deformation modes take advantage of the way in which splay, twist, and bend distortions of the director field can be exchanged on a curved surface. Finally, we demonstrate inverted solutions. Our findings demonstrate a mechanism for passive defect driven morphogenesis as well as the fusion of + 1 / 2 topological defect pairs on deformable surfaces.}, archive = {J_PRL}, author = {D. J. G. Pearce and C. Thibault and Q. Chaboche and C. Blanch-Mercader}, doi = {10.1103/PhysRevLett.134.018402}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018402}, shortjournal = {Phys. Rev. Lett.}, title = {Passive defect driven morphogenesis in nematic membranes}, volume = {134}, year = {2025}, }
• (2025). Emergent rate-based dynamics in duplicate-free populations of spiking neurons. PRL, 134(1), 018401. (www)

  @article{ , abstract = {Can spiking neural networks (SNNs) approximate the dynamics of recurrent neural networks? Arguments in classical mean-field theory based on laws of large numbers provide a positive answer when each neuron in the network has many “duplicates”, i.e., other neurons with almost perfectly correlated inputs. Using a disordered network model that guarantees the absence of duplicates, we show that duplicate-free SNNs can converge to recurrent neural networks, thanks to the concentration of measure phenomenon. This result reveals a general mechanism underlying the emergence of rate-based dynamics in large SNNs.}, archive = {J_PRL}, author = {Valentin Schmutz and Johanni Brea and Wulfram Gerstner}, doi = {10.1103/PhysRevLett.134.018401}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018401}, shortjournal = {Phys. Rev. Lett.}, title = {Emergent rate-based dynamics in duplicate-free populations of spiking neurons}, volume = {134}, year = {2025}, }
• (2025). Coexistence of uniform and oscillatory states resulting from nonreciprocity and conservation laws. PRL, 134(1), 018303. (www)

  @article{ , abstract = {Employing a two-species Cahn-Hilliard model with nonreciprocal interactions, we show that the interplay of nonreciprocity and conservation laws results in the robust coexistence of uniform stationary and oscillatory phases as well as of uniform and crystalline phases. For nonequilibrium models with a spurious gradient dynamics structure, such coexistences between two or more nonequilibrium phases and resulting phase diagrams can, nevertheless, be predicted by a Maxwell double-tangent construction. This includes phases with sustained regular or irregular out-of-equilibrium dynamics as further corroborated by bifurcation studies and time simulations.}, archive = {J_PRL}, author = {Daniel Greve and Giorgio Lovato and Tobias Frohoff-Hülsmann and Uwe Thiele}, doi = {10.1103/PhysRevLett.134.018303}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018303}, shortjournal = {Phys. Rev. Lett.}, title = {Coexistence of uniform and oscillatory states resulting from nonreciprocity and conservation laws}, volume = {134}, year = {2025}, }
• (2025). Traveling strings of active dipolar colloids. PRL, 134(1), 018302. (www)

  @article{ , abstract = {We study an intriguing new type of self-assembled active colloidal polymer system in 3D. It is obtained from a suspension of Janus particles in an electric field that induces parallel dipoles in the particles as well as self-propulsion in the plane perpendicular to the field. At low volume fractions, in experiment, the particles self-assemble into 3D columns that are self-propelled in 2D. Explicit numerical simulations combining dipolar interactions and active self-propulsion find an activity dependent transition to a string phase by increasing dipole strength. We classify the collective dynamics of strings as a function of rotational and translational diffusion. Using an anisotropic version of the Rouse model of polymers with active driving, we analytically compute the strings’ collective dynamics and center of mass motion, which matches simulations and is consistent with experimental data. We also discover long range correlations of the fluctuations along the string contour that grow with the active persistence time, a purely active effect that disappears in the thermal limit.}, archive = {J_PRL}, author = {Xichen Chao and Katherine Skipper and C. Patrick Royall and Silke Henkes and Tanniemola B. Liverpool}, doi = {10.1103/PhysRevLett.134.018302}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018302}, shortjournal = {Phys. Rev. Lett.}, title = {Traveling strings of active dipolar colloids}, volume = {134}, year = {2025}, }
• (2025). Evolving motility of active droplets is captured by a self-repelling random walk model. PRL, 134(1), 018301. (www)

  @article{ , abstract = {In living matter, concentration gradients of nutrients carve the motility of microorganisms in a heterogeneous environment. Here, we use swimming droplets as a model system to study how swimmer-trail interactions guide locomotion. Combining experiments and theory, we show that our non-Markovian droplet model quantitatively captures droplet motility. The two fit parameters provide the first estimate of the effective temperature arising from hydrodynamic flows and the coupling strength of the propulsion force. This framework is general and explains memory effects, droplet hovering, and enhanced collective motion.}, archive = {J_PRL}, author = {Wenjun Chen and Adrien Izzet and Ruben Zakine and Eric Clément and Eric Vanden-Eijnden and Jasna Brujic}, doi = {10.1103/PhysRevLett.134.018301}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018301}, shortjournal = {Phys. Rev. Lett.}, title = {Evolving motility of active droplets is captured by a self-repelling random walk model}, volume = {134}, year = {2025}, }
• (2025). Encoding fast and fault-tolerant memories in bulk and nanoscale amorphous solids. PRL, 134(1), 018202. (www)

  @article{ , abstract = {We investigate the memory effects in cyclically deformed amorphous solids through computer simulations. Applying oscillatory shear deformations in all orthogonal directions during encoding creates fault-tolerant memories that are agnostic to the reading direction. Our extensive system size analysis shows that memory encoding is faster in small systems and becomes exceedingly challenging as systems approach the thermodynamic limit. To capitalize on the quickness of memory encoding in small system sizes, it is important to demonstrate that memory can be encoded in nanoscale objects, where open surfaces play a crucial role. We achieve this by going from 3D bulk to pseudo-1D nanorods. Using tension-compression cycles on these nanorods, we show that memory encoding and reading are also possible in the presence of free surfaces.}, archive = {J_PRL}, author = {Monoj Adhikari and Rishabh Sharma and Smarajit Karmakar}, doi = {10.1103/PhysRevLett.134.018202}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018202}, shortjournal = {Phys. Rev. Lett.}, title = {Encoding fast and fault-tolerant memories in bulk and nanoscale amorphous solids}, volume = {134}, year = {2025}, }
• (2025). Colloidal crystallization on cones. PRL, 134(1), 018201. (www)

  @article{ , abstract = {We explore experimentally how a conical surface frustrates the growth of colloidal crystals. Whereas crystals on a cylinder can form perfect commensurate bands, crystals on a cone tend to form tilt grain boundaries with misorientation angles set by the conical geometry. However, at small cone angles, where the surface deviates only slightly from that of a cylinder, crystals can form commensurate bands, the widths limited by the emergence of dislocations. The dislocations allow the crystal to continue growing beyond the limiting width. We relate these effects to the gradient in circumference on a cone, a consequence of the Gaussian curvature localized at the apex.}, archive = {J_PRL}, author = {Jessica H. Sun and Grace H. Zhang and Abigail Plummer and Caroline Martin and Nabila Tanjeem and David R. Nelson and Vinothan N. Manoharan}, doi = {10.1103/PhysRevLett.134.018201}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018201}, shortjournal = {Phys. Rev. Lett.}, title = {Colloidal crystallization on cones}, volume = {134}, year = {2025}, }
• (2025). X-ray diffraction reveals the consequences of strong deformation in thin smectic films: Dilation and chevron formation. PRL, 134(1), 018101. (www)

  @article{ , abstract = {Smectic liquid crystals can be viewed as model systems for lamellar structures for which there has been extensive theoretical development. We demonstrate that a nonlinear energy description is required with respect to the usual Landau–de Gennes elasticity in order to explain the observed layer spacing of highly curved smectic layers. Using x-ray diffraction we have quantitatively determined the dilation of bent layers distorted by antagonistic anchoring (as high as 1.8% of dilation for the most bent smectic layers) and accurately described it by the minimal nonlinear expression for energy. We observe a 1° tilt of planar layers that are connected to the curved layers. This value is consistent with simple energetic calculations, demonstrating how the bending energy impacts the overall structure of a thin distorted smectic film. Finally, we show that combined x-ray measurements and theoretical modeling allow for the quantitative determination of the number of curved smectic layers and of the resulting thickness of the dilated region with unprecedented precision.}, archive = {J_PRL}, author = {Jean de Dieu Niyonzima and Haifa Jeridi and Lamya Essaoui and Caterina Tosarelli and Alina Vlad and Alessandro Coati and Sebastien Royer and Isabelle Trimaille and Michel Goldmann and Bruno Gallas and Doru Constantin and David Babonneau and Yves Garreau and Bernard Croset and Samo Kralj and Randall D. Kamien and Emmanuelle Lacaze}, doi = {10.1103/PhysRevLett.134.018101}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018101}, shortjournal = {Phys. Rev. Lett.}, title = {X-ray diffraction reveals the consequences of strong deformation in thin smectic films: Dilation and chevron formation}, volume = {134}, year = {2025}, }
• (2025). Geometry of optimal control in chemical reaction networks in the adiabatic limit. PRL, 134(1), 018001. (www)

  @article{ , abstract = {Although optimal control (OC) has been studied in stochastic thermodynamics for systems with continuous state variables, less is known in systems with discrete state variables, such as chemical reaction networks (CRNs). Here, we develop a general theoretical framework to study OC of CRNs for changing the system from an initial distribution of states to a final distribution with minimum dissipation. We derive a “Kirchhoff’s law” for the probability current in the adiabatic limit, from which the optimal kinetic rates are determined analytically for any given probability trajectory allowed by local rate constraints. By using the optimal rates, we show that the total dissipation is determined by a L 2 -distance measure in the probability space and derive an analytical expression for the metric tensor that depends on the probability distribution, network topology, and capacity of each link. Minimizing the total dissipation leads to the geodesic trajectory in the probability space and the corresponding OC protocol is determined by the Kirchhoff’s law. To demonstrate our general approach, we use it to find a lower bound for the minimum dissipation that is tighter than existing bounds obtained with only global constraints in the adiabatic limit. We also apply it to simple networks, e.g., fully connected three-state CRNs with different local constraints and show that indirect pathway and nonfunctional transient state can play a crucial role in switching between different probability distributions efficiently. Future directions in studying OC in CRNs by using our general framework are discussed.}, archive = {J_PRL}, author = {Yikuan Zhang and Qi Ouyang and Yuhai Tu}, doi = {10.1103/PhysRevLett.134.018001}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {018001}, shortjournal = {Phys. Rev. Lett.}, title = {Geometry of optimal control in chemical reaction networks in the adiabatic limit}, volume = {134}, year = {2025}, }
• (2025). Universal statistics of competition in democratic elections. PRL, 134(1), 017401. (www)

  @article{ , abstract = {Elections for public offices in democratic nations are large-scale examples of collective decision-making. As a complex system with a multitude of interactions among agents, we can anticipate that universal macroscopic patterns could emerge independent of microscopic details. Despite the availability of empirical election data, such universality, valid at all scales, countries, and elections, has not yet been observed. In this Letter, we propose a parameter-free voting model and analytically show that the distribution of the victory margin is driven by that of the voter turnout, and a scaled measure depending on margin and turnout leads to a robust universality. This is demonstrated using empirical election data from 34 countries, spanning multiple decades and electoral scales. The deviations from the model predictions and universality indicate possible electoral malpractices. We argue that this universality is a stylized fact indicating the competitive nature of electoral outcomes.}, archive = {J_PRL}, author = {Ritam Pal and Aanjaneya Kumar and M. S. Santhanam}, doi = {10.1103/PhysRevLett.134.017401}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {017401}, shortjournal = {Phys. Rev. Lett.}, title = {Universal statistics of competition in democratic elections}, volume = {134}, year = {2025}, }
• (2025). Blending optimal control and biologically plausible learning for noise-robust physical neural networks. PRL, 134(1), 017301. (www)

  @article{ , abstract = {The rapidly increasing computational demands for artificial intelligence (AI) have spurred the exploration of computing principles beyond conventional digital computers. Physical neural networks (PNNs) offer efficient neuromorphic information processing by harnessing the innate computational power of physical processes; however, training their weight parameters is computationally expensive. We propose a training approach for substantially reducing this training cost. Our training approach merges an optimal control method for continuous-time dynamical systems with a biologically plausible training method—direct feedback alignment. In addition to the reduction of training time, this approach achieves robust processing even under measurement errors and noise without requiring detailed system information. The effectiveness was numerically and experimentally verified in an optoelectronic delay system. Our approach significantly extends the range of physical systems practically usable as PNNs.}, archive = {J_PRL}, author = {Satoshi Sunada and Tomoaki Niiyama and Kazutaka Kanno and Rin Nogami and André Röhm and Takato Awano and Atsushi Uchida}, doi = {10.1103/PhysRevLett.134.017301}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {017301}, shortjournal = {Phys. Rev. Lett.}, title = {Blending optimal control and biologically plausible learning for noise-robust physical neural networks}, volume = {134}, year = {2025}, }
• (2025). Long-lived population inversion in resonantly driven excitonic antiferromagnet. PRL, 134(1), 016901. (www)

  @article{ , abstract = {Van der Waals magnets are an emerging material family for investigating light-matter interactions and spin-correlated excitations. Here, we report the discovery of a photo-induced state with a lifetime of 17 ps in the van der Waals antiferromagnet NiPS 3 , which appears exclusively with resonant pumping at 1.476 eV in the antiferromagnetic state. The long-lived state comes with a negative photoconductivity, a characteristic optical response of population inversion. Our findings demonstrate a promising pathway to potentially achieve long-lived lasing at terahertz frequencies in reduced dimensions.}, archive = {J_PRL}, author = {Jacob A. Warshauer and Huyongqing Chen and Daniel Alejandro Bustamante Lopez and Qishuo Tan and Jing Tang and Xi Ling and Wanzheng Hu}, doi = {10.1103/PhysRevLett.134.016901}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016901}, shortjournal = {Phys. Rev. Lett.}, title = {Long-lived population inversion in resonantly driven excitonic antiferromagnet}, volume = {134}, year = {2025}, }
• (2025). Symmetry strategy for rapid discovery of abundant fractional quantum ferroelectrics. PRL, 134(1), 016801. (www)

  @article{ , abstract = {Traditional ferroelectrics are limited by Neumann’s principle, which confines exploration of ferroelectrics within polar point groups. Our recent work [Ji et al. , Nat. Commun. 15 , 135 (2024) ] proposes the concept of fractional quantum ferroelectricity (FQFE) that extends the playground of ferroelectricity to nonpolar point groups. Here, we apply group theory and introduce an efficient symmetry strategy to identify FQFE candidates. Integrated with a high-throughput screening scheme, we go through 171 527 materials and identify 221 potential FQFE candidates, which are already experimentally synthesized. In addition, we point out for the first time that the essence of FQFE is fractional atomic displacements with respect to lattice vectors, which can actually result in both fractional (type I) and integer (type II) quantized polarization, respectively. Through performing first-principles calculations, we verify the symmetry-predicted switchable FQFE properties in bulk and monolayer . Notably, exhibits an ultralow switching barrier of and interlocked in-plane/out-of-plane polarization, while displays large spontaneous polarization of . Our findings not only advance the understanding on FQFE, but also offer guidance for experimental exploration and design of novel ferroelectric materials.}, archive = {J_PRL}, author = {Guoliang Yu and Junyi Ji and Yingwei Chen and Changsong Xu and H. J. Xiang}, doi = {10.1103/PhysRevLett.134.016801}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016801}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry strategy for rapid discovery of abundant fractional quantum ferroelectrics}, volume = {134}, year = {2025}, }
• (2025). Observation of universal topological magnetoelectric switching in multiferroic ${\mathrm{GdMn}}_{2}{\mathrm{O}}_{5}$. PRL, 134(1), 016708. (www)

  @article{ , abstract = {Topological magnetoelectricity was recently revealed as an emergent topic, which opens a unique route to precisely control magnetoelectric functionality. Here we report the synchronous magnetic-electric-cycle operation of topological magnetoelectric switching in GdMn 2 O 5 . Compared with pure magnetic-cycle operation, this topological winding can be accessed in a much broader parameter space, i.e., orientation of the magnetic field is not limited to the magic angle and the effect can persist up to the Curie temperature. The fine-tuning of the free energy landscape is responsible for this topological behavior.}, archive = {J_PRL}, author = {Haowen Wang and Fan Wang and Ming Yang and Yuting Chang and Mengyi Shi and Liang Li and Jun-Ming Liu and Junfeng Wang and Shuai Dong and Chengliang Lu}, doi = {10.1103/PhysRevLett.134.016708}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016708}, shortjournal = {Phys. Rev. Lett.}, title = {Observation of universal topological magnetoelectric switching in multiferroic ${\mathrm{GdMn}}_{2}{\mathrm{O}}_{5}$}, volume = {134}, year = {2025}, }
• (2025). Unconventional scalings of quantum entropies in long-range heisenberg chains. PRL, 134(1), 016707. (www)

  @article{ , abstract = {In this work, building on state-of-the-art quantum Monte Carlo simulations, we perform systematic finite-size scaling of both entanglement and participation entropies for long-range Heisenberg chain with unfrustrated power-law decaying interactions. We find distinctive scaling behaviors for both quantum entropies in the various regimes explored by tuning the decay exponent α , thus capturing nontrivial features through logarithmic terms, beyond the case of linear Nambu-Goldstone modes. Our systematic analysis reveals that the quantum entanglement information, hidden in the scaling of the two studied entropies, can be obtained to the same level of order parameters and other usual finite-size observables of quantum many-body lattice models. The analysis and results obtained here can readily apply to more quantum criticalities in 1D and 2D systems.}, archive = {J_PRL}, author = {Jiarui Zhao and Nicolas Laflorencie and Zi Yang Meng}, doi = {10.1103/PhysRevLett.134.016707}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016707}, shortjournal = {Phys. Rev. Lett.}, title = {Unconventional scalings of quantum entropies in long-range heisenberg chains}, volume = {134}, year = {2025}, }
• (2025). Hall mass and transverse noether spin currents in noncollinear antiferromagnets. PRL, 134(1), 016706. (www)

  @article{ , abstract = {Noncollinear antiferromagnets (AFMs) have recently attracted attention in the emerging field of antiferromagnetic spintronics because of their various interesting properties. Because of the noncollinear magnetic order, the localized electron spins on different magnetic sublattices are not conserved even when spin-orbit coupling is neglected, making it difficult to understand the transport of spin angular momentum. Here we study the conserved Noether current due to spin-rotation symmetry of the local spins in noncollinear AFMs. Interestingly, we find that a Hall component of the spin current can be generically created by a longitudinal driving force associated with a propagating spin wave, inherently distinguishing noncollinear AFMs from collinear ones. We coin the corresponding Hall coefficient, an isotropic rank-four tensor, as the Hall (inverse) mass, which generally exists in noncollinear AFMs and their polycrystals. The resulting Hall spin current can be realized by spin pumping in a ferromagnet-noncollinear AFM bilayer structure as we demonstrate numerically, for which we also give the criteria of ideal boundary conditions. Our results shed light on the potential of noncollinear AFMs in manipulating the polarization and flow of spin currents in general spintronic devices.}, archive = {J_PRL}, author = {Luke Wernert and Bastián Pradenas and Oleg Tchernyshyov and Hua Chen}, doi = {10.1103/PhysRevLett.134.016706}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016706}, shortjournal = {Phys. Rev. Lett.}, title = {Hall mass and transverse noether spin currents in noncollinear antiferromagnets}, volume = {134}, year = {2025}, }
• (2025). Ultrafast pseudomagnetic fields from electron-nuclear quantum geometry. PRL, 134(1), 016705. (www)

  @article{ , abstract = {Recent experiments demonstrate precise control over coherently excited circular phonon modes using high-intensity terahertz lasers, opening new pathways towards dynamical, ultrafast design of magnetism in functional materials. While the phonon Zeeman effect enables a theoretical description of phonon-induced magnetism, it lacks efficient angular momentum transfer from the phonon to the electron sector. In this work, we put forward a coupling mechanism based on electron-nuclear quantum geometry, with the inverse Faraday effect as a limiting case. This effect is rooted in the phase accumulation of the electronic wave function under a circular evolution of nuclear coordinates. An excitation pulse then induces a transient level splitting between electronic orbitals that carry angular momentum. First-principles simulations on demonstrate that in parts of the Brillouin zone, this splitting between orbitals carrying angular momentum can easily reach 50 meV.}, archive = {J_PRL}, author = {Lennart Klebl and Arne Schobert and Martin Eckstein and Giorgio Sangiovanni and Alexander V. Balatsky and Tim O. Wehling}, doi = {10.1103/PhysRevLett.134.016705}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016705}, shortjournal = {Phys. Rev. Lett.}, title = {Ultrafast pseudomagnetic fields from electron-nuclear quantum geometry}, volume = {134}, year = {2025}, }
• (2025). Magnetic X-ray imaging using a single polarization and multimodal ptychography. PRL, 134(1), 016704. (www)

  @article{ , abstract = {Polarized x-rays allow for imaging birefringent or dichroic properties of materials with nanometric resolution. To disentangle these properties from the electronic density, either a polarization analyzer or several measurements with different polarizations (typically two or more) are needed. Here we demonstrate that ptychography can disentangle these from a single polarization measurement by using a multimodal analysis. This new method provides an alternative to obtain polarization-resolved images of a sample when manipulating the incident polarization is not possible or sufficient.}, archive = {J_PRL}, author = {Marisel Di Pietro Martínez and Alexis Wartelle and Nicolas Mille and Stefan Stanescu and Rachid Belkhou and Farid Fettar and Vincent Favre-Nicolin and Guillaume Beutier}, doi = {10.1103/PhysRevLett.134.016704}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016704}, shortjournal = {Phys. Rev. Lett.}, title = {Magnetic X-ray imaging using a single polarization and multimodal ptychography}, volume = {134}, year = {2025}, }
• (2025). Symmetry-based phenomenological model for magnon transport in a multiferroic. PRL, 134(1), 016703. (www)

  @article{ , abstract = {Magnons—carriers of spin information—can be controlled by electric fields in the multiferroic (BFO), a milestone that brings magnons closer to application in future devices. The origin of magnon-spin currents in BFO, however, is not fully understood due to BFO’s complicated magnetic texture. In this Letter, we present a phenomenological model to elucidate the existence of magnon spin currents in generalized multiferroics by examining the symmetries inherent to their magnetic and polar structures. This model is grounded in experimental data obtained from BFO and its derivatives, which informs the symmetry operations and resultant magnon behavior. By doing so, we address the issue of symmetry-allowed, switchable magnon spin transport in multiferroics, thereby establishing a critical framework for comprehending magnon transport within complex magnetic textures.}, archive = {J_PRL}, author = {Isaac A. Harris and Sajid Husain and Peter Meisenheimer and Maya Ramesh and Hyeon Woo Park and Lucas Caretta and Darrell G. Schlom and Zhi Yao and Lane W. Martin and Jorge Íñiguez-González and Se Kwon Kim and Ramamoorthy Ramesh}, doi = {10.1103/PhysRevLett.134.016703}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016703}, shortjournal = {Phys. Rev. Lett.}, title = {Symmetry-based phenomenological model for magnon transport in a multiferroic}, volume = {134}, year = {2025}, }
• (2025). Room-temperature perovskite ferromagnetic insulator via three-dimensional tensile strain. PRL, 134(1), 016702. (www)

  @article{ , abstract = {Ferromagnetic insulators are receiving ever-increasing research activities driven not only by the unique advantage of low power loss during spin-wave-based information processing but also by the potential to construct next-generation spintronic devices. However, either the exceedingly rare candidates or the low Curie temperature far below room temperature greatly hinder their practical application. Here, through the modulation of a novel three-dimensional (3D) tensile strain, a room-temperature ferromagnetic insulating state with a Curie temperature as high as 594 K is achieved in self-assembled nanocomposite thin films. Atomically resolved electron microscopy quantifications identify the 3D strain state of the thin film, where the out-of-plane and in-plane tensile strains are attributed to the interphase mismatch between the and MgO building blocks and epitaxial constraint, respectively. Combined with the assessment of electronic states and theoretical analysis, we correlate the strain state with the resulting ferromagnetic insulating property and clarify the underlying mechanisms, by which the emergent strain states break the degeneracy of crystal-field splitting and tailor the on-site Coulomb interactions and spin configuration. These findings underscore the efficacy of a three-dimensional strain strategy in engineering the long-desired high-temperature ferromagnetic insulators via the manipulation of strong spin-lattice coupling, providing a promising approach for the exploitation of exotic functionalities in correlated oxides.}, archive = {J_PRL}, author = {Tianyu Li and Yali Yang and Shiqing Deng and Fangyuan Zhu and Tianfu Zhang and Yu Chen and Huanhua Wang and Feixiang Long and Xiaolong Li and Jia-Ou Wang and Tao Zhu and Mingxue Tang and Jiangang He and Oswaldo Diéguez and Er-Jia Guo and Jun Chen}, doi = {10.1103/PhysRevLett.134.016702}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016702}, shortjournal = {Phys. Rev. Lett.}, title = {Room-temperature perovskite ferromagnetic insulator via three-dimensional tensile strain}, volume = {134}, year = {2025}, }
• (2025). Light-induced torque in ferromagnetic metals via orbital angular momentum generated by photon helicity. PRL, 134(1), 016701. (www)

  @article{ , abstract = {We investigated photon-helicity–induced magnetization precession in Co 1 − x Pt x alloy thin films. In addition to field-like torque, attributable to magnetic field generation owing to the “inverse Faraday effect,” we observed nontrivial and large damping-like torque that has never been discussed for single ferromagnetic layer. The composition dependence of these two torques is effectively elucidated by a model that considers mutual coupling via spin-orbit interaction between magnetization and the electronic orbital angular momentum generated by photon helicity. This Letter significantly enhances our understanding of the physics relevant to the interplay of photon helicity and magnetization in magnetic metals.}, archive = {J_PRL}, author = {Koki Nukui and Satoshi Iihama and Kazuaki Ishibashi and Shogo Yamashita and Akimasa Sakuma and Philippe Scheid and Grégory Malinowski and Michel Hehn and Stéphane Mangin and Shigemi Mizukami}, doi = {10.1103/PhysRevLett.134.016701}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016701}, shortjournal = {Phys. Rev. Lett.}, title = {Light-induced torque in ferromagnetic metals via orbital angular momentum generated by photon helicity}, volume = {134}, year = {2025}, }
• (2025). Probing berry curvature in magnetic topological insulators through resonant infrared magnetic circular dichroism. PRL, 134(1), 016601. (www)

  @article{ , abstract = {Probing the quantum geometry and topology in condensed matter systems has relied heavily on static electronic transport experiments in magnetic fields. Yet, contact-free optical measurements have rarely been explored. Here, we report the observation of resonant magnetic circular dichroism (MCD) in the infrared range in thin film exhibiting a spectral intensity that correlates with the anomalous Hall effect. Both phenomena emerge with a field-driven phase transition from an antiferromagnet to a canted ferromagnet. By theoretically relating the MCD to the anomalous Hall effect via Berry curvature for a metallic state, we show that this transition accompanies an abrupt onset of Berry curvature, signaling a topological phase transition from a topological insulator to a doped Chern insulator. Our density functional theory calculation suggests the MCD signal mainly originates from an optical transition at the Brillouin zone edge, hinting at a potential new source of Berry curvature away from the commonly considered point. Our findings demonstrate a novel experimental approach for detecting Berry curvature through spectroscopy of the interband MCD, generally applicable to magnetic materials.}, archive = {J_PRL}, author = {Seul-Ki Bac and Florian Le Mardelé and Jiashu Wang and Mykhaylo Ozerov and Kota Yoshimura and Ivan Mohelský and Xingdan Sun and Benjamin A. Piot and Stefan Wimmer and Andreas Ney and Tatyana Orlova and Maksym Zhukovskyi and Günther Bauer and Gunther Springholz and Xinyu Liu and Milan Orlita and Kyungwha Park and Yi-Ting Hsu and Badih A. Assaf}, doi = {10.1103/PhysRevLett.134.016601}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016601}, shortjournal = {Phys. Rev. Lett.}, title = {Probing berry curvature in magnetic topological insulators through resonant infrared magnetic circular dichroism}, volume = {134}, year = {2025}, }
• (2025). Extended metal-insulator crossover with strong antiferromagnetic spin correlation in half-filled 3D hubbard model. PRL, 134(1), 016503. (www)

  @article{ , abstract = {The Hubbard model at temperatures above the Néel transition, despite being a paramagnet, can exhibit rich physics due to the interplay of Fermi surface, on-site interaction and thermal fluctuations. Nevertheless, the understanding of the crossover physics remains only at a qualitative level, because of the intrinsically smooth behavior. Employing an improved variant of the numerically exact auxiliary-field quantum Monte Carlo algorithm equipped with numerical analytic continuation, we obtain a broad variety of thermodynamic and dynamical properties of the three-dimensional Hubbard model at half filling, quantitatively determine the crossover boundaries, and observe that the metal-insulator crossover regime, in which antiferromagnetic spin correlations appear strongest, exists over an extended regime in between the Fermi liquid for small and the Mott insulator for large . In particular, the location of the most rapid suppression of double occupancy as increases, is found to fully reside in the metallic Fermi liquid regime, in contrast to the conventional intuition that it is a representative feature for entering the Mott insulator. Beside providing a reliable methodology for numerical study of crossover physics, our work can also serve as a timely and important guideline for the most recent optical lattice experiments.}, archive = {J_PRL}, author = {Yu-Feng Song and Youjin Deng and Yuan-Yao He}, doi = {10.1103/PhysRevLett.134.016503}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016503}, shortjournal = {Phys. Rev. Lett.}, title = {Extended metal-insulator crossover with strong antiferromagnetic spin correlation in half-filled 3D hubbard model}, volume = {134}, year = {2025}, }
• (2025). Universal waterfall feature in cuprate superconductors: Evidence of a momentum-driven crossover. PRL, 134(1), 016502. (www)

  @article{ , abstract = {We study two related universal anomalies of the spectral function of cuprates, so-called waterfall and high-energy kink features, by a combined cellular dynamical mean-field theory and angle-resolved photoemission study for the oxychloride (Na-CCOC). Tracing their origin back to an interplay of spin-polaron and local-correlation effects both in undoped and hole-doped (Na-)CCOC, we establish them as a universal crossover between regions differing in the momentum dependence of the coupling and not necessarily in the related quasiparticles’ energies. The proposed scenario extends to doping levels coinciding with the cuprate’s superconducting dome and motivates further investigations of the fate of spin polarons in the superconducting phase.}, archive = {J_PRL}, author = {Benjamin Bacq-Labreuil and Chafic Fawaz and Yuichi Okazaki and Yukiko Obata and Hervé Cercellier and Patrick Le Fèvre and François Bertran and David Santos-Cottin and Hajime Yamamoto and Ikuya Yamada and Masaki Azuma and Koji Horiba and Hiroshi Kumigashira and Matteo d’Astuto and Silke Biermann and Benjamin Lenz}, doi = {10.1103/PhysRevLett.134.016502}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016502}, shortjournal = {Phys. Rev. Lett.}, title = {Universal waterfall feature in cuprate superconductors: Evidence of a momentum-driven crossover}, volume = {134}, year = {2025}, }
• (2025). Spin correlations in the parent phase of ${\mathrm{Li}}_{1\ensuremath{-}x}{\mathrm{Fe}}_{x}\mathrm{ODFeSe}$. PRL, 134(1), 016501. (www)

  @article{ , abstract = {Elucidating spin correlations in the parent compounds of high-temperature superconductors is crucial for understanding superconductivity. We used neutron scattering to study spin correlations in Li 1 − x Fe x ODFeSe , an insulating material with reduced electron carriers compared to its superconducting counterpart ( T c = 41 K ), serving as the undoped parent compound. Our findings show a reduced total fluctuating moment in this insulator relative to FeSe and 122 iron pnictides, likely due to increased interlayer distances from intercalation, which enhance fluctuations and reduce the intensity of spin excitations. Moreover, we observed a V-shaped spin wavelike excitation dispersion, contrasting with the twisted hourglass pattern in the superconducting counterpart. Electron doping shifts spin excitation from ( π , 0 ) point to an incommensurate position towards ( π , π ) direction below 65 meV. This transition from V-shaped to hourglasslike dispersion, akin to behaviors in hole-doped cuprates, suggests a potential shared mechanism in magnetism and superconductivity across these diverse systems.}, archive = {J_PRL}, author = {Hongliang Wo and Bingying Pan and Die Hu and Yu Feng and A. D. Christianson and Jun Zhao}, doi = {10.1103/PhysRevLett.134.016501}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016501}, shortjournal = {Phys. Rev. Lett.}, title = {Spin correlations in the parent phase of ${\mathrm{Li}}_{1\ensuremath{-}x}{\mathrm{Fe}}_{x}\mathrm{ODFeSe}$}, volume = {134}, year = {2025}, }
• (2025). Effect of overdamped phonons on the fundamental band gap of perovskites. PRL, 134(1), 016403. (www)

  @article{ , abstract = {Anharmonic atomic motions can strongly influence the optoelectronic properties of materials but how these effects are connected to the underlying phonon band structure is not understood well. We investigate how the electronic band gap is influenced by overdamped phonons, which occur in an intriguing regime of phonon-phonon interactions where vibrational lifetimes fall below one oscillation period. We contrast the anharmonic halide perovskite , known to exhibit overdamped phonons in its cubic phase, with the anharmonic oxide perovskite where the phonons are underdamped at sufficiently high temperatures. Our results show that overdamped phonons strongly impact the band gap and cause slow dynamic fluctuations of electronic levels that have been implicated in the unique optoelectronic properties of halide perovskites. This finding is enabled by developing augmented stochastic Monte Carlo methods accounting for phonon renormalization and imaginary modes that are typically neglected. Our work provides guidelines for capturing anharmonic effects in theoretical calculations of materials.}, archive = {J_PRL}, author = {Xiangzhou Zhu and David A. Egger}, doi = {10.1103/PhysRevLett.134.016403}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016403}, shortjournal = {Phys. Rev. Lett.}, title = {Effect of overdamped phonons on the fundamental band gap of perovskites}, volume = {134}, year = {2025}, }
• (2025). Accurate correlation potentials from the self-consistent random phase approximation. PRL, 134(1), 016402. (www)

  @article{ , abstract = {Density-functional theory (DFT) within the Kohn-Sham (KS) formalism is the most widely used approach to treat electronic structures of molecules and solids in physics, chemistry, and materials science, and the development of more accurate functionals for the KS exchange and correlation energy has been a major research focus for decades. The corresponding exchange and correlation potentials, on the other hand, have attracted little attention. Those cases for which reference potentials are available showed that in particular correlation potentials from common approximate density functionals are of poor quality and sometimes have little in common with the exact potentials. This hampers the further development of KS-DFT. Here, we show that highly accurate correlation potentials can be obtained within the random phase approximation (RPA). In conjunction with the exact exchange potential, which, like the RPA correlation potential, is accessible within the optimized effective potential method, highly accurate exchange-correlation potentials are available and provide a basis for the further development of DFT. We present a numerically stable approach for efficiently carrying out self-consistent RPA calculations and combine it with a KS inversion method to obtain reference correlation potentials from highly accurate electron densities from coupled cluster calculations. Accurate exchange-correlation potentials have to yield KS eigenvalues for the highest occupied molecular orbital that are close to the negative of the ionization potential. This is indeed the case, the RPA highest occupied molecular orbital eigenvalues yield ionization potentials that can compete with ionization potentials.}, archive = {J_PRL}, author = {Egor Trushin and Steffen Fauser and Andreas Mölkner and Jannis Erhard and Andreas Görling}, doi = {10.1103/PhysRevLett.134.016402}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016402}, shortjournal = {Phys. Rev. Lett.}, title = {Accurate correlation potentials from the self-consistent random phase approximation}, volume = {134}, year = {2025}, }
• (2025). Piezoresistivity as a fingerprint of ferroaxial transitions. PRL, 134(1), 016401. (www)

  @article{ , abstract = {Recent progress in the understanding of the collective behavior of electrons and ions has revealed new types of ferroic orders beyond ferroelectricity and ferromagnetism, such as the ferroaxial state. The latter retains only rotational symmetry around a single axis and reflection symmetry with respect to a single mirror plane, both of which are set by an emergent electric toroidal dipole moment. Because of this unusual symmetry-breaking pattern, it has been challenging to directly measure the ferroaxial order parameter, despite the increasing attention this state has drawn. Here, we show that off-diagonal components of the piezoresistivity tensor (i.e., the linear change in resistivity under strain) transform the same way as the ferroaxial moments, providing a direct probe of such order parameters. We identify two new proper ferroaxial materials through a materials database search, and use first-principles calculations to evaluate the piezoconductivity of the double-perovskite , revealing its connection to ferroaxial order and to octahedral rotation modes.}, archive = {J_PRL}, author = {Ezra Day-Roberts and Rafael M. Fernandes and Turan Birol}, doi = {10.1103/PhysRevLett.134.016401}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016401}, shortjournal = {Phys. Rev. Lett.}, title = {Piezoresistivity as a fingerprint of ferroaxial transitions}, volume = {134}, year = {2025}, }
• (2025). Stability and mobility of disconnections in solute atmospheres: Insights from interfacial defect diagrams. PRL, 134(1), 016202. (www)

  @article{ , abstract = {This Letter explores the stability of disconnections (step-dislocation defects) at grain boundaries in binary alloys. We introduce interfacial defect diagrams, derived from atomistic simulations and segregation theory, to predict the stability of disconnections in the temperature-solute concentration phase space and relate it to governing segregation mechanisms. These diagrams reveal multiple stability regimes influenced by solute-induced clustering and pinning effects impacting the thermal migration of disconnections and offering insights into their thermodynamics and kinetic properties.}, archive = {J_PRL}, author = {Chongze Hu and Douglas L. Medlin and Rémi Dingreville}, doi = {10.1103/PhysRevLett.134.016202}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016202}, shortjournal = {Phys. Rev. Lett.}, title = {Stability and mobility of disconnections in solute atmospheres: Insights from interfacial defect diagrams}, volume = {134}, year = {2025}, }
• (2025). Cooling and heating nuclear spins by strongly localized electrons. PRL, 134(1), 016201. (www)

  @article{ , abstract = {The concept of nuclear spin temperature has been a cornerstone of the theory of dynamic nuclear spin polarization by electrons in various semiconductor structures for decades. Still, it is not always applicable to strongly localized electrons due to their long spin correlation times. This motivated the use of the oversimplified central spin model for the description of the nuclear spin dynamics in quantum dots. Here, we present a microscopic theory that bridges the gap between these two approaches by describing the nuclear spin thermodynamics for systems with long electron spin correlation times. Importantly, our theory predicts that efficient nuclear spin cooling by strongly localized electrons requires an external magnetic field by far exceeding the local field of nuclear spin-spin interaction, and that the time of the nuclear spin heating by unpolarized electrons may change by several orders of magnitude depending on the magnetic field.}, archive = {J_PRL}, author = {D. S. Smirnov and K. V. Kavokin}, doi = {10.1103/PhysRevLett.134.016201}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {016201}, shortjournal = {Phys. Rev. Lett.}, title = {Cooling and heating nuclear spins by strongly localized electrons}, volume = {134}, year = {2025}, }
• (2025). Narrowband terahertz emission from a plasma oscillator imbedded in a plasma density gradient. PRL, 134(1), 015001. (www)

  @article{ , abstract = {A novel method is presented for generating radiation using the beat wave of a bifrequency laser pulse to excite plasma oscillations in a plasma slab that has a density gradient. The plasma wave is localized where it is excited resonantly and becomes a plasma oscillator that produces a beam of radially polarized, terahertz radiation. Particle-in-cell simulations and a theoretical analysis are used to demonstrate its main characteristics, such as its narrow bandwidth. The radiator should have useful applications including driving terahertz-band particle accelerators and for pump-probe experiments.}, archive = {J_PRL}, author = {Manoj Kumar and Bernhard Ersfeld and Jaeho Lee and Dohyun Park and Seungyun Kim and Inhyuk Nam and Minseok Kim and Seongjin Jeon and Dino A. Jaroszynski and Hyyong Suk and Min Sup Hur}, doi = {10.1103/PhysRevLett.134.015001}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {015001}, shortjournal = {Phys. Rev. Lett.}, title = {Narrowband terahertz emission from a plasma oscillator imbedded in a plasma density gradient}, volume = {134}, year = {2025}, }
• (2025). Sedimentation dynamics of bodies with two planes of symmetry. PRL, 134(1), 014002. (www)

  @article{ , abstract = {We show that bodies with two planes of symmetry can display a range of behaviors even without inertia. Any such body supports a conserved quantity in its dynamics, and is either a settler, a drifter or a flutterer, depending only on its shape. At large time, settlers and drifters, respectively, fall vertically and obliquely, while flutterers rotate forever while executing intricate patterns. The dynamics of flutterers decouples into a periodic and a Floquet part with different timescales, giving periodicity or quasiperiodicity. We design a set of bodies and use the boundary integral method to show that settlers, drifters, and flutterers, all lie in this set.}, archive = {J_PRL}, author = {Harshit Joshi and Rama Govindarajan}, doi = {10.1103/PhysRevLett.134.014002}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {014002}, shortjournal = {Phys. Rev. Lett.}, title = {Sedimentation dynamics of bodies with two planes of symmetry}, volume = {134}, year = {2025}, }
• (2025). Phase-locking parametric instability coupling longitudinal and transverse waves on rivulets in a hele-shaw cell. PRL, 134(1), 014001. (www)

  @article{ , abstract = {We report an instability exhibited by a fluid system when coupling two distinct types of waves, both linearly damped. While none of them is unstable on its own, they amplify one another, resulting in a previously unreported convective instability. An external excitation is used to induce a parametric cross-coupling between longitudinal and transverse deformations of a liquid bridge between two vertical glass plates. Coherent amplification results in waves satisfying a synchronization condition, which selects a precise wavelength. We derive a model for this instability using depth-averaged Navier-Stokes equations, showing the physical origin of the coamplification, and confirm its relevance experimentally. Our findings open new perspectives in the study of parametrically controlled pattern formation, and invites the search for analogous parametric cross-coupling instabilities in other systems exhibiting distinct wave types, from plasma to elastic media.}, archive = {J_PRL}, author = {Grégoire Le Lay and Adrian Daerr}, doi = {10.1103/PhysRevLett.134.014001}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {014001}, shortjournal = {Phys. Rev. Lett.}, title = {Phase-locking parametric instability coupling longitudinal and transverse waves on rivulets in a hele-shaw cell}, volume = {134}, year = {2025}, }
• (2025). Janus bound states in the continuum with asymmetric topological charges. PRL, 134(1), 013805. (www)

  @article{ , abstract = {We propose a novel topological defect called Janus bound states in the continuum (BICs), featuring asymmetric topological charges in upward and downward radiation channels. Our approach involves a photonic crystal slab (PCS) that initially exhibits both out-of-plane and in-plane mirror symmetry, and this PCS possesses one BIC at the point and two BICs off the point. By introducing certain perturbations that break the out-of-plane mirror symmetry, the two off- BICs decompose into four circularly polarized states ( points) with identical topological charges (each with half the topological charge of the original BIC) while the at- BIC is preserved. Then, we selectively manipulate the four points associated with the downward radiation channel to converge at the at- BIC, forming a Janus BIC with distinct topological charges for upward and downward radiation. By further introducing in-plane mirror symmetry perturbation, we can bring two of the points with the same handedness and identical topological charges for upward radiation to merge into the Janus BIC. This process results in a Janus chiral BIC which exhibits large intrinsic chirality and an infinite factor. Janus BICs can induce distinct Pancharatnam-Berry phase singularities in momentum space for different incident channels, providing a new approach to control orbital angular momentum. Janus chiral BICs hold promise in enhancing direction-dependent and spin-dependent asymmetric light-matter interaction, opening new pathways for improving chirality-dependent operation for on-chip devices.}, archive = {J_PRL}, author = {Meng Kang and Meng Xiao and C. T. Chan}, doi = {10.1103/PhysRevLett.134.013805}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013805}, shortjournal = {Phys. Rev. Lett.}, title = {Janus bound states in the continuum with asymmetric topological charges}, volume = {134}, year = {2025}, }
• (2025). Direct detection of down-converted photons spontaneously produced at a single josephson junction. PRL, 134(1), 013804. (www)

  @article{ , abstract = {We study spontaneous photon decay into multiple photons triggered by strong nonlinearities in an experimental simulator of a bosonic quantum impurity model. Previously, spectroscopic signatures of photon conversion were reported and evidenced as resonances in the many-body spectrum of these systems. Here, we report on the observation of multimode fluorescence of a small Josephson junction embedded in a high impedance superconducting transmission line. Measurement of the down-converted photons is achieved using state-of-the-art broadband parametric amplifiers. Photon triplet emission is explicitly demonstrated at a given frequency as the counterpart of inelastic photon decay at 3 × the emission frequency. These results open exciting prospects for the burgeoning field of many-body quantum optics and offer a direct signature of the ultrastrong light-matter coupling.}, archive = {J_PRL}, author = {Dorian Fraudet and Izak Snyman and Denis M. Basko and Sébastien Léger and Théo Sépulcre and Arpit Ranadive and Gwenael Le Gal and Alba Torras-Coloma and Wiebke Guichard and Serge Florens and Nicolas Roch}, doi = {10.1103/PhysRevLett.134.013804}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013804}, shortjournal = {Phys. Rev. Lett.}, title = {Direct detection of down-converted photons spontaneously produced at a single josephson junction}, volume = {134}, year = {2025}, }
• (2025). Perturbation theory for resonant states near a bound state in the continuum. PRL, 134(1), 013803. (www)

  @article{ , abstract = {In this work, we develop a perturbation theory to analyze resonant states near a bound state in the continuum (BIC) in photonic crystal slabs. The theory allows us to rigorously determine the asymptotic behavior of Q -factor and the far-field polarization. We show that the resonant states close to a BIC can be nearly circularly polarized if the scattering matrix satisfies a certain condition. Moreover, our theory offers a novel perspective on super-BICs and provides a clear and precise condition to efficiently identify them in both symmetric and asymmetric structures without requiring a merging process. For practical applications, we find a super-BIC in a square lattice of rods on a dielectric substrate. Our theory addresses the non-Hermitian nature of the system, can be generalized to treat other structures that support BICs, and has potential applications in resonance and chiral optics.}, archive = {J_PRL}, author = {Nan Zhang and Ya Yan Lu}, doi = {10.1103/PhysRevLett.134.013803}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013803}, shortjournal = {Phys. Rev. Lett.}, title = {Perturbation theory for resonant states near a bound state in the continuum}, volume = {134}, year = {2025}, }
• (2025). Dual-color coherent perfect absorber. PRL, 134(1), 013802. (www)

  @article{ , abstract = {Perfect absorption of light critically affects light-matter interaction for various applications. Coherent perfect absorbers (CPAs) gain the unique capability of controlling light with light in a linear fashion. Multicolor CPAs [S. Longhi, Time-reversed optical parametric oscillation, Phys. Rev. Lett. 107 , 033901 (2011) ] are highly desirable for broadband and nonlinear light-to-light coherent control but the experimental demonstration has still remained elusive. Here, for the first time, we experimentally observe a dual-color version of a CPA (DC-CPA) through a second harmonic generation in a single whispering-gallery-mode microcavity. The DC-CPA enables simultaneous perfect absorption of both the incoming fundamental wave and its second harmonic. Similar to its linear counterpart, coherent control in the DC-CPA can also be realized by tuning the relative phase and intensity between the two-colored waves through nonlinear interference instead of the linear one. This scheme breaks the linear boundary of the traditional CPA into a multifrequency domain and paves the way toward all-optical signal processing and quantum information.}, archive = {J_PRL}, author = {Boyi Xue and Jintian Lin and Jiankun Hou and Yicheng Zhu and Ruixin Ma and Xianfeng Chen and Ya Cheng and Li Ge and Wenjie Wan}, doi = {10.1103/PhysRevLett.134.013802}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013802}, shortjournal = {Phys. Rev. Lett.}, title = {Dual-color coherent perfect absorber}, volume = {134}, year = {2025}, }
• (2025). Topological spin states in 3D coupled electromagnetic fields. PRL, 134(1), 013801. (www)

  @article{ , abstract = {Topological defects are nonsmooth field configurations with singularities that widely exist in physics and multidisciplinary areas. Here, we introduce near-field polarization evolution and the resulting topological spin states in a system of silicon-based coupled waveguides. The topological spin structures originate from 3D evanescent field coupling that transforms the trivial transverse spin into the topological spin states in a 2D plane. Moreover, we show that the periodic coupling of higher-order electromagnetic modes can produce intriguing spin defect (singularity) arrays, including those with alternately topological charges of . These findings may further expand the family of electromagnetic topological structures, and open new avenues to engineer photon emission and light-matter interactions on integrated photonic platforms.}, archive = {J_PRL}, author = {Liang Fang and Yuanjiang Xiang and Qinjun Chen and Shuangchun Wen}, doi = {10.1103/PhysRevLett.134.013801}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013801}, shortjournal = {Phys. Rev. Lett.}, title = {Topological spin states in 3D coupled electromagnetic fields}, volume = {134}, year = {2025}, }
• (2025). Chiral interaction induced near-perfect photon blockade. PRL, 134(1), 013602. (www)

  @article{ , abstract = {Based on the scattering matrix method, we theoretically demonstrate that the chiral interaction can induce the almost perfect photon blockade (PB) in the waveguide-cavity quantum electrodynamics system. The mechanism relies on the multiphoton path’s interference within the waveguide, which is clearly shown by the analytic parameter regime for . When cavities are introduced into the system, there are optimal parameter points accordingly for the almost perfect PB, where the required lowest chirality decreases exponentially with increasing , and these optimal points are robust against disorder in the system’s frequencies. Under resonant driving and fixed chirality conditions, the output light depends solely on the parity of ( ), with a coherent state emerging for even numbers of cavities and a single-photon state for odd numbers. Our Letter offers an alternative route for achieving almost perfect PB effects with high single-photon transmission by employing the chirality of system, with potential application in the on-chip single-photon source with integrability.}, archive = {J_PRL}, author = {Zhi-Guang Lu and Ying Wu and Xin-You Lü}, doi = {10.1103/PhysRevLett.134.013602}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013602}, shortjournal = {Phys. Rev. Lett.}, title = {Chiral interaction induced near-perfect photon blockade}, volume = {134}, year = {2025}, }
• (2025). Nonlinear optics using intense optical coherent state superpositions. PRL, 134(1), 013601. (www)

  @article{ , abstract = {Superpositions of coherent light states are vital for quantum technologies. However, restrictions in existing state preparation and characterization schemes, in combination with decoherence effects, prevent their intensity enhancement and implementation in nonlinear optics. Here, by developing a decoherence-free approach, we generate intense femtosecond-duration infrared coherent state superpositions (CSSs) with a mean photon number orders of magnitude higher than the existing CSS sources. We utilize them in nonlinear optics to drive the second harmonic generation process in an optical crystal. We experimentally and theoretically show that the nonclassical nature of the intense infrared CSS is imprinted in the second-order autocorrelation traces. Additionally, theoretical analysis shows that the quantum features of the infrared CSS are also present in the generated second harmonic. The findings introduce the optical CSS into the realm of nonlinear quantum optics, opening up new paths in quantum information science and quantum light engineering by creating nonclassical light states in various spectral regions via nonlinear up-conversion processes.}, archive = {J_PRL}, author = {Th. Lamprou and J. Rivera-Dean and P. Stammer and M. Lewenstein and P. Tzallas}, doi = {10.1103/PhysRevLett.134.013601}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013601}, shortjournal = {Phys. Rev. Lett.}, title = {Nonlinear optics using intense optical coherent state superpositions}, volume = {134}, year = {2025}, }
• (2025). Continuous collective strong coupling of strontium atoms to a high finesse ring cavity. PRL, 134(1), 013403. (www)

  @article{ , abstract = {We demonstrate continuous loading and strong collective coupling of atoms to a high finesse ring cavity. A series of spatially separated laser cooling stages delivers a continuous flux of into an intracavity magic wavelength lattice where the atoms are deterministically transported inside the ring cavity. We observe a continuous atom-cavity vacuum Rabi splitting, demonstrating the first steady-state strong collective coupling on a narrow linewidth atomic transition. This Letter opens the path to future continuous cold atom devices, such as a continuous wave superradiant laser with millihertz linewidth and low vibration sensitivity, enabling searches for new physics and technologies.}, archive = {J_PRL}, author = {Julia R. K. Cline and Vera M. Schäfer and Zhijing Niu and Dylan J. Young and Tai Hyun Yoon and James K. Thompson}, doi = {10.1103/PhysRevLett.134.013403}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013403}, shortjournal = {Phys. Rev. Lett.}, title = {Continuous collective strong coupling of strontium atoms to a high finesse ring cavity}, volume = {134}, year = {2025}, }
• (2025). Production and stabilization of a spin mixture of ultracold dipolar bose gases. PRL, 134(1), 013402. (www)

  @article{ , abstract = {Mixtures of ultracold gases with long-range interactions are expected to open new avenues in the study of quantum matter. Natural candidates for this research are spin mixtures of atomic species with large magnetic moments. However, the lifetime of such assemblies can be strongly affected by the dipolar relaxation that occurs in spin-flip collisions. Here we present experimental results for a mixture composed of the two lowest Zeeman states of Dy 162 atoms, that act as dark states with respect to a light-induced quadratic Zeeman effect. We show that, due to an interference phenomenon, the rate for such inelastic processes is dramatically reduced with respect to the Wigner threshold law. Additionally, we determine the scattering lengths characterizing the s -wave interaction between these states, providing all necessary data to predict the miscibility range of the mixture, depending on its dimensionality.}, archive = {J_PRL}, author = {Maxime Lecomte and Alexandre Journeaux and Julie Veschambre and Jean Dalibard and Raphael Lopes}, doi = {10.1103/PhysRevLett.134.013402}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013402}, shortjournal = {Phys. Rev. Lett.}, title = {Production and stabilization of a spin mixture of ultracold dipolar bose gases}, volume = {134}, year = {2025}, }
• (2025). Dirac points and shear instability induced crystal transitions in honeycomb supersolids. PRL, 134(1), 013401. (www)

  @article{ , abstract = {The honeycomb supersolid state is predicted to form in a dipolar Bose-Einstein condensate with a planar confining potential. Our results for its excitation spectrum reveal the gapless bands and the emergence of Dirac points at the Brillouin zone edge, manifesting as points where the second sound and transverse sound bands touch. The honeycomb supersolid has three sound speeds that we connect to its elastic parameters through hydrodynamic theory. From this analysis we find conditions where a shear instability occurs as the honeycomb rigidity disappears. This gives insight into the nonequilibrium dynamics following an interaction quench, where the honeycomb pattern melts and different crystal orders emerge.}, archive = {J_PRL}, author = {P. B. Blakie}, doi = {10.1103/PhysRevLett.134.013401}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013401}, shortjournal = {Phys. Rev. Lett.}, title = {Dirac points and shear instability induced crystal transitions in honeycomb supersolids}, volume = {134}, year = {2025}, }
• (2025). Quantifying light-assisted collisions in optical tweezers across the hyperfine spectrum. PRL, 134(1), 013202. (www)

  @article{ , abstract = {We investigate the role of hyperfine structure in resonant-dipole interactions between two atoms cotrapped in an optical tweezer. Two-body loss rates from light-assisted collisions (LACs) are measured across the Rb 87 hyperfine spectrum and connected to properties of molecular photoassociation potentials via a semiclassical model. To obtain our results, we introduce an imaging technique that leverages repulsive LACs to detect two atoms in a trap, thereby circumventing parity constraints in tweezers. Our findings offer key insights for exploiting hyperfine structure in laser-induced collisions to control cold atoms and molecules in a broad range of quantum science applications.}, archive = {J_PRL}, author = {Steven K. Pampel and Matteo Marinelli and Mark O. Brown and José P. D’Incao and Cindy A. Regal}, doi = {10.1103/PhysRevLett.134.013202}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013202}, shortjournal = {Phys. Rev. Lett.}, title = {Quantifying light-assisted collisions in optical tweezers across the hyperfine spectrum}, volume = {134}, year = {2025}, }
• (2025). Operating a multi-ion clock with dynamical decoupling. PRL, 134(1), 013201. (www)

  @article{ , abstract = {We study and characterize a quasicontinuous dynamical decoupling scheme that effectively suppresses dominant frequency shifts in a multi-ion optical clock. Addressing the challenge of inhomogeneous frequency shifts in such systems, our scheme mitigates primary contributors, namely, the electric quadrupole and the linear Zeeman shifts. Based on 8 8 S r + ions, we implement the scheme in linear chains of up to 7 ions and demonstrate a significant suppression of the shift by more than 3 orders of magnitude, leading to relative frequency inhomogeneity below 7 × 1 0 − 1 7 . Additionally, we evaluate the associated systematic shift arising from the radio-frequency drive used in the QCDD scheme, showing that, in the presented realization, its contribution to the systematic relative frequency uncertainty is below 1 0 − 1 7 , with the potential for further improvement. These results provide a promising avenue toward implementing multi-ion clocks exhibiting an order of magnitude or more improvement in stability while maintaining a similar high degree of accuracy to that of single-ion clocks.}, archive = {J_PRL}, author = {Nitzan Akerman and Roee Ozeri}, doi = {10.1103/PhysRevLett.134.013201}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013201}, shortjournal = {Phys. Rev. Lett.}, title = {Operating a multi-ion clock with dynamical decoupling}, volume = {134}, year = {2025}, }
• (2025). Single-beam grating-chip 3D and 1D optical lattices. PRL, 134(1), 013001. (www)

  @article{ , abstract = {Ultracold atoms are crucial for unlocking truly precise and accurate quantum metrology and provide an essential platform for quantum computing, communication, and memories. One of the largest ongoing challenges is the miniaturization of these quantum devices. Here, we show that the typically macroscopic optical lattice architecture at the heart of many ultraprecise quantum technologies can be realized with a single-input laser beam on the same diffractive chip already used to create the ultracold atoms. Moreover, this inherently ultrastable platform enables access to a plethora of new lattice dimensionalities and geometries, ideally suited for the design of high-accuracy, portable quantum devices.}, archive = {J_PRL}, author = {Alan Bregazzi and James P. McGilligan and Paul F. Griffin and Erling Riis and Aidan S. Arnold}, doi = {10.1103/PhysRevLett.134.013001}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {013001}, shortjournal = {Phys. Rev. Lett.}, title = {Single-beam grating-chip 3D and 1D optical lattices}, volume = {134}, year = {2025}, }
• (2025). Near-threshold dipole strength in $^{10}\mathrm{Be}$ with isoscalar character. PRL, 134(1), 012502. (www)

  @article{ , abstract = {Isoscalar dipole transitions are a distinctive fingerprint of cluster structures. A 1 − resonance at 7.27(10) MeV, located just below the α -emission threshold, has been observed in the deuteron inelastic scattering reactions off Be 10 . The deformation lengths of the excited states in Be 10 below 9 MeV have been inferred from the differential cross sections using coupled channel calculations. This observed 1 − resonance has isoscalar characteristics and exhausts approximately 5%–15% of the isoscalar dipole energy-weighted sum rule, providing evidence for pronounced α cluster structure in Be 10 . The Gamow coupled channel approach supports this interpretation and suggests the near-threshold effect might be playing an important role in this excitation energy domain. The α + α + n + n four-body calculation reproduces the observed enhanced dipole strength, implying that the four-body cluster structure is essential to describe the 1 − states in Be 10 .}, archive = {J_PRL}, author = {J. Chen and Y. Ayyad and D. Bazin and W. Mittig and M. Z. Serikow and N. Keeley and S. M. Wang and B. Zhou and J. C. Zamora and S. Beceiro-Novo and M. Cortesi and M. DeNudt and S. Heinitz and S. Giraud and P. Gueye and C. R. Hoffman and B. P. Kay and E. A. Maugeri and B. G. Monteagudo and H. Li and W. P. Liu and A. Muñoz and F. Ndayisabye and J. Pereira and N. Rijal and C. Santamaria and D. Schumann and N. Watwood and G. Votta and P. Yin and C. X. Yuan and Y. N. Zhang}, doi = {10.1103/PhysRevLett.134.012502}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {012502}, shortjournal = {Phys. Rev. Lett.}, title = {Near-threshold dipole strength in $^{10}\mathrm{Be}$ with isoscalar character}, volume = {134}, year = {2025}, }
• (2025). Ab initio strategy for taming the nuclear-structure dependence of ${V}_{ud}$ extractions: The $^{10}\mathrm{C}\ensuremath{\rightarrow}^{10}\mathrm{B}$ superallowed transition. PRL, 134(1), 012501. (www)

  @article{ , abstract = {We report the first ab initio calculation of the nuclear-structure-dependent radiative correction to the superallowed transition, computed with the no-core shell model and chiral effective field theory. We obtain with a 1.6-times reduction in the total uncertainty when compared to the current literature estimate based on the shell model and Fermi gas picture. This Letter paves the way for a precise determination of from superallowed beta decays within a systematically improvable framework.}, archive = {J_PRL}, author = {Michael Gennari and Mehdi Drissi and Mikhail Gorchtein and Petr Navrátil and Chien-Yeah Seng}, doi = {10.1103/PhysRevLett.134.012501}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {012501}, shortjournal = {Phys. Rev. Lett.}, title = {Ab initio strategy for taming the nuclear-structure dependence of ${V}_{ud}$ extractions: The $^{10}\mathrm{C}\ensuremath{\rightarrow}^{10}\mathrm{B}$ superallowed transition}, volume = {134}, year = {2025}, }
• (2025). High-temperature QCD static potential beyond leading order. PRL, 134(1), 011905. (www)

  @article{ , abstract = {We calculate the leading and next-to-leading corrections to the real-time QCD static potential in a high-temperature medium in the region where bound states transit from narrow resonances to wide ones. We find sizable contributions to both the real and the imaginary part of the potential. The calculation involves both loop diagrams calculated in the hard thermal loop effective theory and power corrections to the hard thermal loop Lagrangian calculated in QCD. We compare our results with recent lattice data and check the consistency of different methods used in lattice calculations. We also discuss the usefulness of our results to guide lattice inputs.}, archive = {J_PRL}, author = {Margaret E. Carrington and Cristina Manuel and Joan Soto}, doi = {10.1103/PhysRevLett.134.011905}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011905}, shortjournal = {Phys. Rev. Lett.}, title = {High-temperature QCD static potential beyond leading order}, volume = {134}, year = {2025}, }
• (2025). Study of ${D}_{s}^{+}\ensuremath{\rightarrow}{f}_{0}(980){\ensuremath{\rho}}^{+}$ and $\ensuremath{\phi}{\ensuremath{\pi}}^{+}$ decays through ${D}_{s}^{+}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}$. PRL, 134(1), 011904. (www)

  @article{ , abstract = {We perform the first amplitude analysis of decays based on data samples of electron-positron collisions recorded with the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV, corresponding to an integrated luminosity of . We report the observation of with a statistical significance greater than and determine the branching fractions and . Moreover, we measure the relative branching fraction between and to be ., which deviates from the world average value by more than .}, archive = {J_PRL}, author = {M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and J. F. Chang and G. R. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and J. J. Lane and P. Larin and L. Lavezzi and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. Z. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and X. Liu and Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. Ma and Y. M. Ma and F. E. Maas and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and P. Patteri and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. P. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and J. F. Shangguan and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and H. C. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and N. Y. Wang and S. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. C. Xu and Z. P. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. F. Yang and Y. X. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. D. Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and Z. Y. Zhang and Z. Z. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and S. Q. Zhu and T. J. Zhu and W. D. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.011904}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011904}, shortjournal = {Phys. Rev. Lett.}, title = {Study of ${D}_{s}^{+}\ensuremath{\rightarrow}{f}_{0}(980){\ensuremath{\rho}}^{+}$ and $\ensuremath{\phi}{\ensuremath{\pi}}^{+}$ decays through ${D}_{s}^{+}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}$}, volume = {134}, year = {2025}, }
• (2025). QCD constraints on isospin-dense matter and the nuclear equation of state. PRL, 134(1), 011903. (www)

  @article{ , abstract = {Understanding the behavior of dense hadronic matter is a central goal in nuclear physics as it governs the nature and dynamics of astrophysical objects such as supernovae and neutron stars. Because of the nonperturbative nature of quantum chromodynamics (QCD), little is known rigorously about hadronic matter in these extreme conditions. Here, lattice QCD calculations are used to compute thermodynamic quantities and the equation of state of QCD over a wide range of isospin chemical potentials with controlled systematic uncertainties. Agreement is seen with chiral perturbation theory when the chemical potential is small. Comparison to perturbative QCD at large chemical potential allows for an estimate of the gap in the superconducting phase, and this quantity is seen to agree with perturbative determinations. Since the partition function for an isospin chemical potential bounds the partition function for a baryon chemical potential , these calculations also provide rigorous nonperturbative QCD bounds on the symmetric nuclear matter equation of state over a wide range of baryon densities for the first time.}, archive = {J_PRL}, author = {Ryan Abbott and William Detmold and Marc Illa and Assumpta Parreño and Robert J. Perry and Fernando Romero-López and Phiala E. Shanahan and Michael L. Wagman}, doi = {10.1103/PhysRevLett.134.011903}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011903}, shortjournal = {Phys. Rev. Lett.}, title = {QCD constraints on isospin-dense matter and the nuclear equation of state}, volume = {134}, year = {2025}, }
• (2025). Model-independent tests of the hadronic vacuum polarization contribution to the muon $g\ensuremath{-}2$. PRL, 134(1), 011902. (www)

  @article{ , abstract = {The hadronic vacuum polarization (HVP) contributions to the muon g − 2 are the crucial quantity to resolve whether new physics is present or not in the comparison between the standard model (SM) prediction and experimental measurements at Fermilab. They are commonly and historically determined via dispersion relations using a vast catalogue of experimentally measured, low-energy e + e − → hadrons cross section data as input. These dispersive estimates result in a SM prediction that exhibits a muon g − 2 discrepancy of more than 5 σ when compared to experiment. However, recent lattice QCD evaluations of the HVP and a new hadronic cross section measurement from the CMD-3 experiment favor a no-new-physics scenario and, therefore, exhibit a common tension with the previous e + e − → hadrons data. This study explores the current and future implications of these two scenarios on other observables that are also sensitive to the HVP contributions in the hope that they may provide independent tests of the current tensions observed in the muon g − 2 .}, archive = {J_PRL}, author = {Luca Di Luzio and Alexander Keshavarzi and Antonio Masiero and Paride Paradisi}, doi = {10.1103/PhysRevLett.134.011902}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011902}, shortjournal = {Phys. Rev. Lett.}, title = {Model-independent tests of the hadronic vacuum polarization contribution to the muon $g\ensuremath{-}2$}, volume = {134}, year = {2025}, }
• (2025). New standard for the logarithmic accuracy of parton showers. PRL, 134(1), 011901. (www)

  @article{ , abstract = {We report on a major milestone in the construction of logarithmically accurate final-state parton showers, achieving next-to-next-to-leading-logarithmic (NNLL) accuracy for the wide class of observables known as event shapes. The key to this advance lies in the identification of the relation between critical NNLL analytic resummation ingredients and their parton-shower counterparts. Our analytic discussion is supplemented with numerical tests of the logarithmic accuracy of three shower variants for more than a dozen distinct event-shape observables in Z → q q ¯ and Higgs → g g decays. The NNLL terms are phenomenologically sizeable, as illustrated in comparisons to data.}, archive = {J_PRL}, author = {Melissa van Beekveld and Mrinal Dasgupta and Basem Kamal El-Menoufi and Silvia Ferrario Ravasio and Keith Hamilton and Jack Helliwell and Alexander Karlberg and Pier Francesco Monni and Gavin P. Salam and Ludovic Scyboz and Alba Soto-Ontoso and Gregory Soyez}, doi = {10.1103/PhysRevLett.134.011901}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011901}, shortjournal = {Phys. Rev. Lett.}, title = {New standard for the logarithmic accuracy of parton showers}, volume = {134}, year = {2025}, }
• (2025). Dark matter search results from $1.54\text{ }\text{ }\mathrm{Tonne}\ifmmode\cdot\else\textperiodcentered\fi{}\mathrm{Year}$ exposure of PandaX-4T. PRL, 134(1), 011805. (www)

  @article{ , abstract = {In this Letter, we report the dark matter search results from the commissioning run (Run0) and the first science run (Run1) of the PandaX-4T experiment. The two datasets were processed with a unified procedure, with the Run1 data treated blindly. The data processing is improved compared to previous work, unifying the low-level signal reconstruction in a wide energy range up to 120 keV. With a total exposure of 1.54 tonne · year , no significant excess of nuclear recoil events is found. The lowest 90% confidence level exclusion on the spin-independent cross section is 1.6 × 10 − 47 cm 2 at a dark matter mass of 40 GeV / c 2 . Our results represent the most stringent constraint for a dark matter mass above 100 GeV / c 2 .}, archive = {J_PRL}, author = {Zihao Bo and Wei Chen and Xun Chen and Yunhua Chen and Zhaokan Cheng and Xiangyi Cui and Yingjie Fan and Deqing Fang and Zhixing Gao and Zhixing Gao and Lisheng Geng and Karl Giboni and Xunan Guo and Xuyuan Guo and Zichao Guo and Chencheng Han and Ke Han and Changda He and Jinrong He and Di Huang and Houqi Huang and Junting Huang and Ruquan Hou and Yu Hou and Xiangdong Ji and Xiangpan Ji and Yonglin Ju and Chenxiang Li and Jiafu Li and Mingchuan Li and Shuaijie Li and Tao Li and Zhiyuan Li and Qing Lin and Jianglai Liu and Congcong Lu and Xiaoying Lu and Lingyin Luo and Yunyang Luo and Wenbo Ma and Yugang Ma and Yajun Mao and Yue Meng and Xuyang Ning and Binyu Pang and Ningchun Qi and Zhicheng Qian and Xiangxiang Ren and Dong Shan and Xiaofeng Shang and Xiyuan Shao and Guofang Shen and Manbin Shen and Wenliang Sun and Yi Tao and Anqing Wang and Guanbo Wang and Hao Wang and Jiamin Wang and Lei Wang and Meng Wang and Qiuhong Wang and Shaobo Wang and Siguang Wang and Wei Wang and Xiuli Wang and Xu Wang and Zhou Wang and Yuehuan Wei and Weihao Wu and Yuan Wu and Mengjiao Xiao and Xiang Xiao and Kaizhi Xiong and Yifan Xu and Shunyu Yao and Binbin Yan and Xiyu Yan and Yong Yang and Peihua Ye and Chunxu Yu and Ying Yuan and Zhe Yuan and Youhui Yun and Xinning Zeng and Minzhen Zhang and Peng Zhang and Shibo Zhang and Shu Zhang and Tao Zhang and Wei Zhang and Yang Zhang and Yingxin Zhang and Yuanyuan Zhang and Li Zhao and Jifang Zhou and Jiaxu Zhou and Jiayi Zhou and Ning Zhou and Xiaopeng Zhou and Yubo Zhou and Zhizhen Zhou}, doi = {10.1103/PhysRevLett.134.011805}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011805}, shortjournal = {Phys. Rev. Lett.}, title = {Dark matter search results from $1.54\text{ }\text{ }\mathrm{Tonne}\ifmmode\cdot\else\textperiodcentered\fi{}\mathrm{Year}$ exposure of PandaX-4T}, volume = {134}, year = {2025}, }
• (2025). First direct-detection results on sub-GeV dark matter using the SENSEI detector at SNOLAB. PRL, 134(1), 011804. (www)

  @article{ , abstract = {We present the first results from a dark matter search using six Skipper-CCDs in the SENSEI detector operating at SNOLAB. We employ a bias-mitigation technique of hiding approximately 46% of our total data and aggressively mask images to remove backgrounds. Given a total exposure after masking of 100.72 gram-days from well-performing sensors, we observe 55 two-electron events, 4 three-electron events, and no events containing 4–10 electrons. The two-electron events are consistent with pileup from one-electron events. Among the 4 three-electron events, 2 appear in pixels that are likely impacted by detector defects, although not strongly enough to trigger our “hot-pixel” mask. We use these data to set world-leading constraints on sub-GeV dark matter interacting with electrons and nuclei.}, archive = {J_PRL}, author = {Prakruth Adari and Itay M. Bloch and Ana M. Botti and Mariano Cababie and Gustavo Cancelo and Brenda A. Cervantes-Vergara and Michael Crisler and Miguel Daal and Ansh Desai and Ansh Desai and Alex Drlica-Wagner and Rouven Essig and Juan Estrada and Erez Etzion and Guillermo Fernandez Moroni and Stephen E. Holland and Jonathan Kehat and Yaron Korn and Ian Lawson and Steffon Luoma and Aviv Orly and Santiago E. Perez and Dario Rodrigues and Nathan A. Saffold and Silvia Scorza and Aman Singal and Miguel Sofo-Haro and Leandro Stefanazzi and Kelly Stifter and Javier Tiffenberg and Sho Uemura and Edgar Marrufo Villalpando and Tomer Volansky and Yikai Wu and Tien-Tien Yu and Timón Emken and Hailin Xu}, doi = {10.1103/PhysRevLett.134.011804}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011804}, shortjournal = {Phys. Rev. Lett.}, title = {First direct-detection results on sub-GeV dark matter using the SENSEI detector at SNOLAB}, volume = {134}, year = {2025}, }
• (2025). Test of lepton universality and measurement of the form factors of ${D}^{0}\ensuremath{\rightarrow}{K}^{*}(892{)}^{\ensuremath{-}}{\ensuremath{\mu}}^{+}{\ensuremath{\nu}}_{\ensuremath{\mu}}$. PRL, 134(1), 011803. (www)

  @article{ , abstract = {One of the main goals of studying semileptonic decays in flavor physics is to gain a better understanding of hadronic transitions in the nonperturbative region of Quantum Chromodynamics. This involves measuring Cabibbo-Kobayashi-Maskawa matrix elements, understanding form factors, and comparing them with theoretical predictions. We report a first study of the semileptonic decay by analyzing an annihilation data sample of collected at the center-of-mass energy of 3.773 GeV with the BESIII detector. The absolute branching fraction of is measured for the first time, providing necessary input for extracting the Cabibbo-Kobayashi-Maskawa matrix element through this process. This measurement allows us to test lepton flavor universality, with no indication of violation found. Furthermore, a series of hadronic form factors have been determined and compared with theoretical predictions, which will impose stricter constraints on theoretical models.}, archive = {J_PRL}, author = {M. Ablikim and M. N. Achasov and P. Adlarson and O. Afedulidis and X. C. Ai and R. Aliberti and A. Amoroso and Q. An and Y. Bai and Y. Bai and O. Bakina and I. Balossino and Y. Ban and H.-R. Bao and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and I. Boyko and R. A. Briere and A. Brueggemann and H. Cai and X. Cai and A. Calcaterra and G. F. Cao and N. Cao and S. A. Cetin and J. F. Chang and G. R. Che and G. Chelkov and C. Chen and C. H. Chen and Chao Chen and G. Chen and H. S. Chen and H. Y. Chen and M. L. Chen and S. J. Chen and S. L. Chen and S. M. Chen and T. Chen and X. R. Chen and X. T. Chen and Y. B. Chen and Y. Q. Chen and Z. J. Chen and Z. Y. Chen and S. K. Choi and G. Cibinetto and F. Cossio and J. J. Cui and H. L. Dai and J. P. Dai and A. Dbeyssi and R. E. de Boer and D. Dedovich and C. Q. Deng and Z. Y. Deng and A. Denig and I. Denysenko and M. Destefanis and F. De Mori and B. Ding and X. X. Ding and Y. Ding and Y. Ding and J. Dong and L. Y. Dong and M. Y. Dong and X. Dong and M. C. Du and S. X. Du and Y. Y. Duan and Z. H. Duan and P. Egorov and Y. H. Fan and J. Fang and J. Fang and S. S. Fang and W. X. Fang and Y. Fang and Y. Q. Fang and R. Farinelli and L. Fava and F. Feldbauer and G. Felici and C. Q. Feng and J. H. Feng and Y. T. Feng and M. Fritsch and C. D. Fu and J. L. Fu and Y. W. Fu and H. Gao and X. B. Gao and Y. N. Gao and Yang Gao and S. Garbolino and I. Garzia and L. Ge and P. T. Ge and Z. W. Ge and C. Geng and E. M. Gersabeck and A. Gilman and K. Goetzen and L. Gong and W. X. Gong and W. Gradl and S. Gramigna and M. Greco and M. H. Gu and Y. T. Gu and C. Y. Guan and A. Q. Guo and L. B. Guo and M. J. Guo and R. P. Guo and Y. P. Guo and A. Guskov and J. Gutierrez and K. L. Han and T. T. Han and F. Hanisch and X. Q. Hao and F. A. Harris and K. K. He and K. L. He and F. H. Heinsius and C. H. Heinz and Y. K. Heng and C. Herold and T. Holtmann and P. C. Hong and G. Y. Hou and X. T. Hou and Y. R. Hou and Z. L. Hou and B. Y. Hu and H. M. Hu and J. F. Hu and S. L. Hu and T. Hu and Y. Hu and G. S. Huang and K. X. Huang and L. Q. Huang and X. T. Huang and Y. P. Huang and Y. S. Huang and T. Hussain and F. Hölzken and N. Hüsken and N. in der Wiesche and J. Jackson and S. Janchiv and J. H. Jeong and Q. Ji and Q. P. Ji and W. Ji and X. B. Ji and X. L. Ji and Y. Y. Ji and X. Q. Jia and Z. K. Jia and D. Jiang and H. B. Jiang and P. C. Jiang and S. S. Jiang and T. J. Jiang and X. S. Jiang and Y. Jiang and J. B. Jiao and J. K. Jiao and Z. Jiao and S. Jin and Y. Jin and M. Q. Jing and X. M. Jing and T. Johansson and S. Kabana and N. Kalantar-Nayestanaki and X. L. Kang and X. S. Kang and M. Kavatsyuk and B. C. Ke and V. Khachatryan and A. Khoukaz and R. Kiuchi and O. B. Kolcu and B. Kopf and M. Kuessner and X. Kui and N. Kumar and A. Kupsc and W. Kühn and J. J. Lane and P. Larin and L. Lavezzi and T. T. Lei and Z. H. Lei and M. Lellmann and T. Lenz and C. Li and C. Li and C. H. Li and Cheng Li and D. M. Li and F. Li and G. Li and H. B. Li and H. J. Li and H. N. Li and Hui Li and J. R. Li and J. S. Li and K. Li and L. J. Li and L. K. Li and Lei Li and M. H. Li and P. R. Li and Q. M. Li and Q. X. Li and R. Li and S. X. Li and T. Li and W. D. Li and W. G. Li and X. Li and X. H. Li and X. L. Li and X. Y. Li and X. Z. Li and Y. G. Li and Z. J. Li and Z. Y. Li and C. Liang and H. Liang and H. Liang and Y. F. Liang and Y. T. Liang and G. R. Liao and L. Z. Liao and Y. P. Liao and J. Libby and A. Limphirat and C. C. Lin and D. X. Lin and T. Lin and B. J. Liu and B. X. Liu and C. Liu and C. X. Liu and F. Liu and F. H. Liu and Feng Liu and G. M. Liu and H. Liu and H. B. Liu and H. H. Liu and H. M. Liu and Huihui Liu and J. B. Liu and J. Y. Liu and K. Liu and K. Y. Liu and Ke Liu and L. Liu and L. C. Liu and Lu Liu and M. H. Liu and P. L. Liu and Q. Liu and S. B. Liu and T. Liu and W. K. Liu and W. M. Liu and X. Liu and X. Liu and Y. Liu and Y. Liu and Y. B. Liu and Z. A. Liu and Z. D. Liu and Z. Q. Liu and X. C. Lou and F. X. Lu and H. J. Lu and J. G. Lu and X. L. Lu and Y. Lu and Y. P. Lu and Z. H. Lu and C. L. Luo and J. R. Luo and M. X. Luo and T. Luo and X. L. Luo and X. R. Lyu and Y. F. Lyu and F. C. Ma and H. Ma and H. L. Ma and J. L. Ma and L. L. Ma and M. M. Ma and Q. M. Ma and R. Q. Ma and T. Ma and X. T. Ma and X. Y. Ma and Y. Ma and Y. M. Ma and F. E. Maas and M. Maggiora and S. Malde and Y. J. Mao and Z. P. Mao and S. Marcello and Z. X. Meng and J. G. Messchendorp and G. Mezzadri and H. Miao and T. J. Min and R. E. Mitchell and X. H. Mo and B. Moses and N. Yu. Muchnoi and J. Muskalla and Y. Nefedov and F. Nerling and L. S. Nie and I. B. Nikolaev and Z. Ning and S. Nisar and Q. L. Niu and W. D. Niu and Y. Niu and S. L. Olsen and Q. Ouyang and S. Pacetti and X. Pan and Y. Pan and A. Pathak and P. Patteri and Y. P. Pei and M. Pelizaeus and H. P. Peng and Y. Y. Peng and K. Peters and J. L. Ping and R. G. Ping and S. Plura and V. Prasad and F. Z. Qi and H. Qi and H. R. Qi and M. Qi and T. Y. Qi and S. Qian and W. B. Qian and C. F. Qiao and X. K. Qiao and J. J. Qin and L. Q. Qin and L. Y. Qin and X. S. Qin and Z. H. Qin and J. F. Qiu and Z. H. Qu and C. F. Redmer and K. J. Ren and A. Rivetti and M. Rolo and G. Rong and Ch. Rosner and S. N. Ruan and N. Salone and A. Sarantsev and Y. Schelhaas and K. Schoenning and M. Scodeggio and K. Y. Shan and W. Shan and X. Y. Shan and Z. J. Shang and L. G. Shao and M. Shao and C. P. Shen and H. F. Shen and W. H. Shen and X. Y. Shen and B. A. Shi and H. Shi and H. C. Shi and J. L. Shi and J. Y. Shi and Q. Q. Shi and S. Y. Shi and X. Shi and J. J. Song and T. Z. Song and W. M. Song and Y. J. Song and Y. X. Song and S. Sosio and S. Spataro and F. Stieler and Y. J. Su and G. B. Sun and G. X. Sun and H. Sun and H. K. Sun and J. F. Sun and K. Sun and L. Sun and S. S. Sun and T. Sun and W. Y. Sun and Y. Sun and Y. J. Sun and Y. Z. Sun and Z. Q. Sun and Z. T. Sun and C. J. Tang and G. Y. Tang and J. Tang and M. Tang and Y. A. Tang and L. Y. Tao and Q. T. Tao and M. Tat and J. X. Teng and V. Thoren and W. H. Tian and Y. Tian and Z. F. Tian and I. Uman and Y. Wan and S. J. Wang and B. Wang and B. L. Wang and Bo Wang and D. Y. Wang and F. Wang and H. J. Wang and J. J. Wang and J. P. Wang and K. Wang and L. L. Wang and M. Wang and N. Y. Wang and S. Wang and S. Wang and T. Wang and T. J. Wang and W. Wang and W. Wang and W. P. Wang and X. Wang and X. F. Wang and X. J. Wang and X. L. Wang and X. N. Wang and Y. Wang and Y. D. Wang and Y. F. Wang and Y. L. Wang and Y. N. Wang and Y. Q. Wang and Yaqian Wang and Yi Wang and Z. Wang and Z. L. Wang and Z. Y. Wang and Ziyi Wang and D. H. Wei and F. Weidner and S. P. Wen and Y. R. Wen and U. Wiedner and G. Wilkinson and M. Wolke and L. Wollenberg and C. Wu and J. F. Wu and L. H. Wu and L. J. Wu and X. Wu and X. H. Wu and Y. Wu and Y. H. Wu and Y. J. Wu and Z. Wu and L. Xia and X. M. Xian and B. H. Xiang and T. Xiang and D. Xiao and G. Y. Xiao and S. Y. Xiao and Y. L. Xiao and Z. J. Xiao and C. Xie and X. H. Xie and Y. Xie and Y. G. Xie and Y. H. Xie and Z. P. Xie and T. Y. Xing and C. F. Xu and C. J. Xu and G. F. Xu and H. Y. Xu and M. Xu and Q. J. Xu and Q. N. Xu and W. Xu and W. L. Xu and X. P. Xu and Y. C. Xu and Z. P. Xu and Z. S. Xu and F. Yan and L. Yan and W. B. Yan and W. C. Yan and X. Q. Yan and H. J. Yang and H. L. Yang and H. X. Yang and T. Yang and Y. Yang and Y. F. Yang and Y. F. Yang and Y. X. Yang and Z. W. Yang and Z. P. Yao and M. Ye and M. H. Ye and J. H. Yin and Z. Y. You and B. X. Yu and C. X. Yu and G. Yu and J. S. Yu and T. Yu and X. D. Yu and Y. C. Yu and C. Z. Yuan and J. Yuan and J. Yuan and L. Yuan and S. C. Yuan and Y. Yuan and Z. Y. Yuan and C. X. Yue and A. A. Zafar and F. R. Zeng and S. H. Zeng and X. Zeng and Y. Zeng and Y. J. Zeng and Y. J. Zeng and X. Y. Zhai and Y. C. Zhai and Y. H. Zhan and A. Q. Zhang and B. L. Zhang and B. X. Zhang and D. H. Zhang and G. Y. Zhang and H. Zhang and H. Zhang and H. C. Zhang and H. H. Zhang and H. H. Zhang and H. Q. Zhang and H. R. Zhang and H. Y. Zhang and J. Zhang and J. Zhang and J. J. Zhang and J. L. Zhang and J. Q. Zhang and J. S. Zhang and J. W. Zhang and J. X. Zhang and J. Y. Zhang and J. Z. Zhang and Jianyu Zhang and L. M. Zhang and Lei Zhang and P. Zhang and Q. Y. Zhang and R. Y. Zhang and S. H. Zhang and Shulei Zhang and X. D. Zhang and X. M. Zhang and X. Y. Zhang and Y. Zhang and Y. Zhang and Y. T. Zhang and Y. H. Zhang and Y. M. Zhang and Yan Zhang and Z. D. Zhang and Z. H. Zhang and Z. L. Zhang and Z. Y. Zhang and Z. Y. Zhang and Z. Z. Zhang and G. Zhao and J. Y. Zhao and J. Z. Zhao and L. Zhao and Lei Zhao and M. G. Zhao and N. Zhao and R. P. Zhao and S. J. Zhao and Y. B. Zhao and Y. X. Zhao and Z. G. Zhao and A. Zhemchugov and B. Zheng and B. M. Zheng and J. P. Zheng and W. J. Zheng and Y. H. Zheng and B. Zhong and X. Zhong and H. Zhou and J. Y. Zhou and L. P. Zhou and S. Zhou and X. Zhou and X. K. Zhou and X. R. Zhou and X. Y. Zhou and Y. Z. Zhou and J. Zhu and K. Zhu and K. J. Zhu and K. S. Zhu and L. Zhu and L. X. Zhu and S. H. Zhu and S. Q. Zhu and T. J. Zhu and W. D. Zhu and Y. C. Zhu and Z. A. Zhu and J. H. Zou and J. Zu}, doi = {10.1103/PhysRevLett.134.011803}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011803}, shortjournal = {Phys. Rev. Lett.}, title = {Test of lepton universality and measurement of the form factors of ${D}^{0}\ensuremath{\rightarrow}{K}^{*}(892{)}^{\ensuremath{-}}{\ensuremath{\mu}}^{+}{\ensuremath{\nu}}_{\ensuremath{\mu}}$}, volume = {134}, year = {2025}, }
• (2025). Measurement of $CP$ asymmetries in ${B}^{0}\ensuremath{\rightarrow}{K}_{S}^{0}{\ensuremath{\pi}}^{0}\ensuremath{\gamma}$ decays at belle II. PRL, 134(1), 011802. (www)

  @article{ , abstract = {We report measurements of time-dependent asymmetries in decays based on a data sample of events collected at the resonance with the Belle II detector. The Belle II experiment operates at the SuperKEKB asymmetric-energy collider. We measure decay-time distributions to determine -violating parameters and . We determine these parameters for two ranges of invariant mass: , which is dominated by decays, and a complementary region . Our results have improved precision as compared to previous measurements and are consistent with theory predictions.}, archive = {J_PRL}, author = {I. Adachi and L. Aggarwal and H. Ahmed and H. Aihara and N. Akopov and A. Aloisio and N. Anh Ky and D. M. Asner and H. Atmacan and H. Atmacan and T. Aushev and V. Aushev and M. Aversano and R. Ayad and V. Babu and H. Bae and S. Bahinipati and P. Bambade and Sw. Banerjee and S. Bansal and M. Barrett and J. Baudot and A. Baur and A. Beaubien and F. Becherer and J. Becker and J. V. Bennett and F. U. Bernlochner and V. Bertacchi and M. Bertemes and E. Bertholet and M. Bessner and S. Bettarini and B. Bhuyan and F. Bianchi and L. Bierwirth and T. Bilka and S. Bilokin and D. Biswas and D. Bodrov and A. Bolz and A. Bondar and J. Borah and A. Boschetti and A. Bozek and M. Bračko and P. Branchini and R. A. Briere and T. E. Browder and A. Budano and S. Bussino and M. Campajola and L. Cao and G. Casarosa and C. Cecchi and J. Cerasoli and M.-C. Chang and P. Chang and R. Cheaib and P. Cheema and C. Chen and B. G. Cheon and K. Chilikin and K. Chirapatpimol and H.-E. Cho and K. Cho and S.-J. Cho and S.-K. Choi and S. Choudhury and J. Cochran and L. Corona and J. X. Cui and S. Das and F. Dattola and E. De La Cruz-Burelo and S. A. De La Motte and G. De Nardo and M. De Nuccio and G. De Pietro and R. de Sangro and M. Destefanis and S. Dey and R. Dhamija and A. Di Canto and F. Di Capua and J. Dingfelder and Z. Doležal and I. Domínguez Jiménez and T. V. Dong and M. Dorigo and D. Dorner and K. Dort and D. Dossett and S. Dreyer and S. Dubey and K. Dugic and G. Dujany and P. Ecker and M. Eliachevitch and P. Feichtinger and T. Ferber and D. Ferlewicz and T. Fillinger and C. Finck and G. Finocchiaro and A. Fodor and F. Forti and A. Frey and B. G. Fulsom and A. Gabrielli and E. Ganiev and M. Garcia-Hernandez and R. Garg and G. Gaudino and V. Gaur and A. Gaz and A. Gellrich and G. Ghevondyan and D. Ghosh and H. Ghumaryan and G. Giakoustidis and R. Giordano and A. Giri and A. Glazov and B. Gobbo and R. Godang and O. Gogota and P. Goldenzweig and W. Gradl and T. Grammatico and E. Graziani and D. Greenwald and Z. Gruberová and T. Gu and Y. Guan and K. Gudkova and S. Halder and Y. Han and K. Hara and T. Hara and K. Hayasaka and H. Hayashii and S. Hazra and C. Hearty and M. T. Hedges and A. Heidelbach and I. Heredia de la Cruz and M. Hernández Villanueva and T. Higuchi and M. Hoek and M. Hohmann and P. Horak and C.-L. Hsu and T. Humair and T. Iijima and K. Inami and N. Ipsita and A. Ishikawa and R. Itoh and M. Iwasaki and P. Jackson and W. W. Jacobs and D. E. Jaffe and E.-J. Jang and Q. P. Ji and S. Jia and Y. Jin and K. K. Joo and H. Junkerkalefeld and M. Kaleta and D. Kalita and A. B. Kaliyar and J. Kandra and K. H. Kang and S. Kang and G. Karyan and T. Kawasaki and F. Keil and C. Kiesling and C.-H. Kim and D. Y. Kim and K.-H. Kim and Y.-K. Kim and H. Kindo and K. Kinoshita and P. Kodyš and T. Koga and S. Kohani and K. Kojima and A. Korobov and S. Korpar and E. Kovalenko and R. Kowalewski and T. M. G. Kraetzschmar and P. Križan and P. Krokovny and T. Kuhr and Y. Kulii and J. Kumar and M. Kumar and K. Kumara and T. Kunigo and A. Kuzmin and Y.-J. Kwon and S. Lacaprara and Y.-T. Lai and T. Lam and L. Lanceri and J. S. Lange and M. Laurenza and R. Leboucher and F. R. Le Diberder and M. J. Lee and P. Leo and D. Levit and C. Li and L. K. Li and S. X. Li and Y. Li and Y. B. Li and J. Libby and Y.-R. Lin and M. H. Liu and Q. Y. Liu and Z. Q. Liu and D. Liventsev and S. Longo and T. Lueck and T. Luo and C. Lyu and Y. Ma and M. Maggiora and S. P. Maharana and R. Maiti and S. Maity and G. Mancinelli and R. Manfredi and E. Manoni and M. Mantovano and D. Marcantonio and S. Marcello and C. Marinas and L. Martel and C. Martellini and A. Martini and T. Martinov and L. Massaccesi and M. Masuda and K. Matsuoka and D. Matvienko and S. K. Maurya and J. A. McKenna and R. Mehta and F. Meier and M. Merola and F. Metzner and C. Miller and M. Mirra and S. Mitra and K. Miyabayashi and H. Miyake and R. Mizuk and G. B. Mohanty and N. Molina-Gonzalez and S. Mondal and S. Moneta and H.-G. Moser and M. Mrvar and R. Mussa and I. Nakamura and K. R. Nakamura and M. Nakao and H. Nakazawa and Y. Nakazawa and A. Narimani Charan and M. Naruki and D. Narwal and Z. Natkaniec and A. Natochii and L. Nayak and M. Nayak and G. Nazaryan and M. Neu and C. Niebuhr and S. Nishida and S. Ogawa and Y. Onishchuk and H. Ono and Y. Onuki and P. Oskin and F. Otani and P. Pakhlov and G. Pakhlova and A. Panta and S. Pardi and K. Parham and H. Park and S.-H. Park and B. Paschen and A. Passeri and S. Patra and S. Paul and T. K. Pedlar and R. Peschke and R. Pestotnik and M. Piccolo and L. E. Piilonen and G. Pinna Angioni and P. L. M. Podesta-Lerma and T. Podobnik and S. Pokharel and C. Praz and S. Prell and E. Prencipe and M. T. Prim and I. Prudiiev and H. Purwar and P. Rados and G. Raeuber and S. Raiz and N. Rauls and K. Ravindran and M. Reif and S. Reiter and M. Remnev and I. Ripp-Baudot and G. Rizzo and S. H. Robertson and M. Roehrken and J. M. Roney and A. Rostomyan and N. Rout and G. Russo and D. A. Sanders and S. Sandilya and A. Sangal and L. Santelj and Y. Sato and V. Savinov and B. Scavino and C. Schmitt and C. Schwanda and A. J. Schwartz and M. Schwickardi and Y. Seino and A. Selce and K. Senyo and J. Serrano and M. E. Sevior and C. Sfienti and W. Shan and X. D. Shi and T. Shillington and T. Shimasaki and J.-G. Shiu and D. Shtol and B. Shwartz and A. Sibidanov and F. Simon and J. B. Singh and J. Skorupa and R. J. Sobie and M. Sobotzik and A. Soffer and A. Sokolov and E. Solovieva and S. Spataro and B. Spruck and M. Starič and P. Stavroulakis and S. Stefkova and R. Stroili and M. Sumihama and K. Sumisawa and W. Sutcliffe and H. Svidras and M. Takahashi and M. Takizawa and U. Tamponi and S. Tanaka and K. Tanida and F. Tenchini and A. Thaller and O. Tittel and R. Tiwary and D. Tonelli and E. Torassa and K. Trabelsi and I. Tsaklidis and M. Uchida and I. Ueda and Y. Uematsu and T. Uglov and K. Unger and Y. Unno and K. Uno and S. Uno and P. Urquijo and Y. Ushiroda and S. E. Vahsen and R. van Tonder and K. E. Varvell and M. Veronesi and A. Vinokurova and V. S. Vismaya and L. Vitale and V. Vobbilisetti and R. Volpe and B. Wach and M. Wakai and S. Wallner and E. Wang and M.-Z. Wang and X. L. Wang and Z. Wang and A. Warburton and M. Watanabe and S. Watanuki and C. Wessel and E. Won and Y. Xie and X. P. Xu and B. D. Yabsley and S. Yamada and S. B. Yang and J. Yelton and J. H. Yin and K. Yoshihara and C. Z. Yuan and Y. Yusa and L. Zani and F. Zeng and B. Zhang and Y. Zhang and V. Zhilich and Q. D. Zhou and X. Y. Zhou and V. I. Zhukova and R. Žlebčík}, doi = {10.1103/PhysRevLett.134.011802}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011802}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement of $CP$ asymmetries in ${B}^{0}\ensuremath{\rightarrow}{K}_{S}^{0}{\ensuremath{\pi}}^{0}\ensuremath{\gamma}$ decays at belle II}, volume = {134}, year = {2025}, }
• (2025). First joint oscillation analysis of super-kamiokande atmospheric and T2K accelerator neutrino data. PRL, 134(1), 011801. (www)

  @article{ , abstract = {The Super-Kamiokande and T2K Collaborations present a joint measurement of neutrino oscillation parameters from their atmospheric and beam neutrino data. It uses a common interaction model for events overlapping in neutrino energy and correlated detector systematic uncertainties between the two datasets, which are found to be compatible. Using 3244.4 days of atmospheric data and a beam exposure of 19.7 ( 16.3 ) × 10 20 protons on target in (anti)neutrino mode, the analysis finds a 1.9 σ exclusion of C P conservation (defined as J C P = 0 ) and a 1.2 σ exclusion of the inverted mass ordering.}, archive = {J_PRL}, author = {K. Abe and S. Abe and C. Bronner and Y. Hayato and K. Hiraide and K. Hosokawa and K. Ieki and M. Ikeda and J. Kameda and M. Ikeda and J. Kameda and Y. Kanemura and R. Kaneshima and Y. Kashiwagi and Y. Kataoka and S. Miki and S. Mine and M. Miura and S. Moriyama and M. Nakahata and Y. Nakano and S. Nakayama and Y. Noguchi and K. Sato and H. Sekiya and H. Shiba and K. Shimizu and M. Shiozawa and Y. Sonoda and Y. Suzuki and A. Takeda and Y. Takemoto and H. Tanaka and T. Yano and S. Han and T. Kajita and K. Okumura and T. Tashiro and T. Tomiya and X. Wang and S. Yoshida and P. Fernandez and L. Labarga and N. Ospina and B. Zaldivar and B. W. Pointon and E. Kearns and J. Mirabito and J. L. Raaf and L. Wan and T. Wester and J. Bian and N. J. Griskevich and M. B. Smy and H. W. Sobel and V. Takhistov and A. Yankelevich and J. Hill and M. C. Jang and S. H. Lee and D. H. Moon and R. G. Park and B. Bodur and K. Scholberg and C. W. Walter and A. Beauchêne and O. Drapier and A. Giampaolo and Th. A. Mueller and A. D. Santos and P. Paganini and B. Quilain and R. Rogly and T. Nakamura and J. S. Jang and L. N. Machado and J. G. Learned and K. Choi and N. Iovine and S. Cao and L. H. V. Anthony and D. Martin and N. W. Prouse and M. Scott and Y. Uchida and V. Berardi and N. F. Calabria and M. G. Catanesi and E. Radicioni and A. Langella and G. De Rosa and G. Collazuol and M. Feltre and F. Iacob and M. Mattiazzi and L. Ludovici and M. Gonin and L. Périssé and G. Pronost and C. Fujisawa and S. Horiuchi and M. Kobayashi and Y. M. Liu and Y. Maekawa and Y. Nishimura and R. Okazaki and R. Akutsu and M. Friend and T. Hasegawa and T. Ishida and T. Kobayashi and M. Jakkapu and T. Matsubara and T. Nakadaira and K. Nakamura and Y. Oyama and A. Portocarrero Yrey and K. Sakashita and T. Sekiguchi and T. Tsukamoto and N. Bhuiyan and G. T. Burton and F. Di Lodovico and J. Gao and A. Goldsack and T. Katori and J. Migenda and R. M. Ramsden and Z. Xie and S. Zsoldos and A. T. Suzuki and Y. Takagi and Y. Takeuchi and H. Zhong and J. Feng and L. Feng and J. R. Hu and Z. Hu and M. Kawaue and T. Kikawa and M. Mori and T. Nakaya and R. A. Wendell and K. Yasutome and S. J. Jenkins and N. McCauley and P. Mehta and A. Tarrant and M. J. Wilking and Y. Fukuda and Y. Itow and H. Menjo and K. Ninomiya and Y. Yoshioka and J. Lagoda and M. Mandal and P. Mijakowski and Y. S. Prabhu and J. Zalipska and M. Jia and J. Jiang and W. Shi and C. Yanagisawa and M. Harada and Y. Hino and H. Ishino and Y. Koshio and F. Nakanishi and S. Sakai and T. Tada and T. Tano and T. Ishizuka and G. Barr and D. Barrow and L. Cook and S. Samani and D. Wark and A. Holin and F. Nova and S. Jung and B. S. Yang and J. Y. Yang and J. Yoo and J. E. P. Fannon and L. Kneale and M. Malek and J. M. McElwee and M. D. Thiesse and L. F. Thompson and S. T. Wilson and H. Okazawa and S. M. Lakshmi and S. B. Kim and E. Kwon and J. W. Seo and I. Yu and A. K. Ichikawa and K. D. Nakamura and S. Tairafune and K. Nishijima and A. Eguchi and K. Nakagiri and Y. Nakajima and S. Shima and N. Taniuchi and E. Watanabe and M. Yokoyama and P. de Perio and S. Fujita and C. Jesús-Valls and K. Martens and K. M. Tsui and M. R. Vagins and J. Xia and S. Izumiyama and M. Kuze and R. Matsumoto and K. Terada and R. Asaka and M. Ishitsuka and H. Ito and Y. Ommura and N. Shigeta and M. Shinoki and K. Yamauchi and T. Yoshida and R. Gaur and V. Gousy-Leblanc and M. Hartz and A. Konaka and X. Li and S. Chen and B. D. Xu and Y. Wu and A. Q. Zhang and B. Zhang and M. Posiadala-Zezula and S. B. Boyd and R. Edwards and D. Hadley and M. Nicholson and M. O’Flaherty and B. Richards and A. Ali and B. Jamieson and S. Amanai and Ll. Marti and A. Minamino and R. Shibayama and R. Shimamura and S. Suzuki and K. Abe and S. Abe and N. Akhlaq and R. Akutsu and H. Alarakia-Charles and A. Ali and Y. I. Alj Hakim and S. Alonso Monsalve and C. Andreopoulos and L. Anthony and M. Antonova and S. Aoki and K. A. Apte and T. Arai and T. Arihara and S. Arimoto and Y. Asada and Y. Ashida and E. T. Atkin and N. Babu and M. Barbi and G. J. Barker and G. Barr and D. Barrow and P. Bates and M. Batkiewicz-Kwasniak and V. Berardi and L. Berns and S. Bhadra and A. Blanchet and A. Blondel and S. Bolognesi and S. Bordoni and S. B. Boyd and A. Bravar and C. Bronner and A. Bubak and M. Buizza Avanzini and J. A. Caballero and N. F. Calabria and S. Cao and D. Carabadjac and A. J. Carter and S. L. Cartwright and M. P. Casado and M. G. Catanesi and A. Cervera and J. Chakrani and A. Chalumeau and D. Cherdack and P. S. Chong and A. Chvirova and M. Cicerchia and J. Coleman and G. Collazuol and L. Cook and F. Cormier and A. Cudd and D. D’ago and C. Dalmazzone and T. Daret and P. Dasgupta and C. Davis and Yu. I. Davydov and A. De Roeck and G. De Rosa and T. Dealtry and C. C. Delogu and C. Densham and A. Dergacheva and R. Dharmapal and F. Di Lodovico and G. Diaz Lopez and S. Dolan and D. Douqa and T. A. Doyle and O. Drapier and K. E. Duffy and J. Dumarchez and P. Dunne and K. Dygnarowicz and A. Eguchi and J. Elias and S. Emery-Schrenk and G. Erofeev and A. Ershova and G. Eurin and D. Fedorova and S. Fedotov and M. Feltre and L. Feng and D. Ferlewicz and A. J. Finch and G. A. Fiorentini Aguirre and G. Fiorillo and M. D. Fitton and J. M. Franco Patiño and M. Friend and Y. Fujii and Y. Fukuda and Y. Furui and L. Giannessi and C. Giganti and V. Glagolev and M. Gonin and J. González Rosa and E. A. G. Goodman and A. Gorin and K. Gorshanov and M. Grassi and M. Guigue and D. R. Hadley and J. T. Haigh and S. Han and D. A. Harris and M. Hartz and T. Hasegawa and S. Hassani and N. C. Hastings and Y. Hayato and I. Heitkamp and D. Henaff and Y. Hino and M. Hogan and J. Holeczek and A. Holin and T. Holvey and N. T. Hong Van and T. Honjo and K. Hosokawa and J. Hu and A. K. Ichikawa and K. Ieki and M. Ikeda and T. Ishida and M. Ishitsuka and A. Izmaylov and M. Jakkapu and B. Jamieson and S. J. Jenkins and C. Jesús-Valls and M. Jia and J. J. Jiang and J. Y. Ji and P. Jonsson and S. Joshi and C. K. Jung and M. Kabirnezhad and A. C. Kaboth and T. Kajita and H. Kakuno and J. Kameda and S. Karpova and S. P. Kasetti and V. S. Kasturi and Y. Kataoka and T. Katori and Y. Kawamura and M. Kawaue and E. Kearns and M. Khabibullin and A. Khotjantsev and T. Kikawa and S. King and V. Kiseeva and J. Kisiel and L. Kneale and H. Kobayashi and T. Kobayashi and L. Koch and S. Kodama and M. Kolupanova and A. Konaka and L. L. Kormos and Y. Koshio and T. Koto and K. Kowalik and Y. Kudenko and Y. Kudo and S. Kuribayashi and R. Kurjata and V. Kurochka and T. Kutter and M. Kuze and M. La Commara and L. Labarga and M. Lachat and K. Lachner and J. Lagoda and S. M. Lakshmi and M. Lamers James and A. Langella and J.-F. Laporte and D. Last and N. Latham and M. Laveder and L. Lavitola and M. Lawe and Y. Lee and D. Leon Silverio and S. Levorato and S. Lewis and C. Lin and R. P. Litchfield and S. L. Liu and W. Li and A. Longhin and K. R. Long and A. Lopez Moreno and L. Ludovici and X. Lu and T. Lux and L. N. Machado and L. Magaletti and K. Mahn and K. K. Mahtani and M. Malek and M. Mandal and S. Manly and A. D. Marino and L. Marti-Magro and D. G. R. Martin and M. Martini and J. F. Martin and T. Maruyama and T. Matsubara and R. Matsumoto and V. Matveev and C. Mauger and K. Mavrokoridis and E. Mazzucato and N. McCauley and K. S. McFarland and C. McGrew and J. McKean and A. Mefodiev and G. D. Megias and P. Mehta and L. Mellet and C. Metelko and M. Mezzetto and S. Miki and E. Miller and A. Minamino and O. Mineev and S. Mine and J. Mirabito and M. Miura and L. Molina Bueno and S. Moriyama and S. Moriyama and P. Morrison and Th. A. Mueller and D. Munford and A. Muñoz and L. Munteanu and K. Nagai and Y. Nagai and T. Nakadaira and K. Nakagiri and M. Nakahata and Y. Nakajima and A. Nakamura and K. Nakamura and K. D. Nakamura and Y. Nakano and S. Nakayama and T. Nakaya and K. Nakayoshi and C. E. R. Naseby and T. V. Ngoc and D. T. Nguyen and V. Q. Nguyen and K. Niewczas and S. Nishimori and Y. Nishimura and Y. Noguchi and T. Nosek and F. Nova and P. Novella and J. C. Nugent and H. M. O’Keeffe and L. O’Sullivan and T. Odagawa and R. Okazaki and W. Okinaga and K. Okumura and T. Okusawa and N. Onda and N. Ospina and L. Osu and Y. Oyama and V. Palladino and V. Paolone and M. Pari and J. Parlone and J. Pasternak and D. Payne and G. C. Penn and D. Pershey and M. Pfaff and L. Pickering and G. Pintaudi and C. Pistillo and B. Popov and A. J. Portocarrero Yrey and K. Porwit and M. Posiadala-Zezula and Y. S. Prabhu and H. Prasad and F. Pupilli and B. Quilain and P. T. Quyen and T. Radermacher and E. Radicioni and B. Radics and M. A. Ramirez and P. N. Ratoff and M. Reh and C. Riccio and E. Rondio and S. Roth and N. Roy and A. Rubbia and L. Russo and A. Rychter and W. Saenz and K. Sakashita and F. Sánchez and Y. Sato and T. Schefke and C. M. Schloesser and K. Scholberg and M. Scott and Y. Seiya and T. Sekiguchi and H. Sekiya and D. Sgalaberna and A. Shaikhiev and M. Shiozawa and Y. Shiraishi and A. Shvartsman and N. Skrobova and K. Skwarczynski and D. Smyczek and M. Smy and J. T. Sobczyk and H. Sobel and F. J. P. Soler and A. J. Speers and R. Spina and Y. Stroke and I. A. Suslov and S. Suvorov and A. Suzuki and S. Y. Suzuki and Y. Suzuki and M. Tada and S. Tairafune and A. Takeda and Y. Takeuchi and K. Takifuji and H. K. Tanaka and H. Tanigawa and A. Teklu and V. V. Tereshchenko and N. Thamm and L. F. Thompson and W. Toki and C. Touramanis and T. Tsukamoto and M. Tzanov and Y. Uchida and M. Vagins and D. Vargas and M. Varghese and G. Vasseur and E. Villa and W. G. S. Vinning and U. Virginet and T. Vladisavljevic and T. Wachala and D. Wakabayashi and H. T. Wallace and J. G. Walsh and Y. Wang and L. Wan and D. Wark and M. O. Wascko and A. Weber and R. Wendell and M. J. Wilking and C. Wilkinson and J. R. Wilson and K. Wood and C. Wret and J. Xia and Y.-h. Xu and K. Yamamoto and T. Yamamoto and C. Yanagisawa and G. Yang and T. Yano and K. Yasutome and N. Yershov and U. Yevarouskaya and M. Yokoyama and Y. Yoshimoto and N. Yoshimura and M. Yu and R. Zaki and A. Zalewska and J. Zalipska and K. Zaremba and G. Zarnecki and J. Zhang and X. Y. Zhao and H. Zhong and T. Zhu and M. Ziembicki and E. D. Zimmerman and M. Zito and S. Zsoldos}, doi = {10.1103/PhysRevLett.134.011801}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011801}, shortjournal = {Phys. Rev. Lett.}, title = {First joint oscillation analysis of super-kamiokande atmospheric and T2K accelerator neutrino data}, volume = {134}, year = {2025}, }
• (2025). Multitwist trajectories and decoupling zeros in conformal field theory. PRL, 134(1), 011602. (www)

  @article{ , abstract = {Conformal Regge theory predicts the existence of analytically continued conformal field theory data for complex spin. How could this work when there are so many more operators with large spin compared to small spin? Using planar SYM as a test ground, we find a simple physical picture. Operators do organize themselves into analytic families but the continuation of the higher families have zeros in their structure operator product expansion constants for lower integer spins. They thus decouple. Newton’s interpolation series technique is perfectly suited to this physical problem and will allow us to explore the complex spin half-plane.}, archive = {J_PRL}, author = {Alexandre Homrich and David Simmons-Duffin and Pedro Vieira}, doi = {10.1103/PhysRevLett.134.011602}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011602}, shortjournal = {Phys. Rev. Lett.}, title = {Multitwist trajectories and decoupling zeros in conformal field theory}, volume = {134}, year = {2025}, }
• (2025). Revising the full one-loop gauge prefactor in electroweak vacuum stability. PRL, 134(1), 011601. (www)

  @article{ , abstract = {We revisit the decay rate of the electroweak vacuum in the standard model with the full one-loop prefactor. We focus on the gauge degrees of freedom and derive the degeneracy factors appearing in the functional determinant using group theoretical arguments. Our treatment shows that the transverse modes were previously overcounted, so we revise the calculation of that part of the prefactor. The new result modifies the gauge fields’ contribution by 6% and slightly decreases the previously predicted lifetime of the electroweak vacuum, which remains much longer than the age of the Universe. Our discussion of the transverse mode degeneracy applies to any calculation of functional determinants involving gauge fields in four dimensions.}, archive = {J_PRL}, author = {Pietro Baratella and Miha Nemevšek and Yutaro Shoji and Katarina Trailović and Lorenzo Ubaldi}, doi = {10.1103/PhysRevLett.134.011601}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011601}, shortjournal = {Phys. Rev. Lett.}, title = {Revising the full one-loop gauge prefactor in electroweak vacuum stability}, volume = {134}, year = {2025}, }
• (2025). Star cluster population of high mass black hole mergers in gravitational wave data. PRL, 134(1), 011401. (www)

  @article{ , abstract = {Stellar evolution theories predict a gap in the black hole birth mass spectrum as the result of pair instability processes in the cores of massive stars. This gap, however, is not seen in the binary black hole masses inferred from gravitational wave data. One explanation is that black holes form dynamically in dense star clusters where smaller black holes merge to form more massive black holes, populating the mass gap. We show that this model predicts a distribution of the effective and precessing spin parameters, and , within the mass gap that is insensitive to assumptions about black hole natal spins and other astrophysical parameters. We analyze the distribution of as a function of primary mass for the black hole binaries in the third gravitational wave transient catalog. We infer the presence of a high mass and isotropically spinning population of black holes that is consistent with hierarchical formation in dense star clusters and a pair-instability mass gap with a lower edge at . We compute a Bayes factor relative to models that do not allow for a high mass population with a distinct distribution. Upcoming data will enable us to tightly constrain the hierarchical formation hypothesis and refine our understanding of binary black hole formation.}, archive = {J_PRL}, author = {Fabio Antonini and Isobel M. Romero-Shaw and Thomas Callister}, doi = {10.1103/PhysRevLett.134.011401}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {011401}, shortjournal = {Phys. Rev. Lett.}, title = {Star cluster population of high mass black hole mergers in gravitational wave data}, volume = {134}, year = {2025}, }
• (2025). Beyond the quantum cram\'er-rao bound. PRL, 134(1), 010804. (www)

  @article{ , abstract = {The quantum Cramér-Rao bound (QCRB) stands as a cornerstone of quantum metrology. Yet, akin to its classical counterpart, it provides only local information and overlooks higher-order details. We leverage the theory of higher-order asymptotics to circumvent these issues, providing corrections to the performance of estimators beyond the QCRB. While the QCRB often yields a whole family of optimal states and several optimal measurements, our approach allows us to identify optimal states and measurements within the family that are otherwise equivalent according to the QCRB alone; these are requisite for optimal metrology before reaching the asymptotic limit. These results are especially pertinent when dealing with unitary processes.}, archive = {J_PRL}, author = {J. R. Hervas and A. Z. Goldberg and A. S. Sanz and Z. Hradil and J. Řeháček and L. L. Sánchez-Soto}, doi = {10.1103/PhysRevLett.134.010804}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010804}, shortjournal = {Phys. Rev. Lett.}, title = {Beyond the quantum cram\'er-rao bound}, volume = {134}, year = {2025}, }
• (2025). Quantum comb tomography via learning isometries on stiefel manifold. PRL, 134(1), 010803. (www)

  @article{ , abstract = {Explicit mathematical reconstructions of quantum combs play a significant role in developing quantum information science. However, tremendous parameter requirements and physical constraint implementations have become computationally nonignorable encumbrances. In this Letter, we propose an efficient method for quantum comb tomography by learning isometries on the Stiefel manifold via solving a series of unconstrained optimization problems with significantly fewer parameters. The stepwise isometry estimation shows the capability for providing information of the truncated quantum comb while processing the tomography. Remarkably, this method enables the dimension-reduced quantum comb tomography by reducing the ancillary dimensions of isometries with bounded error. As a result, our proposed method exhibits high accuracy and efficiency.}, archive = {J_PRL}, author = {Ze-Tong Li and Xin-Lin He and Cong-Cong Zheng and Yu-Qian Dong and Tian Luan and Xu-Tao Yu and Zai-Chen Zhang}, doi = {10.1103/PhysRevLett.134.010803}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010803}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum comb tomography via learning isometries on stiefel manifold}, volume = {134}, year = {2025}, }
• (2025). Reliability function of classical-quantum channels. PRL, 134(1), 010802. (www)

  @article{ , abstract = {We study the reliability function of general classical-quantum channels, which describes the optimal exponent of the decay of decoding error when the communication rate is below the capacity. As the main result, we prove a lower bound, in terms of the quantum Rényi information in Petz’s form, for the reliability function. This resolves Holevo’s conjecture proposed in 2000, a long-standing open problem in quantum information theory. It turns out that the obtained lower bound matches the upper bound derived by Dalai in 2013, when the communication rate is above a critical value. Thus, we have determined the reliability function in this high-rate case. Our approach relies on Renes’ breakthrough made in 2022, which relates classical-quantum channel coding to that of privacy amplification, as well as our new characterization of the channel Rényi information.}, archive = {J_PRL}, author = {Ke Li and Dong Yang}, doi = {10.1103/PhysRevLett.134.010802}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010802}, shortjournal = {Phys. Rev. Lett.}, title = {Reliability function of classical-quantum channels}, volume = {134}, year = {2025}, }
• (2025). Fundamental limits of metrology at thermal equilibrium. PRL, 134(1), 010801. (www)

  @article{ , abstract = {We consider the estimation of an unknown parameter θ through a quantum probe at thermal equilibrium. The probe is assumed to be in a Gibbs state according to its Hamiltonian H θ , which is divided in a parameter-encoding term H θ P and an additional, parameter-independent control H C . Given a fixed encoding, we find the maximal quantum Fisher information attainable via arbitrary H C , which provides a fundamental bound on the measurement precision. We elucidate the role of quantum coherence between encoding and control in different temperature regimes, which include ground state metrology as a limiting case. In the case of locally encoded parameters, the optimal sensitivity presents an N 2 scaling in terms of the number of particles of the probe, which can be reached, at finite temperature, with local measurements and no entanglement. We apply our results to paradigmatic spin chain models, showing that these fundamental limits can be approached using local two-body interactions. Our results set the fundamental limits and optimal control for metrology with thermal and ground state probes, including probes at the verge of criticality.}, archive = {J_PRL}, author = {Paolo Abiuso and Pavel Sekatski and John Calsamiglia and Martí Perarnau-Llobet}, doi = {10.1103/PhysRevLett.134.010801}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010801}, shortjournal = {Phys. Rev. Lett.}, title = {Fundamental limits of metrology at thermal equilibrium}, volume = {134}, year = {2025}, }
• (2025). Compression of quantum shallow-circuit states. PRL, 134(1), 010603. (www)

  @article{ , abstract = {Shallow quantum circuits feature not only computational advantages over their classical counterparts but also cutting-edge applications. Storing quantum information generated by shallow circuits is a fundamental question of both theoretical and practical importance that remained largely unexplored. In this Letter, we show that N copies of an unknown n -qubit state generated by a fixed-depth circuit can be compressed into a hybrid memory of O ( n log 2 N ) (qu)bits, which achieves the optimal scaling of memory cost. Our work shows that the computational complexity of resources can significantly impact the rate of quantum information processing, offering a unique and unified view of quantum Shannon theory and quantum computing.}, archive = {J_PRL}, author = {Yuxiang Yang}, doi = {10.1103/PhysRevLett.134.010603}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010603}, shortjournal = {Phys. Rev. Lett.}, title = {Compression of quantum shallow-circuit states}, volume = {134}, year = {2025}, }
• (2025). Programmable quantum simulations on a trapped-ion quantum computer with a global drive. PRL, 134(1), 010602. (www)

  @article{ , abstract = {Simulation of quantum systems is notoriously challenging for classical computers, while quantum hardware is naturally well-suited for this task. However, the imperfections of contemporary quantum systems pose a considerable challenge in carrying out accurate simulations over long evolution times. Here, we experimentally demonstrate a method for quantum simulations on a small-scale trapped-ion–based quantum simulator. Our method enables quantum simulations of programmable spin-Hamiltonians, using only simple global fields, driving all qubits homogeneously and simultaneously. We measure the evolution of a quantum Ising ring and accurately reconstruct the Hamiltonian parameters, showcasing an accurate and high-fidelity simulation. Our method enables a significant reduction in the required control and depth of quantum simulations, thus generating longer evolution times with higher accuracy.}, archive = {J_PRL}, author = {Yotam Shapira and Jovan Markov and Nitzan Akerman and Ady Stern and Roee Ozeri}, doi = {10.1103/PhysRevLett.134.010602}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010602}, shortjournal = {Phys. Rev. Lett.}, title = {Programmable quantum simulations on a trapped-ion quantum computer with a global drive}, volume = {134}, year = {2025}, }
• (2025). Experimental realization of direct entangling gates between dual-type qubits. PRL, 134(1), 010601. (www)

  @article{ , abstract = {Dual-type qubits have become a promising way to suppress the crosstalk error of auxiliary operations in large-scale ion trap quantum computation. Here we demonstrate a direct entangling gate between dual-type qubits encoded in the and hyperfine manifolds of ions. Our scheme is economic in the hardware, requiring only a single 532 nm laser system to entangle both qubit types by driving their Raman transitions. We achieve a Bell state fidelity of 96.3(4)% for the dual-type Molmer-Sorensen gate between an ion pair, comparable to that for the same-type or gates. This technique can reduce the overhead for back-and-forth conversions between dual-type qubits in the quantum circuit with wide applications in quantum error correction and ion-photon quantum networks.}, archive = {J_PRL}, author = {Chenxi Wang and Chuanxin Huang and Hongxuan Zhang and Hongyuan Hu and Zhichao Mao and Panyu Hou and Yukai Wu and Zichao Zhou and Luming Duan}, doi = {10.1103/PhysRevLett.134.010601}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010601}, shortjournal = {Phys. Rev. Lett.}, title = {Experimental realization of direct entangling gates between dual-type qubits}, volume = {134}, year = {2025}, }
• (2025). Minimal hubbard models of maximal hilbert space fragmentation. PRL, 134(1), 010411. (www)

  @article{ , abstract = {We show that Hubbard models with nearest-neighbor hopping and a nearest-neighbor hardcore constraint exhibit “maximal” Hilbert space fragmentation in many lattices of arbitrary dimension . Focusing on the rhombus chain and the Lieb lattice, we demonstrate that the fragmentation is strong for all fillings in the thermodynamic limit, and explicitly construct all emergent integrals of motion, which include an extensive set of higher-form symmetries. Blockades consisting of frozen particles partition the system in real space, leading to anomalous dynamics. Our results are potentially relevant to optical lattices of dipolar and Rydberg-dressed atoms.}, archive = {J_PRL}, author = {Yves H. Kwan and Patrick H. Wilhelm and Sounak Biswas and S. A. Parameswaran}, doi = {10.1103/PhysRevLett.134.010411}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010411}, shortjournal = {Phys. Rev. Lett.}, title = {Minimal hubbard models of maximal hilbert space fragmentation}, volume = {134}, year = {2025}, }
• (2025). Measurement-induced spectral transition. PRL, 134(1), 010410. (www)

  @article{ , abstract = {We show that noisy quantum dynamics exposed to generalized measurements exhibit a spectral transition between gapless and gapped phases. To this end, we employ the Lyapunov spectrum obtained through singular values of a nonunitary matrix describing the dynamics. We discover that the gapless and gapped phases, respectively, correspond to the volume-law and area-law phases of the entanglement entropy for the dominant Lyapunov vector. This correspondence between the spectral gap and the scaling of entanglement offers an intriguing common structure with ground-state phase transitions. We also discuss some crucial differences from ground-state transitions, such as the extensive entanglement and the exponentially small gaps. Furthermore, we show that the spectral transition leads to the transition of the timescale for the memory loss and purification of initial states.}, archive = {J_PRL}, author = {Ken Mochizuki and Ryusuke Hamazaki}, doi = {10.1103/PhysRevLett.134.010410}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010410}, shortjournal = {Phys. Rev. Lett.}, title = {Measurement-induced spectral transition}, volume = {134}, year = {2025}, }
• (2025). Defect production across higher-order phase transitions beyond kibble-zurek scaling. PRL, 134(1), 010409. (www)

  @article{ , abstract = {The Kibble-Zurek mechanism predicts a universal scaling behavior of the defect production when a system is slowly quenched across a critical phase transition point. Here, we discover that the universal scaling behavior across a higher-order topological phase transition does not conform to the traditional Kibble-Zurek mechanism. To explain the anomalous scaling exponent, we develop a solvable Landau-Zener model that takes into account the role of topological edge band that dominates the phase transition. For a two-dimensional boundary-obstructed higher-order topological system, the Kibble-Zurek scaling must be modified to adopt the effective dimension of topological edge band instead of the real physical dimension. We also find that across the boundary-obstructed higher-order topological phase transition, boundary conditions can drastically modify the scaling behaviors. For comparison, we investigate the slow quench dynamics across the bulk-obstructed phase transitions and a single multicritical point, which obeys the Kibble-Zurek mechanism with physical dimension.}, archive = {J_PRL}, author = {Menghua Deng and Zhoujian Sun and Fuxiang Li}, doi = {10.1103/PhysRevLett.134.010409}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010409}, shortjournal = {Phys. Rev. Lett.}, title = {Defect production across higher-order phase transitions beyond kibble-zurek scaling}, volume = {134}, year = {2025}, }
• (2025). Correlations enable lossless ergotropy transport. PRL, 134(1), 010408. (www)

  @article{ , abstract = {“A battery powers a device” can be read as “work stored in the battery is being transported to the device.” In quantum batteries, the total amount of stored work can be measured by ergotropy, which is the maximal work extractable by unitary operations. Transporting ergotropy is fundamentally different from transporting energy, and here we find that ergotropy can be gained even when the transmission channel is strictly energy conserving. We show that, generically, ergotropy transport is lossy whenever the two systems start uncorrelated. In contrast, for a large class of correlated initial states, transport can be gainful. Furthermore, a single correlated state can be used multiple times, allowing to transport without losses an order of magnitude more work than the battery capacity. Correlations are thus a useful resource for ergotropy transport, and we quantify how this resource is consumed during gainful transport.}, archive = {J_PRL}, author = {Rick P. A. Simon and Janet Anders and Karen V. Hovhannisyan}, doi = {10.1103/PhysRevLett.134.010408}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010408}, shortjournal = {Phys. Rev. Lett.}, title = {Correlations enable lossless ergotropy transport}, volume = {134}, year = {2025}, }
• (2025). Quantum zeno engines and heat pumps. PRL, 134(1), 010407. (www)

  @article{ , abstract = {We study the implementation of quantum engines and quantum heat pumps where the quantum adiabatic transformations are replaced by quantum Zeno strokes. During these strokes, frequent measurements are selectively performed on the external state of the system avoiding transition between different levels. This effectively delivers almost ideal isentropic transformations. We concentrate on the characterization of the performance of a quantum Zeno heat pump implemented with a quantum harmonic oscillator, showing that optimal performance can be achieved faster than with shortcut-to-adiabaticity techniques.}, archive = {J_PRL}, author = {Giovanni Barontini}, doi = {10.1103/PhysRevLett.134.010407}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010407}, shortjournal = {Phys. Rev. Lett.}, title = {Quantum zeno engines and heat pumps}, volume = {134}, year = {2025}, }
• (2025). Universal upper bound on ergotropy and no-go theorem by the eigenstate thermalization hypothesis. PRL, 134(1), 010406. (www)

  @article{ , abstract = {We show that the maximum extractable work (ergotropy) from a quantum many-body system is constrained by “local athermality” of an initial state and “local entropy decrease” brought about by quantum operations. The obtained universal upper bound on ergotropy implies that the eigenstate thermalization hypothesis prohibits work extraction from energy eigenstates by means of finite-time unitary operations. This no-go property implies that Planck’s principle, a form of the second law of thermodynamics, holds even for pure quantum states. Our result bridges two independently studied concepts of quantum thermodynamics, the second law and thermalization, via “intrasystem” correlations in many-body systems as a resource for work extraction.}, archive = {J_PRL}, author = {Akihiro Hokkyo and Masahito Ueda}, doi = {10.1103/PhysRevLett.134.010406}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010406}, shortjournal = {Phys. Rev. Lett.}, title = {Universal upper bound on ergotropy and no-go theorem by the eigenstate thermalization hypothesis}, volume = {134}, year = {2025}, }
• (2025). Navier-stokes equations for nearly integrable quantum gases. PRL, 134(1), 010405. (www)

  @article{ , abstract = {The Navier-Stokes equations are paradigmatic equations describing hydrodynamics of an interacting system with microscopic interactions encoded in transport coefficients. In this work we show how the Navier-Stokes equations arise from the microscopic dynamics of nearly integrable 1D quantum many-body systems. We build upon the recently developed hydrodynamics of integrable models to study the effective Boltzmann equation with collision integral taking into account the non-integrable interactions. We compute the transport coefficients and find that the resulting Navier-Stokes equations have two regimes, which differ in the viscous properties of the fluid. We illustrate the method by computing the transport coefficients for an experimentally relevant case of coupled 1D cold-atomic gases.}, archive = {J_PRL}, author = {Maciej Łebek and Miłosz Panfil}, doi = {10.1103/PhysRevLett.134.010405}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010405}, shortjournal = {Phys. Rev. Lett.}, title = {Navier-stokes equations for nearly integrable quantum gases}, volume = {134}, year = {2025}, }
• (2025). Universal correlations in chaotic many-body quantum states: Fock-space formulation of berry's random wave model. PRL, 134(1), 010404. (www)

  @article{ , abstract = {The apparent randomness of chaotic eigenstates in interacting quantum systems hides subtle correlations dynamically imposed by their finite energy per particle. These correlations are revealed when Berry’s approach for chaotic eigenfunctions in single-particle systems is lifted into many-body space. We achieve this by a many-body semiclassical analysis, appropriate for the mesoscopic regime of a large but finite number of particles. We thereby identify as signatures of chaotic many-body eigenstates the universality of both their cross-correlations and the Gaussian distribution of expansion coefficients. Combined, these two features imprint characteristic features to the morphology of eigenstates that we check against extensive quantum simulations. The universality of eigenstate correlations for fixed energy density is hence a further signature of many-body quantum chaos that, while consistent with the eigenstate thermalization hypothesis, lies beyond random matrix theory.}, archive = {J_PRL}, author = {Florian Schoeppl and Rémy Dubertrand and Juan-Diego Urbina and Klaus Richter}, doi = {10.1103/PhysRevLett.134.010404}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010404}, shortjournal = {Phys. Rev. Lett.}, title = {Universal correlations in chaotic many-body quantum states: Fock-space formulation of berry's random wave model}, volume = {134}, year = {2025}, }
• (2025). Stable symmetry-protected topological phases in systems with heralded noise. PRL, 134(1), 010403. (www)

  @article{ , abstract = {We present a family of local quantum channels whose steady states exhibit stable mixed-state symmetry-protected topological (SPT) order. Motivated by recent experimental progress on “erasure conversion” techniques that allow one to identify ( herald ) decoherence processes, we consider open systems with biased erasure noise, which leads to strongly symmetric heralded errors. We utilize this heralding to construct a local correction protocol that effectively confines errors into short-ranged pairs in the steady state. Using a combination of numerical simulations and mean-field analysis, we show that our protocol stabilizes SPT order against a sufficiently low rate of decoherence. As the rate of heralded noise increases, SPT order is eventually lost through a directed percolation transition. We further find that while introducing unheralded errors destroys SPT order in the limit of long length scales and timescales, the correction protocol is sufficient for ensuring that local SPT order persists, with a correlation length that diverges as , where is the fraction of errors that are heralded.}, archive = {J_PRL}, author = {Sanket Chirame and Fiona J. Burnell and Sarang Gopalakrishnan and Abhinav Prem}, doi = {10.1103/PhysRevLett.134.010403}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010403}, shortjournal = {Phys. Rev. Lett.}, title = {Stable symmetry-protected topological phases in systems with heralded noise}, volume = {134}, year = {2025}, }
• (2025). Measuring the spectral form factor in many-body chaotic and localized phases of quantum processors. PRL, 134(1), 010402. (www)

  @article{ , abstract = {The spectral form factor (SFF) captures universal spectral fluctuations as signatures of quantum chaos, and has been instrumental in advancing multiple frontiers of physics including the studies of black holes and quantum many-body systems. The measurement of the SFF in many-body systems is however challenging due to the difficulty in resolving level spacings that become exponentially small with increasing system size. Here, we utilize the random measurement toolbox to perform a direct experimental measurement of the SFF, and hence probe the presence or absence of chaos in quantum many-body systems on superconducting quantum processors. For a Floquet chaotic system, we observe signatures of both short- and long-range spectral correlations in the SFF given by the ramp-plateau behavior. Furthermore, for a Hamiltonian system we utilize the SFF to distinguish a quantum many-body chaotic phase and the prethermal many-body localization. We observe the dip-ramp-plateau behavior of random matrix theory in the chaotic phase and contrast the scaling of the plateau time in system size between the many-body chaotic and localized phases. Finally, we probe the eigenstate statistics by measuring a generalization of the SFF, known as the partial SFF, and observe distinct behaviors in the purity of the reduced density matrices in these two phases. This work unveils a new experimental way of extracting the universal signatures of many-body quantum chaos in quantum devices by probing short- and long-range correlations in the energy spectrum and eigenstates.}, archive = {J_PRL}, author = {Hang Dong and Pengfei Zhang and Ceren B. Dağ and Yu Gao and Ning Wang and Jinfeng Deng and Xu Zhang and Jiachen Chen and Shibo Xu and Ke Wang and Yaozu Wu and Chuanyu Zhang and Feitong Jin and Xuhao Zhu and Aosai Zhang and Yiren Zou and Ziqi Tan and Zhengyi Cui and Zitian Zhu and Fanhao Shen and Tingting Li and Jiarun Zhong and Zehang Bao and Hekang Li and Zhen Wang and Qiujiang Guo and Chao Song and Fangli Liu and Amos Chan and Lei Ying and H. Wang}, doi = {10.1103/PhysRevLett.134.010402}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010402}, shortjournal = {Phys. Rev. Lett.}, title = {Measuring the spectral form factor in many-body chaotic and localized phases of quantum processors}, volume = {134}, year = {2025}, }
• (2025). Anticoncentration and state design of random tensor networks. PRL, 134(1), 010401. (www)

  @article{ , abstract = {We investigate quantum random tensor network states in which the dimension of the bond scales polynomially with the size of the system N . Specifically, we examine the delocalization properties of random matrix product states (RMPS) in the computational basis by deriving an exact analytical expression for the inverse participation ratio (IPR) of any degree, applicable to both open and closed boundary conditions. For bond dimensions χ ∼ γ N , we determine the leading order of the associated overlaps probability distribution and demonstrate its convergence to the Porter-Thomas distribution, characteristic of Haar-random states, as γ increases. Additionally, we provide numerical evidence for the frame potential, measuring the 2-distance from the Haar ensemble, which confirms the convergence of random MPS to Haar-like behavior for χ ≫ N . We extend this analysis to two-dimensional systems using random projected entangled pair states, where we similarly observe the convergence of IPRs to their Haar values for χ ≫ N . These findings demonstrate that random tensor networks with bond dimensions scaling polynomially in the system size are fully Haar anticoncentrated and approximate unitary designs, regardless of the spatial dimension.}, archive = {J_PRL}, author = {Guglielmo Lami and Jacopo De Nardis and Xhek Turkeshi}, doi = {10.1103/PhysRevLett.134.010401}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010401}, shortjournal = {Phys. Rev. Lett.}, title = {Anticoncentration and state design of random tensor networks}, volume = {134}, year = {2025}, }
• (2025). Orbital angular momentum experiment converting contextuality into nonlocality. PRL, 134(1), 010203. (www)

  @article{ , abstract = {It was recently revealed by Cabello in a theoretical Letter [ Phys. Rev. Lett. 127 , 070401 (2021) ] that nonlocality and contextuality, as two intuitively distinctive yet both critical quantum resources, can be surprisingly connected through Bell inequalities associated with state-independent contextuality sets. It provides a general unified method capable of converting contextuality into bipartite nonlocality. However, experimental tests of the inequalities are challenging and noise sensitive, and the requirements for the quantum states purity, dimensionality, and degree of entanglement have blocked the experimental implementation. We report a first experimental test of Cabello’s inequalities from state-independent contextuality sets, by leveraging two-photon high-dimensional orbital angular momentum entangled states. Distinguishing from the standard single-particle ways, our experiment spotlights that the state-independent contextuality sets can be tested in a bipartite scenario, by which the “compatibility” or “sharpness” loopholes can be effectively avoided. Our results provide a new perspective and demonstrate the principle that contextuality, a widely used quantum resource, can be used in different physical scenarios.}, archive = {J_PRL}, author = {Jianqi Sheng and Dongkai Zhang and Lixiang Chen}, doi = {10.1103/PhysRevLett.134.010203}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010203}, shortjournal = {Phys. Rev. Lett.}, title = {Orbital angular momentum experiment converting contextuality into nonlocality}, volume = {134}, year = {2025}, }
• (2025). Topologically robust quantum network nonlocality. PRL, 134(1), 010202. (www)

  @article{ , abstract = {We discuss quantum network Bell nonlocality in a setting where the network structure is not fully known. More concretely, an honest user may trust their local network topology, but not the structure of the rest of the network, involving distant (and potentially dishonest) parties. We demonstrate that quantum network nonlocality can still be demonstrated in such a setting, hence exhibiting topological robustness. Specifically, we present quantum distributions obtained from a simple network that cannot be reproduced by classical models, even when the latter are based on more powerful networks. In particular, we show that in a large ring network, the knowledge of only a small part of the network structure (involving only two or three neighboring parties) is enough to guarantee nonlocality over the entire network. This shows that quantum network nonlocality can be extremely robust to changes in the network topology. Moreover, we demonstrate that applications of quantum nonlocality, such as the black-box certification of randomness and entanglement, are also possible in such a setting.}, archive = {J_PRL}, author = {Sadra Boreiri and Tamás Kriváchy and Pavel Sekatski and Antoine Girardin and Nicolas Brunner}, doi = {10.1103/PhysRevLett.134.010202}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010202}, shortjournal = {Phys. Rev. Lett.}, title = {Topologically robust quantum network nonlocality}, volume = {134}, year = {2025}, }
• (2025). Simplest bipartite perfect quantum strategies. PRL, 134(1), 010201. (www)

  @article{ , abstract = {A bipartite perfect quantum strategy (BPQS) allows two players who cannot communicate with each other to always win a nonlocal game. BPQSs are rare but fundamental in light of some recent results in quantum information, computation, and foundations. A more than 40-year-old open problem is how many inputs (measurement settings) a BPQS requires. A related problem is how many inputs are needed if, in addition, the quantum system has minimum dimension. A third, apparently unrelated, problem is what is the connection between BPQSs and state-independent contextuality, which inspired the first BPQSs. Here, we solve the third problem: we prove that every BPQS defines a Kochen-Specker set. We use this result to identify the BPQS with the smallest number of inputs, both in the general case and in the case of minimum dimension, and solve some related problems. We conjecture that the BPQSs presented here are the solutions to the first two problems.}, archive = {J_PRL}, author = {Adán Cabello}, doi = {10.1103/PhysRevLett.134.010201}, journal = {Physical Review Letters}, month = {1}, number = {1}, pages = {010201}, shortjournal = {Phys. Rev. Lett.}, title = {Simplest bipartite perfect quantum strategies}, volume = {134}, year = {2025}, }